
GENERAL INFORMATION ....................1-VIII
About this Manual ............................1-VIII
Warranty ..........................................1-VIII
Declaration of Conformity...................1-VIII
Preface.............................................. 1-2
Introduction ...............................................1-2
Powerful and Versatile Functions ........ 1-2
No Mistakes........................................1-3
Design Innovations.................................... 1-3
State of the Art Technology Gives
Durable Use........................................ 1-3
High Resolution................................... 1-3
Remote Control ......................................... 1-4
Fast GPIB Bus....................................1-4
Safety................................................ 1-5
Introduction ...............................................1-5
Safety Precautions .................................... 1-5
Caution and Warning Statements........1-6
Symbols..............................................1-6
If in Doubt about Safety....................... 1-6
Disposal of Hazardous Materials......... 1-6
Unpacking ........................................ 1-7
Check List ................................................. 1-7
Identification.............................................. 1-7
Installation................................................. 1-8
Supply Voltage.................................... 1-8
Battery Supply..................................... 1-8
Grounding ............................................1-8
Orientation and Cooling ...................... 1-8
Fold-Down Support .............................1-9
Rackmount Adapter ............................ 1-9
2 Using the Controls
Basic Controls ........................................... 2-2
Secondary Controls................................... 2-4
Connectors & Indicators...................... 2-4
Rear Panel.......................................... 2-5
Rear Panel (CNT-91R/71B).................2-6
Description of Keys ...................................2-7
Power ................................................. 2-7
Select Function...................................2-7
Autoset/Preset .................................... 2-8
Move Cursor ....................................... 2-8
Display Contrast.................................. 2-8
Enter................................................... 2-8
Save & Exit ......................................... 2-8
Don't Save & Exit................................ 2-8
Presentation Modes............................ 2-9
Entering Numeric Values.................. 2-10
Hard Menu Keys............................... 2-10
Default Settings ....................................... 2-19
3 Input Signal Conditioning
Input Amplifier............................................ 3-2
Impedance ......................................... 3-2
Attenuation......................................... 3-2
Coupling............................................. 3-3
Filter ................................................... 3-3
Man/Auto............................................ 3-4
Trig..................................................... 3-5
How to Reduce or Ignore Noise and
Interference ........................................... 3-6
Trigger Hysteresis .............................. 3-6
How to use Trigger Level Setting........ 3-7
4 Measuring Functions
Introduction to This Chapter........... 4-2
Selecting Function .................................... 4-2
Frequency Measurements .............. 4-3
FREQ A, B................................................ 4-3
FREQ C.................................................... 4-4
CNT-90/91(R)..................................... 4-4
CNT-90XL .......................................... 4-4
RATIO A/B, B/A, C/A, C/B ........................ 4-4
BURST A, B, C......................................... 4-4
1-8
Triggering........................................... 4-4
Burst Measurements using Manual
Presetting........................................... 4-5
Frequency Modulated Signals................... 4-6
Carrier Wave Frequency f0................. 4-6
f
max
.................................................... 4-7
f
min
..................................................... 4-7
Δf
p-p
.................................................... 4-8
Errors in f
max
, f
min
, and Δf
p-p
.................. 4-8
AM Signals ............................................... 4-8
Carrier Wave Frequency..................... 4-8
Modulating Frequency ........................ 4-9
Theory of Measurement............................ 4-9
Reciprocal Counting ........................... 4-9
Sample-Hold..................................... 4-10
Time-Out .......................................... 4-10
Measuring Speed ............................. 4-10
PERIOD.................................................. 4-13
Single A, B & Avg. A, B, C ................ 4-13
III
Environmental Considerations.............1-6

Single A, B Back-to-Back .................. 4-14
Frequency A, B Back-to-Back ........... 4-14
Time Measurements ...................... 4-15
Introduction ............................................. 4-15
Triggering.......................................... 4-15
Time Interval ........................................... 4-16
Time Interval A to B........................... 4-16
Time Interval B to A........................... 4-16
Time Interval A to A, B to B............... 4-16
CNT-91(R): Time Interval Error (TIE)....... 4-16
Rise/Fall Time A/B .................................. 4-16
Pulse Width A/B ...................................... 4-17
Duty Factor A/B....................................... 4-17
Measurement Errors................................ 4-18
Hysteresis.........................................4-18
Overdrive and Pulse Rounding.......... 4-18
Auto Trigger......................................4-19
Phase .............................................. 4-20
What is Phase?....................................... 4-20
Resolution............................................... 4-20
Possible Errors........................................ 4-20
Inaccuracies...................................... 4-21
Totalize [CNT-91(R) only] .............. 4-24
Totalize in General .................................. 4-24
TOT A MAN ............................................ 4-24
TOT B MAN ............................................ 4-24
TOT A+B MAN........................................ 4-24
TOT A–B MAN........................................ 4-25
Applications ...................................... 4-25
TOT A/B MAN......................................... 4-25
Totalize & Arming.................................... 4-25
Examples.......................................... 4-25
Voltage............................................ 4-27
V
MAX
, V
MIN
, VPP......................................... 4-27
V
RMS
........................................................ 4-28
5 Measurement Control
About This Chapter ...................................5-2
Measurement Time .............................5-2
Gate Indicator ..................................... 5-2
Single Measurements ......................... 5-2
Hold/Run & Restart .............................5-2
Arming ................................................ 5-2
Start Arming........................................ 5-3
Stop Arming........................................ 5-3
Controlling Measurement Timing... 5-4
The Measurement Process .......................5-4
Resolution as Function of Measurement
Time.................................................... 5-4
Measurement Time and Rates ............5-5
What is Arming?.................................. 5-5
Arming Setup Time ................................... 5-9
Arming Examples...................................... 5-9
Introduction to Arming Examples ........ 5-9
#1 Measuring the First Burst Pulse..... 5-9
#2 Measuring the Second Burst
Pulse #1 and #4 ................................ 5-12
#4 Profiling ........................................ 5-13
6 Process
Introduction............................................... 6-2
Averaging........................................... 6-2
Mathematics ............................................. 6-2
Example: ........................................... 6-2
Statistics................................................... 6-3
Allan Deviation vs. Standard Deviation6-3
Selecting Sampling Parameters.......... 6-3
Measuring Speed ............................... 6-4
Determining Long or Short Time
Instability ............................................ 6-4
Statistics and Mathematics ............... 6-5
Confidence Limits............................... 6-5
Jitter Measurements ........................... 6-5
Limits........................................................ 6-6
Limit Behavior..................................... 6-6
Limit Mode.......................................... 6-6
Limits and Graphics.................................. 6-7
7 Performance Check
General Information.................................. 7-2
Preparations ............................................. 7-2
Test Equipment ........................................ 7-2
Front Panel Controls................................. 7-3
Internal Self-Tests .............................. 7-3
Keyboard Test.................................... 7-3
Short Form Specification Test ................... 7-5
Sensitivity and Frequency Range ....... 7-5
Voltage............................................... 7-6
Trigger Indicators vs. Trigger Levels... 7-7
Input Controls ..................................... 7-8
Reference Oscillators (not CNT-91R) . 7-8
Rubidium Oscillator (CNT-91R and
CNT-91R/71B) ................................... 7-8
Resolution Test .................................. 7-9
Rear Inputs/Outputs.................................. 7-9
10 MHz OUT (all models) 0.1, 1, 5 & 10
MHz OUT(CNT-91R/71B
EXT REF FREQ INPUT...................... 7-9
EXT ARM INPUT.............................. 7-10
Measuring Functions ............................... 7-10
Check of HOLD OFF Function ................. 7-10
RF Inputs................................................. 7-12
Checking Input C............................... 7-12
Power Measurement
(CNT-90XL only)................................ 7-13
Battery Supply ......................................... 7-13
IV
#3 Measuring the Time Between Burst
Pulse.................................................. 5-11
[CNT-90XL option 28 only].......................4-29
Pulsed Signals

Option 23/90 for CNT-90 & CNT-90XL
only................................................... 7-13
8 Specifications
CNT-90 .............................................. 8-2
Introduction ...............................................8-3
Measurement Functions............................ 8-3
Frequency A, B, C............................... 8-3
Frequency Burst A, B, C...................... 8-3
Period A, B, C Average....................... 8-3
Period A, B Single ............................... 8-4
Ratio A/B, B/A, C/A, C/B ..................... 8-4
Time Interval A to B, B to A, A to A, B to B
........................................................... 8-4
Pulse Width A, B ................................. 8-4
Rise and Fall Time A, B....................... 8-4
Phase A Rel. B, B Rel. A..................... 8-5
Duty Factor A, B.................................. 8-5
V
max
, V
min
, V
p-p
A, B.............................. 8-5
Timestamping A, B, C ......................... 8-6
Auto Set / Manual Set ......................... 8-6
Input and Output Specifications................. 8-6
Inputs A and B .................................... 8-6
Input C (Option 10).............................. 8-7
Input C (Option 13).............................. 8-7
Input C (Options 14 & 14B) ................. 8-8
Rear Panel Inputs & Outputs............... 8-8
Auxiliary Functions .................................... 8-8
Trigger Hold-Off .................................. 8-8
External Start/Stop Arming.................. 8-8
Statistics ............................................. 8-8
Mathematics ....................................... 8-9
Other Functions .................................. 8-9
Display................................................8-9
GPIB Interface .................................... 8-9
USB Interface.................................... 8-10
TimeView™ ...................................... 8-10
Battery Unit ............................................. 8-10
Option 23/90 ..................................... 8-10
Measurement Uncertainties..................... 8-11
Random Uncertainties (1) ............... 8-11
Systematic Uncertainties................... 8-11
Total Uncertainty (2) .......................8-11
Time Interval, Pulse Width, Rise/Fall Time
......................................................... 8-11
Frequency & Period .......................... 8-11
Frequency Ratio f1/f2......................... 8-12
Phase ............................................... 8-12
Duty Factor ....................................... 8-12
Calibration............................................... 8-13
Definition of Terms ............................ 8-13
General Specifications ............................ 8-13
Environmental Data........................... 8-13
Power Requirements......................... 8-13
Dimensions & Weight........................ 8-14
Ordering Information ............................... 8-14
Timebase Options................................... 8-15
Explanations..................................... 8-15
CNT-90XL ....................................... 8-16
Introduction............................................. 8-17
Measurement Functions ......................... 8-17
Frequency A, B, C ............................ 8-17
Frequency Burst A, B ....................... 8-17
Period A, B, C Average..................... 8-17
Period A, B Single ............................ 8-17
Ratio A/B, B/A, C/A, C/B................... 8-17
Time Interval A to B, B to A, A to A, B to B
.......................................................... 8-17
Pulse Width A, B............................... 8-18
Rise and Fall Time A, B.................... 8-18
Phase A Rel. B, B Rel. A .................. 8-18
Duty Factor A, B ............................... 8-18
V
max
, V
min
, V
p-p
A, B ........................... 8-18
Power C ........................................... 8-18
Timestamping A, B ........................... 8-19
(option 28 only).................................. 8-19
Auto Set / Manual Set....................... 8-19
Input and Output Specifications .............. 8-19
Inputs A and B.................................. 8-19
Input C.............................................. 8-20
Rear Panel Inputs & Outputs ............ 8-20
Auxiliary Functions.................................. 8-20
Trigger Hold-Off................................ 8-20
External Start/Stop Arming ............... 8-20
Statistics........................................... 8-20
Mathematics ..................................... 8-20
Other Functions................................ 8-20
Display ............................................. 8-21
GPIB Interface.................................. 8-21
USB Interface ................................... 8-21
TimeView™...................................... 8-21
Battery Unit............................................. 8-21
Option 23/90..................................... 8-21
Measurement Uncertainties .................... 8-22
Random Uncertainties (1σ)............... 8-22
Systematic Uncertainties .................. 8-22
Total Uncertainty (2σ)....................... 8-22
Time Interval, Pulse Width, Rise/Fall Time
.......................................................... 8-22
Frequency & Period A, B .................. 8-22
Frequency & Period C ...................... 8-22
Frequency Ratio fA/fB or fB/fA ............. 8-23
Frequency Ratio fC/fA or fC/fB ............. 8-23
Phase............................................... 8-23
Duty Factor....................................... 8-23
Calibration .............................................. 8-23
Definition of Terms ........................... 8-23
General Specifications............................ 8-24
Environmental Data .......................... 8-24
Power Requirements ........................ 8-24
Dimensions & Weight ....................... 8-24
Ordering Information............................... 8-24
Timebase Options................................... 8-25
Pulsed RF parameters input C

Explanations ..................................... 8-25
CNT-91(R) ....................................... 8-30
Introduction ............................................. 8-31
Measurement Functions.......................... 8-31
Frequency A, B, C............................. 8-31
Frequency Burst A, B, C.................... 8-31
Period A, B, C Average..................... 8-31
Period A, B Single ............................. 8-32
Period A, B Back-to-Back.................. 8-32
Ratio A/B, B/A, C/A, C/B ................... 8-32
Time Interval A to B, B to A, A to A, B to B
......................................................... 8-32
Pulse Width A, B ............................... 8-32
Rise and Fall Time A, B..................... 8-32
Time Interval Error (TIE) A, B............ 8-33
Phase A Rel. B, B Rel. A................... 8-33
Duty Factor A, B................................ 8-33
V
max
, V
min
, V
p-p
A, B............................ 8-33
Totalize A, B, A+B, A-B, A/B ............. 8-34
Timestamping A, B............................ 8-34
Auto Set / Manual Set ....................... 8-34
Input and Output Specifications............... 8-35
Inputs A and B .................................. 8-35
Input C (Option 10)............................ 8-35
Input C (Option 13)............................ 8-36
Input C (Options 14 & 14B) ............... 8-36
Rear Panel Inputs & Outputs............. 8-36
Auxiliary Functions .................................. 8-37
Trigger Hold-Off ................................ 8-37
External Start/Stop Arming................ 8-37
Statistics ........................................... 8-37
Mathematics ..................................... 8-38
Other Functions ................................ 8-38
Display..............................................8-38
GPIB Interface .................................. 8-38
USB Interface.................................... 8-39
TimeView™ ...................................... 8-39
Measurement Uncertainties..................... 8-40
Random Uncertainties (1) ............... 8-40
Systematic Uncertainties................... 8-40
Total Uncertainty (2) .......................8-40
Time Interval, Pulse Width, Rise/Fall Time
......................................................... 8-40
Frequency & Period .......................... 8-41
Frequency Ratio f1/f2......................... 8-41
Phase ............................................... 8-41
Duty Factor ....................................... 8-41
Calibration............................................... 8-42
Definition of Terms ............................ 8-42
General Specifications ............................ 8-42
Environmental Data........................... 8-42
Power Requirements......................... 8-43
Dimensions & Weight........................ 8-43
Ordering Information ............................... 8-43
Timebase Options CNT-91...................... 8-44
Explanations ..................................... 8-44
Timebase Specifications CNT-91R ......... 8-45
Explanations..................................... 8-45
CNT-91R/71B.................................... 8-46
Introduction............................................. 8-47
Measurement Functions ......................... 8-47
Frequency A, B, C ............................ 8-47
Frequency Burst A, B, C................... 8-47
Period A, B, C Average..................... 8-47
Period A, B Single ............................ 8-48
Period A, B Back-to-Back ................. 8-48
Ratio A/B, B/A, C/A, C/B................... 8-48
Time Interval A to B, B to A, A to A, B to B
......................................................... 8-48
Pulse Width A, B............................... 8-48
Rise and Fall Time A, B .................... 8-48
Time Interval Error (TIE) A, B ........... 8-49
Phase A Rel. B, B Rel. A .................. 8-49
Duty Factor A, B ............................... 8-49
V
max
, V
min
, V
p-p
A, B ........................... 8-49
Totalize A, B, A+B, A-B, A/B............. 8-50
Timestamping A, B ........................... 8-50
Auto Set / Manual Set....................... 8-50
Input and Output Specifications .............. 8-51
Inputs A and B.................................. 8-51
Input C.............................................. 8-51
Rear Panel Inputs & Outputs ............ 8-52
Auxiliary Functions.................................. 8-52
Trigger Hold-Off................................ 8-52
External Start/Stop Arming ............... 8-52
Statistics........................................... 8-52
Mathematics ..................................... 8-53
Other Functions................................ 8-53
Display ............................................. 8-53
GPIB Interface.................................. 8-53
USB Interface ................................... 8-54
TimeView™...................................... 8-54
Measurement Uncertainties .................... 8-55
Random Uncertainties (1)............... 8-55
Systematic Uncertainties .................. 8-55
Total Uncertainty (2)....................... 8-55
Time Interval, Pulse Width, Rise/Fall Time
......................................................... 8-55
Frequency & Period.......................... 8-56
Frequency Ratio f1/f2......................... 8-56
Phase............................................... 8-56
Duty Factor....................................... 8-56
Calibration .............................................. 8-57
Definition of Terms ........................... 8-57
General Specifications............................ 8-57
Environmental Data .......................... 8-57
Power Requirements ........................ 8-58
Dimensions & Weight ....................... 8-58
Timebase Specifications CNT-91R/71B..8-59
Explanations..................................... 8-59

GENERAL INFORMATION
About this Manual
This manual contains directions for use that apply to the Timer/Counter/Analyzers CNT-90 and
CNT-91 as well as the Frequency Calibrator/Analyzer CNT-91R and CNT-91R/71B and the Microwave Counter/Analyzer CNT-90XL.
In order to simplify the references, these instruments are further referred to throughout this
manual as the '9X', whenever the information applies to all types. Differences are clearly
marked.
Examples:
CNT-90 means CNT-90 and CNT-90/XL
CNT-90/91 means CNT-90 and CNT-91
CNT-91(R) means CNT-91, CNT-91R and CNT-91R/71B
Chapter 8; Specifications is divided into four separate sections to increase legibility. Much of
the contents is common, so redundant data is the price in this case.
The Warranty Statement is part of the folder Important Information that is included with the
shipment.
Declaration of Conformity
The complete text with formal statements concerning product identification, manufacturer and
standards used for type testing is available on request.

Preface
Introduction
Congratulations on your choice of instrument.
It will serve you well and stay ahead of most
competition for many years to come.
Your instrument is designed to bring you a
new dimension to bench-top and system
counting. It gives significantly increased
performance compared to traditional
Timer/Counters. The '9X' offers the following
advantages:
—12 digits of frequency resolution per sec-
ond and 50 or 100 ps resolution, as a result
of high-resolution interpolating reciprocal
counting.
—Optional oven-controlled timebase oscilla-
tors, except th
e CNT-91R &
CNT-91R/71B, which have a fixed ultrastabl
e rubidium oscillator.
—CNT-90, CNT-91(R):
A variety of RF prescaler options with upper
frequency limits ranging from 3 GHz t
o 20
GHz.
—CNT-91R/71B:
5 Reference frequency outputs covering 100
kHz, 1 MHz, 5 MHz and 10 MHz.
—CNT-90XL:
A number of microwave inputs with upper
frequency limits ranging from 27 GHz to 60
GHz.
—CNT-90(XL):
Optional built-in Li-Ion battery supply
realizes instant high-prescision measurements
in the field and true UPS operation.
—Integrated high performance GPIB inter-
face using SCPI commands.
—A fast USB interface that replaces the tra-
ditional but slower RS-232 serial interface.
—Timestamping; the counter records the rel-
ative position in time of measurements
with high resolution and accuracy.
—A high measurement rate of up to 250
k readings/s to internal memory.
Powerful and Versatile
Functions
A unique performance feature in your new
instrument is the comprehensive arming
possibilities, which allow you to characterize
virtually any type of complex signal
concerning frequency and time.
For instance, you can insert a delay between
the external arming condition and the actual
arming of the counter. Read more about
Arming in Chapter 5, "Measurement
Control".
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
1-2

In addition to the traditional measurement
functions of a timer/counter, these
instruments have a multitude of other
functions such as phase, duty factor,
rise/fall-time and peak voltage. The counter
can perform all measurement functions on
both main inputs (A & B). Most measurement
functions can be armed, either via one of the
main inputs or via a separate arming channel
(E).
By using the built-in mathematics and statistics functions, the instrument can process the
measurement results on your benchtop, without the need for a controller. Math functions
include inversion, scaling and offset.
Statistics functions include Max, Min and
Mean as well as Standard and Allan
Deviation on sample sizes up to 2*109.
You will soon find that your instrument is
more or less self-explanatory with an intuitive
user interface. A menu tree with few levels
makes the timer/counter easy to operate. The
large backlit graphic LCD is the center of information and can show you several signal
parameters at the same time as well as setting
status and operator messages.
Statistics based on measurement samples can
easily be presented as histograms or trend
plots in addition to standard numerical measurement results like m
ax, min, mean and
standard deviation.
The AUTO function triggers automatically on
any input waveform. A bus-learn mode simplifies GPIB programming. With bus-learn
mode, manual counter settings can be transferred to the control
ler for later
reprogramming. There is no need to learn
code and syntax for each individual counter
setting if you are an occasional GPIB bus
user.
State of the Art Technology
Gives Durable Use
These counters are designed for quality and
durability. The design is highly integrated.
The digital counting circuitry consists of just
one custom-developed FPGA and a 32-bit
microcontroller. The high integration and low
component count reduces power
consumption and results in an MTBF of
30,000 hours. Modern surface-mount
technology ensures high production quality.
A rugged mechanical construction, including
a metal cabinet that withstands mechanical
shocks and protects against EMI, is also a
valuable feature.
The use of reciprocal interpolating counting
in this new counter results in excellent
relative resolution: 12 digits/s for all
frequencies.
The measurement is synchronized with the
input cycles instead of the timebase. Simultaneously with the normal "digital" counting,
the counter makes analog measurements of
the time between the start/stop trigger events
and the next following clock pulse. This is
done in four identical circuits by charging an
integrating capacitor with a constant current,
starting at the trigger event. Charging is
stopped at the leading edge of the first
following clock pulse.
The stored charge in
the integrating capacitor represents the time
difference between the start trigger event and
the leading edge of the first following clock
pulse. A similar charge integration is made
for the stop trigger event.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

When the "digital" part of the measurement
is ready, the stored charges in the capacitors
are measured by means of Analog/Digital
Converters.
The counter's microprocessor calculates the
result after completing all measurements, i.e.
the digital time measurement and the analog
interpolation measurements.
The result is that the basic "digital resolution"
of + 1 clock pulse (10 ns) is reduced to 100 ps
for the CNT-90 and 50 ps for the CNT-91(R).
Since the measurement is synchronized with
the input signal
, the resolution for frequency
measurements is very high and independent
of frequency.
The counters have 14 display digits to
ensure that the display itself does not restrict
the resolution.
This instrument is programmable via two interfaces, GPIB and USB.
The GPIB interface offers full general functionality and compliance with the latest standards in use, the IEEE 488.2
1987 for HW
and the SCPI 1999 for SW.
In addition to this 'native' mode of operation
there is also a second mode that emulates the
Agilent 53131/132 command set for easy exc
hange of instrume
nts in operational ATE
systems.
The USB interface is mainly intended for the
lab environment in conjunction with the optional TimeView™ analysis software. The
communication protocol is a proprietary version of SCPI.
These counters are not only extremely
powerful and versatile bench-top
instruments, they also feature extraordinary
bus properties.
The bus transfer rate is up to 4000
triggered measurements/s in CNT-91(R).
Array measurements to the internal
memory can reach 250 k measurements/s.
This very high measurement rate makes new
measurements possible. For example, you
can perform jitter analysis on several tens of
thousands of pulse width measurements and
capture them in less than a second.
An extensive Programmer's Handbook helps
you understand SCPI and counter programming.
The counter is easy to use in GPIB environments. A built-in bus-learn mode enables
you to make all counter settings manually
and transfer them to the controller. The
response can later be used to reprogram the
counter to the same settings. This eliminates
the need for the occasional user to learn all
individual programming codes.
Complete (manually set) counter settings can
also be stored in 20 internal memory
locations and can easily be recalled on a later
occasion. Ten of them can be user protected.
USER MANUAL ● CNT 9x Series ● Rev. 20 December 2017

Even though we know that you are eager to
get going, we urge you to take a few minutes
to read through this part of the introductory
chapter carefully before plugging the line
connector into the wall outlet.
This instrument has been designed and tested
for Measurement Category I, Pollution
Degree 2, in accordance with EN/IEC
61010-1:2001 and CAN/CSA-C22.2 No.
61010-1-04 (including approval). It has been
supplied in a safe condition.
Study this manual thoroughly to acquire adequate knowledge of the instrument,
especially
the section on Safety Precautions hereafter
and the section on Installation on page 1-7.
All equipment that can be connected to line
power is a potential danger to life. Handling
restrictions imposed on such equipment
should be observed.
To ensure the correct and safe operation of
the instrument, it is essential that you follow
generally accepted safety procedures in
addition to the safety precautions specified in
this manual.
The instrument is designed to be used by
trained personnel only. Removing the cover
for repair, maintenance, and adjustment of
the instrument must be done by qualified
personnel who are aware of the hazards
involved.
The warranty
commitments are rendered
void if unauthorized access to the interior
of the instrument has taken place during
the given warranty period.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Statements
CAUTION: Shows where incorrect
procedures can cause damage to, or
destruction of equipment or other
property.
WARNING: Shows a potential danger that
requires correct procedures or practices
to prevent personal injury.
Shows where the protective ground
terminal is connected inside the instrument.
Never remove or loosen this screw.
This symbol is used for identifying
the functional ground of an I/O signal. It is
always connected to the instrument chassis.
Indicates that the operator should
One such symbol is printed on the instrument,
below the A and B inputs. It points out that
the damage level for the input voltage
decreases from 350 V
p to 12Vrms when you
switch the input impedance from 1 M to
50.
Whenever you suspect that it is unsafe to use
the instrument, you must make it inoperative
by doing the following:
—Disconnect the line cord
—Clearly mark the instrument to prevent its
further operation
Do not overlook the safety instructions!
— Inform your Spectracom representative.
For example, the instrument is likely to be unsafe if it is visibly damaged.
If your instrument was ordered with a built-in
battery supply (Option 23/90), it contains 12
Li-Ion cells arranged as a fixed battery pack
with internal protection circuitry.
Even though this type of cell does not cause
environmental damage in the same way as
NiCd, for instance, you should dispose of a
worn-out battery pack at an authorized recycling station or return it to Pendulum.
Note: Individual cells cannot be replaced.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Environmental Considerations
This section provides information about the environmental impact of the product.
Product End-of-Life Handling
Observe the following guidelines when recycling an instrument or component:
Equipment recycling
Production of this equipment required the extraction and use of natural resources. The
equipment may contain substances that could be harmful to the environment or human health
if impropely handled at the product's end of life. To avoid release of such substances into the
environment and to reduce the use of natural resources, we encourage you to recycle this
product in an appropriate system that will ensure that most of the materials are reused or
recycled appropriately.
This symbol indicates that this product complies with European Union
requirements according to Directives 2012/19/EU and 2006/66/EC on waste
electrical and electronic equipment (WEEE) and batteries.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
1-6

Unpacking
Check that the shipment is complete and that
no damage has occurred during
transportation. If the contents are
incomplete or damaged, file a claim with the
carrier immediately. Also notify your local
Pendulum sales or service organization in
case repair or replacement may be required.
Check List
The shipment should contain the following:
— Counter/Timer/Analyzer CNT-90/91 or
Frequency Calibrator/Analyzer CNT-91R
or CNT-91R/71B or Microwave Counter/Analyzer CNT-90XL
N-to-BNC Adapter (only CNT-90/91(R)
with prescaler options having a type N
connector)
Printed version of the Getting Started
Manual
Brochure with Important Information
Certificate of Calibration
Options you ordered should be installed.
See Identification below.
Service Manual (CNT-91R/71B
only)
The type plate on the rear panel shows type
number and serial number. See illustrations
on page 2-5 and 2-6. Installed options are
listed under the menu User Options - About,
where you can also find information on
firmware version and calibration date. See
page 2-15.
The CNT-91R/71B version is identified by a
unique identification marking, or UID. This
permanent tag contains a barcode and allows
customers to track easily their inventory and
property.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Supply Voltage
■ Setting
The Counter may be connected to any AC
supply with a voltage rating of 90 to 265
Vrms , 45 to 440 Hz. The counter automatically
adjusts itself to the input line voltage.
The secondary supply voltages are electronically protected against overload or short circuit. The primary line voltage side is
protected by a fuse located on the power
supply unit. The fuse rating covers the full
voltage range. Consequently there is no need
for the user to replace the fuse under any
operating conditions, nor is it accessible from
the outside.
CAUTION: If this fuse is blown, it is likely
that the power supply is badly damaged.
Do not replace the fuse. Send the counter
to the local Service Center.
Removing the cover for repair, maintenance
and adjustment must be done by qualified
and trained personnel only, who are fully
aware of the hazards involved.
The warranty commitments are
rendered void if unauthorized access to
the interior of the instrument has taken
place during the given warranty period.
■ CNT-90 & CNT-90XL only
It is possible to run the counter from an optional battery supply, Option 23/90.
You must charge the battery before use or
storage. The counter charges the battery
automatically when connected to line power
or an external DC source, whether the
instrument is in standby or turned on. See the
specifications for charging time in different
modes of operation.
Grounding faults in the line voltage supply
will make any instrument connected to it dangerous. Before connecting any unit to the
power line, you must make sure that the protective ground functions correctly. Only then
can a unit be connected to the power line and
only by using a three-wire line cord. No other
method of grounding is permitted. Extension
cords must always have a protective ground
conductor.
CAUTION: If a unit is moved from a cold to
a warm environment, condensation may
cause a shock hazard. Ensure, therefore,
that the grounding requirements are
strictly met.
WARNING: Never interrupt the grounding
cord. Any interruption of the protective
ground connection inside or outside the
instrument or disconnection of the
protective ground terminal is likely to
make the instrument dangerous.
The counter can be operated in any position
desired. Make sure that the air flow through
the ventilation slots at the top, and side panels
is not obstructed. Leave 5 centimeters (2
inches) of space around the counter.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Capacitors inside the instrument can hold
their charge even if the instrument has
For bench-top use, a fold-down support is
been separated from all voltage sources.
available for use underneath the counter. This
support can also be used as a handle to carry
the instrument.
Fig. 1-2 Fold-down support for comfortable
Fig. 1-4
Fitting the rack mount brackets on the
Dimensions for rackmounting hardware.
If you have ordered a 19-inch rack-mount kit
for your instrument, it has to be assembled after
delivery of the instrument. The rackmount kit
consists of the following:
— 2 brackets, (short, left; long, right)
— 4 screws, M5 x 8
— 4 screws, M6 x 8
WARNING: Do not perform any internal
service or adjustment of this instrument
unless you are qualified to do so
Before you remove the cover, disconnect
mains cord and wait for one minute.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

■ Assembling the Rackmount Kit
— Make sure the power cord is
disconnected from the instrument.
— Turn the instrument upside down.
Remove the screws and push the counter
out of the cover.
Undo the two screws (A) and remove
Remove the rear feet by undoing the
two screws (B).
Remove the four decorative plugs (C)
that cover the screw holes on the right
and left side of the front panel.
Grip the front panel and gently push at the
rear.
Pull the instrument out of the cover.
Remove the four feet from the cover.
Use a screwdriver as shown in the following
illustration or a pair of pliers to remove the
springs holding each foot, then push out the
feet.
Removing feet from the cover.
Push the instrument back into the cover.
Mount the two rear feet with the screws
(B) to the rear panel.
Put the two screws (A) back.
Fasten the brackets at the left and right
side with the screws included as illustrated
in Fig 1-6
Fasten the instrument in the rack via
screws in the four rack-mounting holes
The long bracket has an opening so that cables
for Input A, B, and C can be routed inside the
rack.
■ Reversing the Rackmount Kit
The instrument may also be mounted to the
right in the rack. To do so, swap the position
of the two brackets.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

A more elaborate description of the front and
survey, the purpose of which is to make you
rear panels including the user interface with
familiar with the layout of the instrument.
its menu system follows after this
See also the appendix.
Opens the menu from which
you can adjust all settings for
Input B like Coupling,
Impedance and Attenuation.
Opens the menu from which
you can adjust all settings
for Input A like Coupling,
Impedance and Attenuation.
Select measurement parameters such as measurement time, number of
measurements, and so on.
The LED lights up when the
counter is in STANDBY mode,
indicating that power is still
applied to an internal optional
OCXO, if one has been
installed, or to the rubidium
oscillator in the CNT-91R.
Toggling secondary
power switch. Pressing
this button in standby
mode turns the counter
ON and restores the
settings as they were at
power-down.
Menu for selecting one
of a set of formulas for
modifying the
measurement result.
Three constants can
be entered from the
keyboard.
Numerical limits can
also be entered for
status reporting and
recording.
Controls the following
items:
1. Settings memory
2. Calibration
3. Interface
4. Self-test
5. Blank digits
6. About
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Confirms menu
selections without
leaving the menu
level.
selections and
moves up one level
in the menu tree.
CURSOR
CONTROL
marked by text
display, can be
directions.
Adjusts input trigger
voltages
automatically to the
optimum levels for
the chosen
measurement
function.
Double-click for
default settings.
presentation mode
with one main
parameter and a
number of auxiliary
parameters.
presentation
modes. Switching
is done by toggling
the key.
Enters one of three
statistics
Enters the normal
numerical
Initiates one new
measurement if
HOLD is active.
Menu tree for
selecting measurement function.
You can use the
seven softkeys
below the display
for confirmation.
Toggles between
HOLD (one-shot)
mode and RUN
(continuous) mode.
Freezes the result
after completion of a
measurement if
HOLD is active.
Moves up one
menu level without
confirming
selections made.
Exits REMOTE
mode if not
LOCAL
LOCKOUT.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

320 x 97 pixels LCD with backlight for showing
The function of these seven keys is menu demeasurement results in numerical as well
as
pendent. Actual function is indicated on the LCD.
graphical format. The display is also the center of the
Depressing a softkey is often a faster alternative to
dynamic user interface, comprising menu trees,
moving the cursor to the desired position and then
indicators and information boxes.
pressing OK.
Blinking LED
dicates correct
in-
A pending measurement causes
are used for all types of
Sometimes you may want to enter numeric values like the constants
and limits asked for when you are utilizing the postprocessing
features in MATH/LIMIT mode. These twelve keys are to be used for
this purpose.
INPUT
CNT-90/91(R): A
number of optional RF
prescalers are
CNT-90XL: One of
a
number of
microwave
converters is
mounted.
Conn. type dep.
on
frequency
spec.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
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Using the Controls
Rear Panel
Type Plate
Indicates instrument
type and serial number.
Pulse Output
[CNT-91(R) only]
User definable to serve
as output for built-in
pulse generator, gate
indicator or alarm.
Optional Main Input Connectors (not
with Option 23/90)
The front panel inputs can be moved to the rear
panel by means of an optional cable kit. Note
that the input capacitance will be higher.
Fan
A temp. sensor controls the speed
of the fan. Normal bench-top use
means low speed, whereas
rack-mounting and/or options may
result in higher speed.
Protective Ground
Terminal
This is where the protective
ground wire is connected
inside the instrument. Never
tamper with this screw!
Line Power Inle
AC 90-265 VRMS, 45-440 Hz
no range switching needed.
External Arming Input
See page 5-7.
Reference Output 10
MHz derived from the
internal or,
if present,
the external reference.
GPIB Connector
Address set via User Options
Menu.
External Reference Input
Can be automatically selected
if a signal is present and
approved as timebase source,
see Chapter 9.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
USB Connector
Universal Serial Bus (USB)
for data communication with
PC.
Ext. DC Connector
Part of Option 23/90 for
CNT-90(XL).
Range: 12-18 V Note the
polarity.
2-5
o~
=

Additional output frequencies
Connectors
These connectors provide additional output
frequencies which are, from left to right, 100kHz,
Protective Ground
Terminal
This is where the protective
ground wire is connected
inside the instrument. Never
tamper with this screw!
A temp. sensor controls the speed
of the fan. Normal bench-top use
pulse generator, gate
indicator or alarm.
means low speed, whereas
rack-mounting and/or options may
Hz, no range switching
needed.
10 MHz derived from the
internal or, if present, the
Universal Serial Bus (USB)
for data communication with
external reference.
Address set via User Options
selected if a signal is present
and approved as timebase
source, see Chapter 9.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

The charging level indicator shows:
• the relative charging level in percent
Power
The ON/OFF key is a toggling secondary
power switch. Part of the instrument is always
ON as long as power is applied, and this
standby condition is indicated by a red LED
above the key. This indicator is consequently
not lit while the instrument is in operation.
■ CNT-91R and CNT-91R/71B only
While the rubidium oscillator is warming up, an
open padlock symbol labeled RB is flashing at
the top right corner of the display, indicating
that the control loop is not locked. Normal time
to lock is about 5 min. Do not start measuring
until the unlock symbol disappears.
Information exchange between the rubidium
oscillator and the CPU takes place over a serial
bus. Any malfunction in the UART-con-trolled
communication link will be reported in a pop-up
message box on the display.
■ CNT-90(XL) w. Option 23/90
The User Interface Screens have two indicators near the upper right corner of the display.
One is a power supply status indicator and
the other is a battery charging level indicator.
The status indicator shows:
a fixed battery symbol when the internal
battery is the active power source
a charging battery symbol when the internal
battery is being charged
a power plug symbol when the mains is the
active power source
a power plug symbol on top of a battery
symbol when the instrument has been
prepared for UPS operation and charging is
not going on
This hard key is marked MEAS FUNC.
When you depress it, one of the menus
below will open.
CNT-90: Select measurement function.
CNT-90XL: Select measurement
function.
CNT-91(R): Select measurement
function.
The current selection is indicated by text in-
version that is also indicating the cursor position. Select the measurement function you
want by depressing the corresponding softkey
right below the display.
Alternatively you can move the cursor to the
wanted position with the
RIGHT/LEFT arrow
keys. Confirm by pressing
ENTER.
A new menu will appear where the contents
depend on the function. If you for instance
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

have selected Frequency, you can then select
between Frequency, Frequency Ratio and
Frequency Burst. Finally you have to decide
which input channel(s) to use.
By depressing this key once after selecting
the wanted measurement function and input
channel, you will most probably get a
measurement result. The
AUTOSET system
ensures that the trigger levels are set
optimally for each combination of
measurement function and input signal
amplitude, provided relatively normal signal
waveforms are applied. If Manual Trigger has
been selected before pressing the AUTOSET
key, the system will make the necessary
adjustments once (Auto Once) and then
return to its inactive condition.
AUTOSET performs the following functions:
Set automatic trigger levels
Set Auto Trig Low Freq to
100 Hz, if fin>100Hz, or to
f
in,
if 10<fin<100 Hz, or to
A higher value means faster settling time.
By depressing this key twice within two seconds, you will enter the
Preset mode, and a
more extensive automatic setting will take
place. In addition to the functions above, the
following functions will be performed:
• Set Meas Time to 200 ms
• Switch off Hold-Off
• Set HOLD/RUN to RUN
• Switch off MATH/LIM
• Switch off Analog and Digital Filters
• Set Timebase Ref to Auto
• Switch off Arming
An even more comprehensive preset function
can be performed by recalling the factory default settings. See page 2-16.
There are four arrow keys for moving the
cursor, normally marked by text inversion,
around the menu trees in two dimensions.
When no cursor is visible (no active menu selected), the
UP/DOWN arrows are used for
adjusting the LCD display contrast ratio.
The key marked ENTER enables you to confirm a choice without leaving your menu
position.
This hard key is marked EXIT/OK. You will
confirm your selection by depressing it, and
at the same time you will leave the current
menu level for the next higher level.
This hard key is marked CANCEL. By de-
pressing it you will enter the preceding menu
level without confirming any selections made
at the current level.
If the instrument is in
REMOTE mode, this key
is used for returning to
LOCAL mode, unless
LOCAL LOCKOUT has been programmed.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Main and aux. parameters.
Value mode gives single line numerical pre-
sentation of individual results, where the main
parameter is displayed in large characters with
full resolution together with a number of
auxiliary parameters in small characters with
limited resolution.
If Limit Behavior is set to Alarm and Limit
Mode is set to Range you can visualize the de-
viation of your measurements in relation to the
set limits. The numerical readout is now combined with a traditional analog pointer-type instrument, wh
ere the current value is
represented by a "smiley". The limits are
presented as numerical values below the main
parameter, and their positions are marked with
vertical bars labelled LL (lower limit) and UL
(upper limit) on the autoscaled graph.
If one of the limits has been exceeded, the
limit indicator at the to
p of the display will be
flashing. In case the current measurement is
out of the visible graph area, it is indicated by
means of a left or a right arrowhead.
If you want to treat a number of measurements
with statistical methods, this is the key to
operate. There are three display modes
available by toggling the key:
Statistics presented numerically.
In this mode the statistical information is dis-
played as numerical data containing the following elements:
P-P: peak-to-peak deviation
Statistics presented as a histogram.
The bins in the histogram are always
autoscaled based on the measured data. Limits,
if enabled, and center of graph are shown as
vertical dotted lines. Data outside the limits are
not used for autoscaling but are replaced by an
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
2-9

arrow indicating the direction where
example is the Trig Lvl setting as part of the
non-displayed values have been recorded.
This mode is used for observing periodic fluc-
tuations or possible trends. Each plot terminates
(if
HOLD is activated) or restarts (if RUN is
activated) after the set number of samples. The
trend plot is always autoscaled based on the
measured data, starting with 0 at restart. Limits
are shown as horizontal lines if enabled.
When the instrument is controlled from the
GPIB bus or the USB bus, the operating mode
changes to
Remote, indicated by the label
REM on the display. All front panel keys ex-
cept
CANCEL are then disabled. See also page
2-8 for more information on this key.
Sometimes you may want to enter constants
and limits in a value input menu, for instance
one of those that you can reach when you
press the
MATH/LIMIT key.
You may also want to select a value that is not
in the list of fixed values available by pressing
the
UP/DOWN arrow keys. One example is
Meas Time under SETTINGS.
A similar situation arises when the desired
value is too far away to reach conveniently by
incrementing or decrementing the original
value with the UP/DOWN arrow keys. One
Whenever it is possible to enter numeric val-
ues, the keys marked with 0-9;. (decimal
point) and ± (stands for Change Sign)take on
their alternative numeric meaning.
It is often convenient to enter values using the
scientific format. For that purpose, the
rightmost softkey is marked
EE (stands for
Enter Exponent), making it easy to switch between the manti
ssa and the exponent.
Press EXIT/OK to store the new value or
CANCEL to keep the old one.
These keys are mainly used for opening fixed
menus from which further selections can be
made by means of the softkeys or the cursor/select keys.
By depressing this key, the bottom part of the
display will show the settings for Input A (B).
The active settings are in bold characters and
can be changed by depressing the corresponding softkey below the display. You can also
move the cursor, indicated by text inversion, to
the desired position with the
RIGHT/LEFT
arrow keys and then change the active setting
with the
ENTER key.
The selections that can be made using this
menu are:
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Trigger Slope: positive or negative, indicated
by corresponding symbols
Trigger Level:2numerical input via front panel
keyboard. If Auto Trigger is active, you can
change the default trigger level manually as a
percentage of the amplitude.
Always Auto when measuring
risetime or falltime
The absolute level can either be
adjusted using the up/down arrow keys
or by pressing ENTER to reach the
numerical input menu.
Pressing the corresponding softkey or
ENTER opens the Filter Settings menu.
See Fig. 2-10. You can select a fixed
100 kHz analog filter or an adjustable
digital filter. The equivalent cutoff
frequency is set via the value input
menu that opens if you select Digital LP
Frequency from the menu.
Selecting analog or digital filter.
The settings under Input B are equal to those
under Input A.
This key accesses a host of menus that affect
the measurement. The figure above is valid
after changing the default measuring time to 10
Submenu for entering measuring time.
This value input menu is active if you select a
frequency function. Longer measuring time
means fewer measurements per second and
gives higher resolution.
Burst
Entering burst parameters.
This settings menu is active if the selected
measurement function is BURST - a special
case of FREQUENCY - and facilitates measurements on pu
lse-modulated signals. Both
the carrier frequency and the modulating frequency - the pulse repetition frequency (PRF) can be measured, often without the support of
an external arming signal.
2-11
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

start. A typical use is to clean up signals gen-
erated by bouncing relay contacts.
CNT-90 & CNT-90XL: Setting arming
conditions.
CNT-91(R): Setting arming conditions.
Arming is the general term used for the means
to control the actual start/stop of a
measurement. The normal free-running mode is
inhibited and triggering takes place when
certain pretrigger conditions are fulfilled.
The signal or signals used for initiating the
arming can be applied to three channels (A, B,
E), and the start channel can be different from
the stop channel. All conditions can be set via
this menu.
NOTE: Stop Delay can only be used for realizing the
function Timed Totalize in the CNT-91(R).
The trigger hold-off submenu.
A value input menu is opened where you can
set the delay during which the stop trigger
conditions are ignored after the measurement
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Entering statistics parameters.
In this menu you can do the following:
Set the number of samples used for calculation
of various statistical measures.
Set the number of bins in the histogram view.
The delay between measurements, called
pacing, can be set to ON or OFF, and the time
can be set within the range 2 s - 500 s.
Selecting timebase reference source.
Here you can decide if the counter is to use an
Internal or an External timebase. A third al-
ternative is
Auto. Then the external timebase
will be selected if a valid signal is present at
the reference input. The EXT REF indicator at
the upper right corner of the display shows that
the instrument is using an external timebase
reference.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
2-13

CNT-90: The 'Misc' submenu.
Fig. 2-22 CNT-90XL: The 'Input C Acquisition'
submenu.
CNT-90XL: The 'Misc' submenu.
CNT-91(R): The 'Misc' submenu.
The options in this menu are:
Smart Measure with submenus:
■ Smart Time Interval (valid only if the
selected measurement function is Time
Interval)
The counter decides by means
timestamping which measurement channel
precedes the other.
■ Smart Frequency (valid only If the selected
measurement function is Frequency or
Period Average) By means of continuous
timestamping and regression analysis, the
resolution is increased for measuring times
between 0.2 s and
100 s.
• Input C Acquisition (CNT-90XL only)
Auto
means
that the whole specified frequency range
is scanned for valid input signals.
Manual means that a narrow band around the
manually entered center frequency is monitored
for valid input signals. This mode is compulsory
when measuring burst signals but is also recommended for FM signals, when the app
roximate fr
equency is known. An additional
feature is that the measurement results are
presented much faster, as the acquisition
process is skipped.
NOTE: Signal frequencies outside the manual
capture range may cause erroneous results.
In order to draw the operator's attention
to this
eventuality, the sign "M.ACQ" is visible in the
upper right corner of the display.
Auto Trig Low Freq
In a value input menu you can set the lower
frequency limit for automatic triggering and
voltage measurements within the range 1 Hz 100 kHz. A higher limit means faster settling
time and consequently faster measurements.
Timeout
From this submenu you can activate/deactivate
the timeout function and set the maximum time
the instrument will wait for a pending
measurement to finish before outputting a zero
result. The range is 10 ms to 1000 s.
Interpolatator Calibration
By switching off the interpolator calibration, you
can increase the measurement speed at the
expense of accuracy.
TIE (CNT-91 only)
From a submenu you can either let the counter
choose the reference frequency automatically
(Auto) or enter it manually.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Selecting Math or Limits parameters.
You enter a menu where you can choose be-
tween inputting data for the Mathematics or the
Limits postprocessing unit.
The Math branch is used for modifying the
measurement result mathematically before
presentation on the display. Thus you can make
the counter show directly what you want
without tedious recalculations, e.g.
revolutions/min instead of Hz.
The
Limits branch is used for setting numerical
limits and selecting the way the instrument will
report the measurement results in relation to
them.
Let us explore the
Math submenu by pressing
the corresponding softkey below the display.
The display tells you that the Math function is
not active, so press the Math Off key once to
open the formula selection menu.
Select one of the five different formulas,
where K, L and M are constants that the user
can set to any value. X stands for the current
non-modified measurement result.
Selecting formula constants.
Each of the softkeys below the constant labels
opens a value input menu like the one below.
Entering numeric values for constants.
Use the numeric input keys to enter the man-
tissa and the exponent, and use the EE key to
toggle between the input fields. The key
marked X0 is used for entering the display
reading as the value of the constant.
The
Limit submenu is treated in a similar way,
and its features are explored beginning on
page 6-6.
Selecting Math formula for
postprocessing.
2-15
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

CNT-90: The User Options menu.
CNT-90XL & CNT-90 with Option 23/90:
The User Options menu.
CNT-91(R): The User Options menu.
From this menu you can reach a number of
submenus that do not directly affect the
measurement. You can choose between a
number of modes by pressing the
corresponding softkey.
Twenty complete front panel setups can be
stored in non-volatile memory. Access to the
first ten memory positions is prohibited when
Setup Protect is ON. Switching OFF Setup
Protect releases all ten memory positions si-
multaneou
sly.
The different setups can be individually labeled to make it easier for the operator to remember the application.
Fig. 2-32 The memory management menu
after pressing Setup.
The following can be done:
Selecting memory position for saving
a measurement setup.
Browse through the available memory positions
by using the
RIGHT/LEFT arrow keys. For
faster browsing, press the key
Next to skip to
the next memory bank. Press the softkey below
the number (1-20) where you want to save the
setting.
The menu appearance after pressing
Save/Recall.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Fig. 2-34 Selecting memory position for recalling
a measurement setup.
Select the memory position from which you
want to retrieve the contents in the same way
as under Save current setup above. You can
also choose Default to restore the
preprogrammed factory settings. See the
table on page 2-19 for a complete list of
these settings.
Modify labels
Select a memory position to which you want
to assign a label. See the descriptions under
Save/Recall setup above. Now you can enter
alphanumeric characters from the front panel.
See the figure below.
The seven softkeys below the display are
for entering letters and digits in the same
way as you write SMS messages on a cell
phone.
Setup protection
Toggle the softkey to switch between the
ON/OFF modes. When ON is active,
the memory positions 1-10 are all
protected against accidental overwriting.
Entering alphanumeric characters.
The memory management menu after
pressing Dataset.
This feature is available in statistics mode
only, and if HOLD has been pressed prior to
initiating a measurement with
RESTART. Up
to 8 different datasets can be saved in FLASH
memory, each containing up to 32000 samples.
If the pending measurement has more than
32000 samples, only the last 32000 will be
saved. A default label will be assigned to the
dataset. It can be changed in a similar way as
the setup labels. See Modify labels above.
Save
Select a memory position, accept or change the
name, and press
OK.
Recall
Select a memory position and press
OK.
Total Reset
The safety screen below will appear. Pressing
OK will restore all factory settings and erase all
user information.
The Total Reset safety screen.
This menu entry is accessible only for calibration purposes and is password-protected.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
2-17

Press Test Mode to open the menu with avail-
Fig. 2-38 Selecting active bus interface. Bus Type
Select the active bus interface. The alternatives
are GPIB and USB. If you select GPIB, you are
also supposed to select the GPIB Mode and the
GPIB Address. See the next two paragraphs.
GPIB Mode
There are two command systems to choose
from.
Native
The SCPI command set used in this mode fully
exploits all the features of this instrument series.
Compatible
The SCPI command set used in this mode is adapted
to be compatible with Agilent 53131/132/181.
GPIB Address
Value input menu for setting the GPIB address.
Test
A general self-test is always performed every
time you power-up the instrument, but you can
order a specific test from this menu at any time.
Selecting a specific test.
Select one of them and press Start Test to run
it.
Digits Blank
Jittery measurement results can be made easier
for an operator to read by masking one or
more of the LSDs on the display.
Place the cursor at the submenu Digits Blank
and increment/decrement the number by means
of the UP/DOWN arrow keys, or press the soft
key beneath the submenu and enter the desired
number between 0 and 13 from the keyboard.
The blanked digits will be represented by
dashes on the display. The default value for the
number of blanked digits is 0.
Misc (CNT-90XL & CNT-90 with Option
23/90)
The CNT-90XL without Option 23/90 has a
single submenu called Units. By pressing this
softkey you get to the submenu Power. Press
Power and then select dBm or W as the unit of
measurement, when either of the functions
Frequency C or Power C is selected from the
MEAS FUNC menu.
The CNT-90 with Option 23/90 has a single
submenu called Use Battery in Standby. By
toggling this softkey you can decide if the internal OCXO will remain powered or not when
you turn off the instrument in battery operation
mode.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

The CNT-90XL with Option 23/90 has a
combination of the two submenus mentioned
above. See the figure below.
The 'Misc' submenu for
CNT-90XL with battery option.
The rear panel pulse output can be used for
three different purposes:
Press the softkey Output to open the submenu
Fig. 2-42 Selecting output mode and pulse parameters.
Off is the default mode and inhibits all activity
on the output connector.
The pulse generator parameters Period and
Width can be entered by first pressing the
corresponding softkeys, then setting the
numerical values as usual. By placing the
cursor over the parameter, you can also set the
values directly in 1-2-5 steps with the
UP/DOWN arrow keys.
Press Output Mode to enter the mode selection
menu below:
• Gate Open indicates to external equipment
when a measurement is in progress.
Pulse Generator activates a continuous pulse
train having the parameters entered in the
previous menu.
Alarm can be set to be active low or active
high. The MATH/LIM menu is used for setting
up the behavior and the numerical limits that
trigger the alarm.
Output Mode selection menu.
The amplitude is fixed at TTL levels into
50irrespective of the output mode.
About
Here you can find information on:
instrument firmware version
timebase option & calibration date
■ The CNT-91R reports "Rubidium" in this
field.
RF input option
■ The CNT-90XL reports the upper
frequency limit.
This key serves the purpose of manual arming.
A pending measurement will be finished and
the result will remain on the display until a
new measurement is triggered by pressing
the
RESTART key.
■ Restart
Often this key is operated in conjunction with
the
HOLD/RUN key (see above), but it can also
be used in free-running mode, especially when
long measuring times are being used, e.g. to
initiate a new measurement after a change in
the input signal.
RESTART will not affect any
front panel settings.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Input Signaling Conditioning
The input amplifiers are used for adapting
the widely varying signals in the ambient
world to the measuring logic of the
timer/counter.
These amplifiers have many controls, and it
is essential to understand how these
controls work together and affect the signal.
The block diagram below shows the order in
which the different controls are connected.
It is not a complete technical diagram but
in- tended to help understanding the
controls.
The menus from which you can adjust the
settings for th
e two main measurement
channels are reached by pressing
INPUT A
respectively INPUT B. See Figure 3-2. The
active choices are shown in boldface on
the bottom line.
The input impedance can be set to 1 M or 50
by toggling the corresponding softkey.
CAUTION: Switching the impedance to 50
when the input voltage is above 12 VRMS
may cause permanent damage to the input
circuitry.
The input signal's amplitude can be attenuated
by 1 or 10 by toggling the softkey marked
1x/10x.
Use attenuation whenever the input signal ex-
ceeds the dynamic input voltage range ±5 V or
Block diagram of the signal conditioning.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Input Signaling Conditioning
else when attenuation can reduce the influence of
noise and interference. See the section dealing
with these matters at the end of this chapter.
Switch between AC coupling and DC coupling
by toggling the softkey
AC/DC.
AC coupling a symmetrical signal.
Use the AC coupling feature to eliminate un-
wanted DC signal components. Always use
AC coupling when the AC signal is superimposed on a DC voltage that is higher than the
trigger level setting range. However, we recommend AC coupling in many other measurement situations as well.
When you measure symmetrical signals,
such as sine and square/triangle waves, AC
cou- pling filters out all DC components.
This means that a 0 V trigger level is always
cen- tered around the middle of the signal
wher
e triggering is most stable.
Missing trigger events due to AC coupling
of signal with varying duty cycle.
Signals with changing duty cycle or with a
very low or high duty cycle do require DC
coupling. Fig. 3-4 shows how pulses can be
missed, while Fig. 3-5shows that triggering
does not occur at all because the signal ampli-
tude and the hysteresis band are not centered.
NOTE: For explanation of the hysteresis band, see
page 4-3.
No triggering due to AC coupling of signal
with low duty cycle.
If you cannot obtain a stable reading, the signal-to-noise ratio (often designated S/N or
SNR) might be too low, probably less than 6 to
10 dB. Then you should use a filter. Certain
conditions call for special solutions like
highpass, bandpass or notch filters, but usually
the unwanted noise signals have higher
frequency than the signal you are interested in.
In that case you can utilize the built-in lowpass
filters. There are both analog and digital
filters, and they can also work together.
The menu choices after selecting FILTER.
The counter has analog LP filters of RC type,
one in each of the channels A and B, with a
cutoff frequency of approximately 100 kHz,
and a signal rejection of 20 dB at 1 MHz.
Accurate frequency measurements of noisy LF
signals (up to 200 kHz) can be made when the
noise components have significantly higher
frequencies than the fundamental signal.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Input Signaling Conditioning
The digital LP filter utilizes the Hold-Off
function described below.
With trigger Hold-Off it is possible to insert a
deadtime in the input trigger circuit. This
means that the input of the counter ignores all
hysteresis band crossings by the input signal
during a preset time after the first trigger
event.
When you set the Hold-Off time to approx.
75% of the cycle time of the signal, erroneous
triggering is inhibited around the point where
the input signal returns through the hysteresis
band. When the signal reaches the trigger point
of the next cycle, the set Hold-Off time has
elapsed and a new and correct trigger will be
initiated.
Instead of letting you calculate a suitable HoldOff time, t
he counter will do the job for you by
converting the filter cutoff frequency you enter
via the value input menu below to an
equivalent Hold-Off time.
Fig. 3-7 Value input menu for setting the cutoff
frequency of the digital filter.
You should be aware of a few limitations to be
able to use the digital filter feature effectively
and unambiguously. First you must have a
rough idea of the frequency to be measured. A
cutoff frequency that is too low might give a
perfectly stable reading that is too low. In such
a case, triggering occurs only on every 2nd,
3rd or 4th cycle. A cutoff frequency that is too
high (>2 times the input frequency) also leads
to a stable reading. Here one noise pulse is
counted for each half-cycle.
Use an oscilloscope for verification if you are
in doubt about the frequency and waveform of
your input signal.
The cutoff frequency setting range is very
wide: 1 Hz - 50 MHz
Digital LP filter operates in the measuring
logic, not in the input amplifier.
Toggle between manual and automatic triggering with this softkey. When
Auto is active the
counter automatically measures the
peak-to-peak levels of the input signal and sets
the trigger level to 50% of that value. The
attenuation is also set automatically.
At rise/fall time measurements the trigger levels are automatically set to 10% and 90% of
the peak values.
When
Manual is active the trigger level is set
in the value input menu designated
Trig. See
below. The current value can be read on the
display before entering th
e menu.
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3-4

Input Signaling Conditioning
The Auto-function measures amplitude and
calculates trigger level rapidly, but if you aim
at higher measurement speed without having
to sacrifice the benefits of automatic triggering, then use the
Auto Trig Low Freq func-
tion to set the lower frequency limit for voltage measuremen
t.
If you know that the signal you are interested
in always has a frequency higher than a certain value f
lo w , then you can enter this value
from a value input menu. The range for flo w is
1 Hz to 100 kHz, and the default value is 100
Hz. The higher value, the faster measurement
speed due to more rapid trigger level voltage
detection.
Even faster measurement speed can be
reached by setting the trigger levels
manually. See
Trig below.
Follow the instructions here to change the
low-frequency limit:
Press SETTINGS Misc Auto
Use the UP/DOWN arrow keys or the numeric input keys to change the low frequency limit to be used during the trigger
level calculation, (default 100 Hz).
Confirm your choice and leave the SET-
TINGS
menu by pressing EXIT/OK three
times.
Value input menu for entering the trigger
level manually.
Use the
UP/DOWN arrow keys or the numeric
input keys to set the trigger level.
A blinking underscore indicates the cursor po-
sition where the next digit will appear. The
LEFT arrow key is used for correction, i.e.
deleting the position preceding the current
cursor position.
Value input menu for setting the trigger
level.
is probably easier to make small ad-
justments around a fixed value by using the
decrementation. Keep the keys depressed for
faster response
Switching over from AUTO to MAN Trigger
Level is automatic if you enter a trigger level
manually.
Converting "Auto" to "Fixed"
The trigger levels used by the auto trigger can
be frozen and turned into fixed trigger levels
simply by toggling the
MAN/AUTO key. The
current calculated trigger level that is visible
on the display under
Trig will be the new fixed
manual level. Subsequent measurements will
be considerably faster since the signal levels
are no longer monitored by the instrument.
You should not use this method if the signal
levels are unstable.
NOTE: You can use auto trigger on
one input and fixed trigger levels on
the other.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Input Signaling Conditioning
Ignore Noise and
Interference
Sensitive counter input circuits are of course
also sensitive to noise. By matching the
signal amplitude to the counter's input
sensitivity, you reduce the risk of erroneous
counts from noise and interference. These
could otherwise ruin a measurement.
Narrow hysteresis gives erroneous
triggering on noisy signals.
Wide trigger hysteresis gives correct
triggering.
To ensure reliable measuring results, the coun-
ter has the following functions to reduce or
eliminate the effect of noise:
Continuously variable trigger level
Continuously variable hysteresis for some
functions
Analog low-pass noise suppression filter
Digital low-pass filter (Trigger Hold-Off)
To make reliable measurements possible on
very noisy signals, you may use several of the
above features simultaneously.
Optimizing the input amplitude and the trigger
level, using the attenuator and the trigger control, is independent of input frequency and
useful over the entire frequency range. LP filters, on the other hand, function selectively
over a limited frequency range.
The signal needs to cross the 20 mV input
hysteresis band before triggering occurs. This
hysteresis prevents the input from self-oscillating and reduces its sensitivity to noise. Other
names for trigger hysteresis are "trigger
sensitivity" and "noise immunity". They explain the various characteristics of the hysteresis.
Erroneous counts when noise passes
hysteresis window.
Fig. 3-10 and Fig. 3-12 show how spurious
signals can cause the input signal to cross the
trigger or hysteresis window more than once
perinputcycleandgiveerroneouscounts.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
3-6

Input Signaling Conditioning
Trigger uncertainty due to noise.
Fig. 3-13 shows that less noise still affects the
trigger point by advancing or delaying it, but
it does not cause erroneous counts. This trigger uncertainty is of particular importance
when measuring low frequency signals, since
the signal slew rate (in V/s) is low for LF signals. To reduce the trigger uncertainty, it is
desirable to cross the hysteresis band as fast
as possible.
Low amplitude delays the trigger point
Fig. 3-14 shows that a high amplitude signal
passes the hysteresis faster than a low amplitude signal. For low frequency measurements
where the trigger uncertainty is of
importance, do not attenuate the signal too
much, and set the sensitivity of the counter
high.
In practice however, trigger errors caused by
erroneous counts (Fig. 3-10 and Fig. 3-12) are
much more important and require just the opposite measures to be take
n.
To avoid erroneous counting caused by spurious signals, you need to avoid excessive input
signal amplitudes. This is particularly valid
when measuring on high impedance circuitry
and when using 1 M input impedance. Under
these conditions, the cables easily pick up
noise.
External attenuation and the internal 10x
attenuator reduce the signal amplitude, including the noise, while the internal sensitivit
y
control in the counter reduces the counter's
sensitivity, including sensitivity to noise. Reduce excessive signal amplitudes with the 10x
attenuator, or with an external coaxial
attenuator, or a 10:1 probe.
Setting
For most frequency measurements, the optimal
triggering is obtained by positioning the mean
trigger level at mid amplitude, using either a
narrow or a wide hysteresis band, depending
on the signal characteristics.
Timing error due to slew rate.
When measuring LF sine wave signals with
little noise, you may want to measure with a
high sensitivity (narrow hysteresis band) to reduce the trigger uncertainty. Triggering at or
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Input Signaling Conditioning
close to the middle of the signal leads to the
smallest trigger (timing) error since the signal
slope is steepest at the sine wave center, see
Fig. 3-15.
When you have to avoid erroneous counts
due to noisy signals, see Fig. 3-12, expanding
the hysteresis window gives the best result if
you still center the window around the middle
of the input signal. The input signal
excursions beyond the hysteresis band should
For normal frequency measurements, i.e.
without arming, the Auto Trigger function
changes to Auto (Wide) Hysteresis, thus wid-
ening the hysteresis window to lie between
70 % and. 30 % of the peak-to-peak ampli-
tude. This is done with a successive approxi-
mation method, by which the signal's MIN.
and MAX. levels are identified, i.e., the
levels where triggering just stops. After this
MIN./MAX. probing, the counter sets the
trigger levels to the calculated values. The
default relative trigger levels are indicated by
70 % on Input A and 30 % on Input B. These
values can be manually adjusted between 50
% and 100 % on Input A and between 0 %
and 50 % on Input B. The signal, however, is
only applied to one channel.
Before each frequency measurement the
counter repeats this signal probing to identify
new MIN/MAX values. A prerequisite to
enable AUTO triggering is therefore that the
input signal is repetitive, i.e., >100 Hz
(default). Another condition is that the signal
amplitude does not change significantly after
the measurement has started.
NOTE: AUTO trigger limits the maximum measuring
rate when an automatic test system makes
many measurements per second. Here you
can increase the measuring rate by
switching off this probin
g if the signal
amplitude is constant. One single command
and the AUTO trigger function determines the
trigger level once and enters it as a fixed
trigger level.
Switching to Man Trig also means Narrow
Hysteresis at the last Auto Level. Pressing
AUTOSET once starts a single automatic
trigger level calculation (Auto Once). This calculated valu
e, 50 % of the peak-to-peak amplitude, will be the new fixed trigger level,
from which you can make manual adjustments
if need be.
As rule of thumb, stable readings are free from
noise or interference.
However, stable readings are not necessarily
correct; harmonic distortion can cause erroneous yet stable readings.
Sine wave signals with much harmonic distortion, see Fig. 3-17, can be measured correctly
by shifting the trigger point to a suitable level
or by using continuously variable sensitivity,
see Fig. 3-16. You can also use Trigger
Hold-Off, in case the measurement result is not
in line with your expectations.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
3-8

This chapter describes the different
measuring functions of the counter. They
have been grouped as follows:
Frequency measurements
— Frequency
— Period
— Ratio
— Burst frequency and PRF.
— FM
— AM
Time measurements
— Time interval.
— Pulse width.
— Duty factor.
— Rise/Fall time.
See also the front panel layout on page 2-3 to
find the keys mentioned in this section together
with short descriptions.
Press MEAS FUNC to open the main menu for
selecting measuring function. The two basic
methods to select a specific function and its
subsequent parameters are described on page
2-7.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
4-2

FREQ A, B
The counter measures frequency between 0
Hz and 400 MHz on Input A and Input B. The
Auto Trig function operates from 1 Hz
(default
100 Hz) to 300 MHz.
The Manual Trig covers the whole frequency
range
Frequencies above 100 Hz and up to 300
MHz are best measured using the Default
Setup. See page 2-16. Then Freq A will be
selected automatically. Other important
automatic settings are AC Coupling, Auto
Trig and Meas Time 200 ms. See below for
an explanation. You are now ready to start
sing the most common function with a fair
chance to get a result without further
adjustments
Summary of Settings for Good
AC Coupling, because possible DC offset
is normally undesirable.
Auto Trig means Auto Hysteresis in this
case, (comparable to AGC) because
superimposed noise exceeding the normal
narrow hysteresis window will be
suppressed.
Meas Time 200 ms to get a reasonable
tradeoff between measurement speed and
resolution.
Some of the settings made above by recalling
the Default Setup can also be made by
activating the AUTOSET key. Pressing it once
means:
—
Auto Trig. Note that this setting will be
made once only if Man Trig has been selected earlier.
Pressing AUTOSET twice within two seconds
also adds the following setting:
— Meas Time 200 ms.
Fig. 4-1 Frequency is measured as the
inverse of the time between one
trigger point and the next;
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

CNT-90/91(R)
With an optional prescaler the counter can
measure up to 3, 8, 15 or 20 GHz on Input C.
These RF inputs are fully automatic and no
setup is required.
The four versions cover the frequency ranges
27, 40, 46 and 60 GHz by means of an
automatic down-conversion technique described
on page 4-12. Faster (manual) acquisition is an
alternative if the measured frequency is fairly
known. Then its nominal value can be entered
via the keyboard as a fixed starting point for the
acquisition process.
An additional feature is the possibility to
measure signal power with high resolution.
C/B
To find the ratio between two input frequencies, the counter counts the cycles on two
channels simultaneously and divides the
result on the primary channel by the result on
the secondary channel.
Ratio can be measured between Input A and
Input B, where either channel can be the primary or the secondary channel. Ratio can
also be measured between Input C and Input
A or between Input C and Input B. Here
Input C is the primary channel.
Note that the resolution calculations
are very different as compared to
frequency measurements. See page
8-55 for details.
A burst signal as in Fig. 4-2 has a carrier
wave (CW) frequency and a modulation
frequency, also called the pulse repetition
frequency (PRF), that switches the CW signal
on and off.
Both the CW frequency, the PRF, and the
number of cycles in a burst are measured
without external arming signals and with or
without selectable start arming delay. See
Chapter 5 "Measurement Control" for a fundamental discussion of arming and arming delay.
The general frequency limitations for the re-
spective measuring channel also apply to
burst measurements. The minimum number of
cycles in a burst on Input A or Input B is 3
below 160 MHz and 6 between 160 MHz and
400 MHz (using Manual Trigger). Burst mea-
surements on Input C involve prescaling, so
the minimum number of cycles will be 3 x
prescaling factor. The 3 GHz option, for ex-
ample, has a prescaling factor of 16 and re-
quires at least 48 cycles in each burst.
The minimum burst duration is 40 ns below
Bursts with a PRF above 50 Hz can be measured with auto triggering on.
The out-of-sync error described under heading
"Possible errors" on page 4-6 may occur more
frequently when using A
uto Trigge
r.
When PRF is below 50 Hz and when the gap
between the bursts is very small, use manual
triggering.
Always try using AUTOSET first. Then the
Auto Trigger and the Auto Sync functions in
combination will give satisfactory results
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

without further tweaking in most cases. Some-
times switching from AUTO to MANual trig-
gering in the
INPUT A/B menus is enough to
get stable readings. The continually calculated
trigger levels will then be fixed.
Input C has always automatic triggering and
AUTOSET only affects the burst synchroni-
zation.
Manual Presetting
You can measure the frequency on Input A
and Input B to 400 MHz and on Input C with
limited specifications to the upper frequency
limit of the prescaler with the internally synchronized BURST function as follows:
Select Freq Burst under the Freq menu
Select A, B, or C as measurement input.
Press SETTINGS and Burst. Select a Meas
Time that is shorter than the burst duration
If you do not know the approximate burst pa-
rameters of your signal, always start with a
short measurement time and increase it gradually until the readout gets unstable.
Press Sync Delay and enter a value longer
than the burst duration and shorter than the
inverse of the PRF. See Fig. 4-3.
Press Start Delay and enter a value longer
than the transient part of the burst pulse.
Select Frequency Limit (160/400 MHz) if
Input A or Input B is to be used.
Set the sync delay so that it expires
in the gap between the bursts.
Use the low limit if possible to minimize the
number of cycles necessary to make a
measurement.
— Press EXIT/OK to measure.
All relevant burst parameters can be read on
the display simultaneously.
Three time values must be set to
measure the correct part of a burst
■ Selecting Measurement Time
The measurement time must be shorter than the
duration of the burst. If the measurement
continues during part of the burst gap, no matter how small a period of time, then the measurement is ruined. Ch
oosing a measurement
time that is too short is better since it only reduces the resolution. Making burst frequency
measurements on short bursts means using
short measurement times, giving a poorer
resolution than normally achieved with the
counter.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

■ How Does the Sync Delay Work?
The sync delay works as an internal start arming delay: it prevents the start of a new measurement until the set sync delay has expired.
See Fig. 4-5.
After the set measurement time has started,
the counter synchronizes the start of the measurement with the second trigger event in the
burst. This means that the measurement does
not start erroneously during the Burst Off
du-ration or inside the burst.
Measuring the frequency of the
carrier wave signal in a burst.
Before the measurement has been synchronized
with the burst signal, the first measurement(s)
could start accidentally during the presence of
a burst. If this would happen and if the
remaining burst duration is shorter than the set
measurement time, the readout of the first
measurement will be wrong. However, after
this first measurement, a properly set
start-arming sync delay time will synchronize
the next measurements.
In manually operated applications, this is not a
problem. In automated test systems where the
result of a single measurement sample must be
reliable, at
least two measurements must be
made, the first to synchronize the measurement
and the second from which the measurement
result can be read out.
Modulated Signals
A frequency modulated signal is a carrier
wave signal (CW frequency = f
0
) that changes
in frequency to values higher and lower than
the frequency f0. It is the modulation signal
that changes the frequency of the carrier
wave.
The counter can measure:
f0 = Carrier frequency.
fmax = Maximum frequency.
fmin = Minimum frequency.
Δf = Frequency swing = fmax -f0.
Carrier Wave Frequency f
0
To determine the carrier wave frequency
measure f
mean which is a close approximation
of f
0.
Press STAT/PLOT to get an overview of all
the statistical parameters.
Select the measurement time so that the counter measures an integral number of
modulation periods. This way the positive
frequency deviations will compensate the
negative deviations during the measurement.
Example: If the modulation frequency is 50
Hz, the measurement time 200 ms will make
the counter measure 10 complete modulation
cycles.
If the modulation is non-continuous, like a
voice signal, it is not possible to fully
compensate positive deviations with
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
4-6

measuring result that is too high or too low.
In the worst case, exactly half a modulation
cycle would be uncompensated for, giving a
maximum uncertainty of:
tmeasuring x f
modulation
x
π
For very accurate measurements of the carrier
wave frequency f0, measure on the
unmodulated signal if it is accessible.
■ Modulation Frequencies above 1 kHz
— Turn off SINGLE.
— Set a long measurement time that is an
even multiple of the inverse of the modulation frequency.
You
will obtain a good approximation when
you select a long measurement time, for instance 10 s, and when the modu
lation fre-
quency is high, above 1000 Hz.
■ Low Modulation Frequencies
Press SETTINGS
STAT and make the No. of
samples
parameter as large as possible
considering the maximum allowed measurement time. Press
STAT/PLOT and let the
counter calculate the mean value of the samples.
You will usually get
good results with 0.1 s
measurement time per sample and more than
30 samples (n 30). You can try out the opti-
mal combination of sample size and measurement time for specific cases. It depends on the
actual f0 and Δfmax.
Here the sampling frequency of the measurement (1/measurement time) is asynchronous
with the modulation frequency. This leads to
individual measurement results which are randomly higher and lower than f0. The statisti-
cally averaged value of the frequency fmean
approaches f0 when the number of averaged
samples is sufficiently large.
When the counter measures instantaneous frequency values (when you select a very short
measurement time), the RMS measurement
uncertainty of the measured value of f0 is:
where n is the number of averaged samples of
Press SETTINGS
STAT and set No. of
Press Meas Time and select a low value.
Press STAT/PLOT and watch fmax.
Press SETTINGS STAT and set No. of
Press Meas Time and select a low value.
Press STAT/PLOT and watch fmin.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

— Press SETTINGS
STAT and set No.of
samples to 1000 or more.
— Press
Meas Time and select a low value.
Press
STAT/PLOT and watch Δf
p-p
.
Δf
p - p
= f
max
- f
min
= 2 x Δf.
Errors in fmax, f min, and Δfp-p
A measurement time corresponding to 1/10cycle, or 36° of the modulation signal, leads to an
error of approx. 1.5%.
Select the measurement time:
Error when determining f
max
To be confident that the captured maximal fre-
quency really is fmax, you must select a sufficiently large number of samples, for instance n
AM Signals
The counter can usually measure both the carrier wave frequency and modulation
frequency of AM signals. These measurements
are much
like the burst measurements described earlier
The carrier wave (CW) is only continuously
present in a narrow amplitude band in the
middle of the signal if the modulation depth is
high. If the sensitivity of the counter is too low,
cycles will be lost, and the measurement
ruined.
Fig. 4-8 Effects of different sensitivity when
measuring the CW Frequency of an
AM signal.
To measure the CW frequency:
Select a measurement time that gives you
the resolution you want.
Turn on
Manual trigger.
Press
Trig level and enter 0 V trigger level
(press the numeric key 0 and EXIT/OK).
Select 1x attenuation to get a narrow hysteresis band.
If the counter triggers on noise, widen the
hysteresis band with the 'variable hysteresis' function, i.e. enter a trigger level >0 V
but <V
P-Pmin. See Fig. 4-8.
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4-8

The easiest way to measure the modulating
frequency is after demodulation, for instance
by means of a so-called RF-detector probe
(also known as a demodulator probe, e.g.
Pomona type 5815) used with AC-coupling of
the input channel. If no suitable demodulator
is available, use the
Freq Burst function to
measure the modulation frequency in the same
way as when measuring Burst PRF.
Measuring the modulating fre-
quency.
Press MEAS FUNC and select Freq
Press SETTINGS
BurstMeas Time
and enter a measurement time that is
approximately 25 %
of the modulating
period.
—
Press Sync Delay and enter a value that
is approximately 75 %
of the
modulating period. See Fig. 4-3.
Press INPUT A and turn on Manual trigger.
Press Trig and enter a trigger level that
makes the counter trigger according to
Fig. 4-9.
Even though the main frequency reading may
now be unstable, the PRF value on the display
will represent the modulating frequency.
Measurement
Reciprocal Counting
Simple frequency counters count the number
of input cycles during a preset gate time, for
instance one second. This leads to a 1 input
cycle count error that, at least for low-frequency measurements, is a major
contribution to uncertainty.
However, the counters described here use a
high-resolution, reciprocal counting technique, synchronizing the measurement start
with the input signal. In this way an exact
number of integral input cycles will be
counted, thereby omitting the1
input cycle
error
.
Synchronization of a
measurement.
After the start of the set measurement time,
the counter synchronizes the beginning of the
actual gate time with the first trigger event
(t
1) of the input signal. See also Fig. 4-10.
In the same way, the counter synchronizes
the stop of the actual gate time with the input
signal, after the set measurement time has
elapsed. The multi-register counting
technique allows you to simultaneously
USER MANUAL
●
CNT 9x Series ● Rev.20 December 2017

quency according to Mr. Hertz
measure the actual gate time (tg) and the
number of cycles (n) that occurred during this
gate time.
Thereafter, the counter calculates the fre-
's definition:
The '9X' measures the gate time, tg, with a
resolution of 100 ps, independent of the measured frequency. Consequently the use of
prescalers does not influence the quantization
error. Therefore, the relative quantization
error is: 100 ps/tg.
For a 1-second measurement time, this value
is:
Except for very low frequencies, tg and the set
measurement time are nearly identical.
If the input signal disappears during the measurement, the counter will behave like a voltmeter with a sampl
e-and-hold feature and will
freeze the result of the previous measurement.
Mainly for GPIB use, you can manually select
a fixed time-out in the menu reached by pressing
SETTINGSMiscTimeout. The range
of the fixed time-out is 10 ms to 1000 s, and
the default setting is
Off.
Select a time that is longer than the cycle time of
the lowest frequency you are going to measure;
multiply the time by the prescaling factor of the
input channel and enter that time as time-out.
When no triggering has occurred during the
time-out, the counter will show NO SIGNAL.
The set measurement time determines the
measuring speed for those functions that utilize averaging -
Frequency and Period Avg.
For continuous signals,
trigger is on and can be increased to:
when Manual trigger is on, or via GPIB:
■ Average and Single Cycle
Measurements
To reduce the actual gate time or measuring
aperture, the counters have very short meas
urement times a
nd a mode called
Single for
period measurements. The latter means that
the counter measures during only one cycle
of the input signal. In applications where the
counter uses an input channel with a
prescaler, the
Single measurement will last as
many cycles as the division factor. If you
want to measure with a very short aperture,
use an input with a low division factor.
Averaging is th
e normal mode for frequency
and period measurements when you want to
reach maximum resolution. There is always a
tradeoff between time and precision,
however, so decide how many digits you
need and use as short a measurement time as
possible to arrive at your objective.
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4-10

■ CNT-90/91(R): Prescaling May
Influence Measurement Time
Prescalers do affect the minimum measurement time, inasmuch as short bursts have to
contain a minimum number of carrier wave
periods. This number depends on the
prescaling factor.
Fig. 4-11 shows the effect of the 3 GHz
prescaler. For 16 input cycles, the prescaler
gives one square wave output cycle. When the
counter uses a prescaler, it counts the number
of prescaled output cycles, here f/16. The display shows the correct input frequency since
the microcomputer compensates for the effect
of the division factor d as follows:
Prescalers do not reduce resolution in recipro-
cal counters. The relative quantization error is
See Table 4-1 to find the prescaling factors
used in different operating modes.
Signals below 100 Hz should be measured
with manual triggering, unless the default setting (100 Hz) is changed. See page 2-13. The
low limit can be set to 1 Hz, but the measurement process will be slowed down considerably if auto triggering is used in conjunction
with very low frequencies.
When measuring pulses with a low repetition
rate, for example a 0.1 Hz pulse with a
non-prescaled function like PERIOD SGL, the
measurement will require at least the duration
of one cycle, that is 10 seconds, and at worst
nearly 20 seconds. The worst case is when a
trigger event took place just before the beginning of a measure
ment time (Fig. 4-12). Measuring the frequency of the same signal will
take twice as long, since this function involves
prescaling by a factor two.
Even if you have chosen a short measurement
time, this measurement will require between 20
and 40 seconds (for this example).
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CNT 9x Series ● Rev.20 December 2017

■ CNT-90XL: Microwave Conversion
As mentioned before, a prescaler in the
C-in-put divides the input frequency before it is
counted by the normal digital counting logic.
The division factor is called prescaler factor
and can have different values depending on the
prescaler type. The 3 GHz prescaler is designed
for a prescaling factor of 16. This means that an
input C frequency of, e.g., 1.024 GHz is
transformed to 64 MHz.
Prescalers are designed for optimum perform
ance when measu
ring stable continuous RF.
Most prescalers are inherently unstable and
would self-oscillate without an input signal. To
prevent a prescaler from oscillating, a
"go-detector" is incorporated. See Fig. 4-13.
The go-detector continuously measures the
level of the input signal and simply blocks the
prescaler output when no signal, or a signal that
is too weak, is present.
Go-detector in the prescaler.
The presence of a burst signal to be measured
makes certain demands upon the signal itself.
Regardless of the basic counter's ability to
measure during very short measurement times,
the burst duration must meet the following
minimum conditions:
Burst
min
> (presc. factor) x (inp. cycle time) x 3
or at least 80 ns
Normally the real minimum limit is set by other
factors, like the speed of the GO-detector. This
speed depends on the specific input option
used.
Measuring frequencies up to 20 GHz is possible with the top-performance prescaler option
14B. The general principles of prescalers are
described in the preceding paragraph.
The different versions of the CNT-90XL are
intended for applications with upper frequency
limits between 27 GHz and 60 GHz.
Here another technique is utilized, down
conversion by means of mixing the unknown
signal with known LO frequencies until there
is a signal present within the passband of the
IF amplifier, in this case 10 - 200 MHz.
A simplified block diagram can be seen in Fig.
4-14.
Microwave acquisition in the
CNT-90XL.
The basic LO frequency range is 430 -
550
MHz and is divided into a number of discrete
frequencies fetched from a look-up table. The
LO output is fed to a comb generator that creates a harmonic spectrum covering the whole
specified microwave range.
The automatic process of calculating the input
frequency consists of the following steps:
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4-12

The purpose of this process is to find out
if there is a measurable signal present at
the input, and if so, fix the LO frequency
that gives rise to an IF signal above a certain threshold lev
el. This is done by sequentially stepping the LO from the
highest value in the look-up table to the
lowest value and applying the resulting
comb generator spectrum to the mixer.
The process is stopped when the signal
detector outputs a status signal to the
processor.
Acquisition
We don't know yet which harmonic
generates the IF signal. First we measure
the IF with the counter. Then we decrease
the LO frequency by 1 MHz and measure
the IF once more. If, for instance, the
difference between the two values is 5
MHz, then we know that the fifth
harmonic is the origin. By examining the
sign of the difference, we can decide if
the original IF should be added to or
subtracted from the calculated harmonic
in order to arrive at
the final value.
Final RF calculation
Now we know the LO frequency, the
multiplication factor 'n' and the sign.
What remains to be done is to count the
IF during a measurement time
corresponding to the desired resolution,
and then the result is used for calculating
the final value to be presented on the
display as: f
x = n x f
LO
± IF
There are a number of conditions that can
complicate the acquisition process. All of
them are handled by measures taken by the
instrument firmware. Two examples:
— One of the step frequencies produces an
IF but not its shifted value. Action: go to
the next table value.
Frequency modulation causes an unstable
'n' value calculation. Action: increase the
measuring time.
Another feature in this instrument is the ability to measure power with high resolution and
moderate accuracy over the entire frequency
range, achieved by storing individual frequency dependent power correction factors in
a memory located inside the conversion unit.
This memory is also used for storing other inf
ormation about t
he converter like identification data.
Single A, B & Avg. A, B, C
From a measuring point of view, the period
function is identical to the frequency function.
This is because the period o f a cyclic signal
has the reciprocal value of the frequency (1/f).
In practice there are two minor differences.
1. The counter calculates FREQUENCY
(always AVG) as:
while it calculates PERIOD AVG as:
2. In the PERIOD SINGLE mode, the counter
uses no prescaler.
All other functions and features as described
earlier under "Frequency" apply to Period
measurements as well.
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This function benefits from the basic
time-stamping calculation method utilized by
this series of counters to obtain consecutive
measurement results without dead time.
Every positive or negative zero crossing (depending on the selected slope) up to the maximum frequency (125 kHz with interpolator
calibration ON or 250 kHz with interpolator
calibration OFF) is time-stamped. For every
new time stamp the previous value is subtracted from the current value and displayed.
In VALUES mode the display is updated every new period if the period time exceeds 200
ms. For shorter times every second, third etc.
result is displayed due to the limited updating
rate.
In STATISTICS mode the graphs and
statisti-cal data contain all periods up to
the maxi-mum input frequency (see above).
For higher frequencies the average period
time during the 4 or 8 µs observation time
is displayed. So, for higher frequencies the
actual function is rather Period Average Back-
to-Back.
The main purpose of this function is to make
continuous measurements of relatively long
period times without losing single periods due
to result processing. A typical example is the
1-pps timebase output from GPS receivers.
Frequency A, B
Back-to-Back
■ CNT-91(R) only
This is the inverse function of Period
Back-to-Back. In
STATISTICS mode mea-
surement time is used for pacing the time
stamps. The pacing parameter is not used in
this case.
Thus a series of consecutive frequency aver-
age measurements without dead time can be
made in order to fulfil the requirements for
correct calculation of Allan variance or
deviation. These statististical measures are,
for instance, widely used by oscillator
manufacturers to describe short-term
stability.
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Measuring the time between a start and a stop
condition on two separate channels is the basis
for all time interval measurements. In addition
to the fundamental function
Time Interval A to
B,
the counters also offer other channel
combinations and derived functions like
Pulse
Width
and Rise/Fall Time.
Time is measured between the
trigger point and the reset point. Accurate
measurements are possible only if the
hysteresis band is narrow.
Triggering
The set trigger level and trigger slope define
the start and stop triggering.
If Auto is on, the counter sets the trigger level
to 50% of the signal amplitude, which is ideal
for most time measurements.
Summary of Conditions for Reliable
Auto Once, that is freezing the levels de-
termined by
Auto Trig, is normally the
best choice when making time measurements. Choose
Man Trig and press
AUTOSET once.
1x Attenuation. Selected automatically if
AUTOSET was used before to set the
trigger levels.
Even though the input amplifiers have high
sensitivity, the hysteresis band has a finite
value that would introduce a small timing
error for signals with different rise and fall
times, for instance asymmetrical pulse signals
like the one in Fig. 4-15. This timing error is
taken care of by using hysteresis compensation
USER
MANUAL ● CNT 9x Series ● Rev.20 December 2017

that virtually moves the trigger points by half
All time interval functions can be found under
the function menu
Time.
The toggling SLOPE keys (marked with a
under the menus INPUT A/B decide which edge
of the signal will start resp. stop the measurement.
The counter measures the time between a start
condition on input A and a stop condition on
input B.
The counter measures the time between a start
condition on input B and a stop condition on
input A.
Time Interval A to A, B to B
When the same (common) signal source supplies both start and stop trigger events, connect
the signal to either input A or input B.
These functions can be used for measuring
rise and fall times between arbitrary trigger
levels.
CNT-91(R): Time
Interval Error (TIE)
This function can be found under the function
menu Time and is only applicable to clock
signals, not data signals.
TIE measurement uses continuous
time-stamping to observe slow phase shifts
(wander) in nominally stable signals during
extended periods of time. Monitoring distributed PLL clocks in synchronous data transmission systems is a typical application.
The frequency of the signal to be checked can
be either manually or automatically set. Auto
detects the frequency from the first two samples. The value is rounded to four digits, e.g.
2.048 MHz and is output on the bus when a
query is sent. It is also displayed as an auxiliary parameter in VALUE mode.
TIE is measured as the time interval between
the input signal and the internal or external
timebase clock. These signals are not
phase-locked, so irrespective of the real time
interval value at the start of a measurement, the
result at t = 0 is mathematically nulled. Thus
the graphic representation in STATIS-TICS
mode starts at the origin of coordinates.
Rise/Fall Time A/B
These functions can be found under the function menu Time.
Rise and fall time can be measured on both input A and input B.
By convention, rise/fall time measurements
are made with the trigger levels set to 10 %
(start) and 90 % (stop) of the maximum pulse
amplitude, see Figure 4-16.
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4-16

The counter measures the time from when the
signal passes 10 % of its amplitude to when it
passes 90 % of its amplitude. The trigger levels are calculated and set automatically.
Auxiliary parameters shown simultaneously
are Slew Rate (V/s), Vmax and Vmin
Trigger levels for rise/fall mea-
surements.
For ECL circuits, the reference levels are 20
% (start) and 80 % (stop). In this case you can
use either of two methods:
1. Select the general Time Interval function
described above and set the trigger levels manually after calculating them from the absolute
peak values. Then you can benefit from the
auxiliary parameters Vmax and Vmin. For
measurements made on input A, use the following settings:
Rise
Time:
Trig Level A = V
min +0.2(Vmax - Vmin)
Trig Level B = Vmin +0.8(Vmax - Vmin)
Fall Time:
Trig Level A = Vmin +0.8(Vmax -
Trig Level B = Vmin +0.2(V
max
- V
min
)
2. Select one of the dedicated Rise/Fall Time
functions, and exploit the possibility to manually adjust the re
lative trigger levels (in %)
when Auto Trigger is active. Both input
channel menus are used for entering the levels,
but only one channel is the active signal input.
See the paragraph on Auto Trigger (page 4-19)
to find out how overshoot or ringing may 71Bfect your measurement.
The function menu designation is Pulse.
Either input A or input B can be used for measuring, and both po
sitive and negative pulse
width can be selected.
Positive pulse width means the time be-
tween a rising edge and the next falling
edge.
Negative pulse width means the time between a falling edge and the next rising
edge.
The selected trigger slope is the start trigger
slope. The counter automatically selects the
inverse polarity as stop slope.
The function menu designation is Pulse.
Either input A or input B can be used for measuring, and both positive and negative duty
factor can be selected. See the preceding paragraph for a definition of positive and negative
in this context.
Duty factor (or duty cycle) is the ratio between
pulse width and period time. The counter
determines this ratio by first making a pulse
width measurement, then a period measurement, and calculates the duty factor as:
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

The total measurement time will be
doubled compared to a single
measurement, because "Duty"
requires 2 measurement steps.
Hysteresis
The trigger hysteresis, among other things,
causes measuring errors, see Figure 4-17. Actual triggering does not occur when the input
signal crosses the trigger level at 50 percent of
the amplitude, but when the input signal has
crossed the entire hysteresis band.
The hysteresis band is about 20 mV with at-
tenuation 1x, and 200 mV with attenuation
10x.
To keep this hysteresis trigger error low, the
attenuator setting should be 1x when possible.
Use the
10x position only when input signals
have excessively large amplitudes, or when
you need to set trigger levels higher than 5 V.
Rounding
Additional timing errors may be caused by
triggering with insufficient overdrive, see Figure 4-18. When triggering occurs too close to
the maximum voltage of a pulse, two phenomena may influence your measurement uncertainty: overdrive and rounding.
Insufficient overdrive causes
Trigger Error.
Overdrive: When the input signal crosses the
hysteresis band with only a marginal
overdrive, triggering may take some
100 ps longer than usual. The specified
worst case 500 ps systematic trigger
error includes this error, but you can
avoid it by having adequate overdrive.
Rounding: Very fast pulses may suffer from
pulse rounding, overshoot, or other
aberrations. Pulse rounding can cause
significant trigger errors, particularly
when measuring on
fast circuitry.
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4-18

Auto Trigger is a great help especially when
you measure on unknown signals. However,
overshoot and ringing may cause
Auto to
choose slightly wrong MIN and MAX signal
levels. This does not affect measurements like
frequency, but transition time measurements
may be affected.
Therefore, when working with known signals
such as logic circuitry, set the trigger levels
manually.
Always use manual trigger levels if the signal
repetition rate is > 300 MHz or drops below
100 H
z (default), or below the low frequency
limit set by entering a value between 1 Hz and
50 kHz in the menu
Auto Trig Low Freq. You
can reach it by pressing
SETTINGSMisc.
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● CNT
9x Series ● Rev.20 December 2017

channel B are enough to calculate the result,
Phase is the time difference between two signals of the same frequency, expressed as an
angle.
The traditional method to measure phase de-
lay with a timer/counter is a two-step process
consisting of two consecutive measurements,
first a period measurement and immediately
after that a time interval measurement. The
phase delay is then mathematically calculated
as:
360°x (Time Interval A- B )
or in other words:
Phase A -B = 360°x Time Delay x FREQ
A somewhat more elaborate method is used in
these counters. It allows the necessary meas
urements to be pe
rformed in one pass by using time-stamping. Two consecutive
time-stamps from trigger events on channel A
and two corresponding time-stamps from
Traditional phase definition.
The frequency range for phase is up to 160
MHz and the resolution depends on the
frequency. For frequencies below 100 kHz
the resolution is 0.001° and for frequencies
above 10 MHz it is 1°. It can be further
improved by averaging through the built-in
statistics functions.
Phase can be measured on input signal frequencies up to 160 MHz. However, at these
very high frequencies the phase resolution is
reduced to:
100ps x 360° x FREQ
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The inaccuracy of Phase A-B measurements
depends on several external parameters:
Peak amplitude and slew rate for input
signals A and B
Some internal parameters are also important:
— Internal time delay between channel A
and B signal paths
— Variations in the hysteresis window be-
tween channel A and B
Let us look deeper into the restrictions and
possibilities of using phase measurements.
Inaccuracy: The measurement errors are of
two kinds:
— Random errors
— Systematic errors
The random errors consist of resolution
(quantization) and noise trigger error.
Systematic errors consist of "inter-channel
delay difference" and "trigger level timing"
errors. Systematic errors are constant for a
given set of input signals, and in general, you
can compensate for them in the controller
(GPIB-systems) or locally via the
MATH/LIM
menu (manual operation) after making calibration measurements. See Methods of Com-
pensation on page 4-23.
The phase quantization error algorithm is:
100 ps x FREQ x 360°
For example, the quantization error for a 1
MHz input signal is thus:
100 ps x 1 x 10
6
x 360° 0.04°
The trigger noise error consists of start and
stop trigger errors that should be added. For
sinusoidal input signals each error is:
Let's use the example above and add some
noise so that the S/N ratio will be 40 dB. This
corresponds to an amplitude ratio of 100
times (and power ratio of 10000 times). Then
the trigger noise will contribute to the random
error with:
The sum of random errors should not be
added linearly, but in an "RMS way", because
of their random nature. Let's do so for our
examples above.
Random error =
The total random errors are thus:
What about random errors caused by internal
amplifier noise? Internal noise contribution is
normally negligible. The phase error caused
by noise on the signal, whether internal or external, is:
For an input signal of 250 mV
rms
and the typi-
cal internal noise figure of 250 V
rms gives us
a S/N-ratio of a minimum of 60 dB (1000
times). This gives us a worst case error of
0.06°. Increasing the input signal to 1.5 V
rms
decreases the error to 0.01°.
Another way to decrease random errors is to
use the statistics features of the instrument
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● CNT 9x Series ● Rev.20 December 2017

and calculate the mean value from a number
■ Systematic Errors in Phase
Measurements
Systematic errors consist o f 3 elements:
— Trigger level timing errors (start and
stop), due to trigger level uncertainty.
The inter-channel propagation delay differ-
ence is typically 500 ps at identical trigger
conditions in both input channels. Therefore,
the corresponding Phase difference is:
Phase difference caused by
inter-channel propagation delay difference
Trigger level timing error
The "trigger level timing error" is depending
on two factors:
— The actual trigger point is not exactly
zero, due to trigger level DAC uncertainty
and comparator offset error.
— The two signals have different slew rates
at the zero-crossing.
Every counter has input hysteresis. This is
necessary to prevent noise to cause erroneous
input triggering. The width of the hysteresis
band determines the maximum sensitivity of
the counter. It is approximately 30 mV, so
when you set a trigger level of 0 V, the actual
trigger point would normally be +15 mV and
the recovery point -15 mV. This kind of tim-
ing error is cancelled out by using hysteresis
compensation.
Hysteresis compensation means that the microcomputer c
an offset the trigger level so
that actual triggering (after offset) equals the
set trigger level (before offset). This general
hysteresis compensation is active in phase as
well as in time interval and rise/fall time
measurements. There is a certain residual
uncertainty of a few mV and there is also a
certain temperature drift of the trigger point.
The nominal trigger point is 0 V with a
n un-
certainty of ± 10 mV.
A sine wave expressed as V(t) = VPx sin (2π
the zero-crosssing. That gives us the
systematic time error when crossing 10 mV,
instead of crossing 0 mV.
And the corresponding phase error in
This error can occur on both inputs, so the
worst case systematic error is thus:
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Worst case
systematic error
Systematic trigger level timing
The calculations above show the typical uncertainties in the constituents that make up the
total systematic error. For a given set of input
signals you can compensate for this error
more or less completely by making
calibration measurements. Depending on the
acceptable residual error, you can use one of
the methods described below. The first one is
very simple but does not take the
inter-channel propagation delay difference
into account. The second one includes all
systematic errors, if it is carried out
meticulously, but it is often not practicable.
Common
settings for the two inputs are:
Slope:
Coupling:
Impedance:
Pos or Neg
AC
1 Mor 50depending on
source and frequency
Trigger:
Trigger Level:
Filter:
Method 1:
Connect the test signals to Input A
and Input
B. Select the function Phase A rel A to find
the initial error. Use the MATH/LIM menu to
enter this value as the constant L in the formula K*X+L by pressing X0 and change sign.
Now the current measurement result (X0) will
be subtracted from the future phase measurements made by selecting Phase A rel B.A
considerable part of the systematic phase errors will thus be cancelled out. Note that this
calibration has to be repeated if the
frequency or the amplitude changes.
Method 2:
Connect one of the signals to be measured to
both Input A and Input B via a 50 power
splitter or a BNC T-piece, depending on the
source impedance. Make sure the cable
lengths between power splitter / T-piece and
instrument inputs are equal. Select the function
Phase A rel B and read the result. Enter
this value as a correction factor in the same
way as described above for Method 1.
In order to minimize the errors you should
also maintain
the signal amplitudes at the inputs, so that the deviation between
calibration and measurement is kept as small
as possible.
The same restrictions as for Method 1
regarding frequency and amplitude apply to
this method, i.e. you should recalibrate
whenever one of these signal parameters
changes.
Residual Systematic Error:
By mathematically (on the bench or in the
controller) applying corrections according to
one of the methods mentioned above, the
systematic error will be reduced, but not
fully eliminated. The residual time delay
error will most probably be negligible, but a
trigger level erro
r will always remain to a
certain extent, especially if the temperature
conditions are not constant.
USER MANUAL ● CNT 9x
Series ● Rev.20 December 2017

Totalize
[CNT-91(R) only]
The Totalize functions add up the number of
trigger events on the two counter inputs A
and B. Several combinations of them are
theoretically possible. Five have been realized
and made available by entering the Totalize
menu.
In addition to controlling the gate manually
by toggling
HOLD/RUN you can also open
and close the gate by using the arming
facilities under
SETTINGS. The different
functions are described below.
The display is updated continually while the
gate is open. Events are accumulated during
consecutive open periods until
RESTART is
pressed.
The manual Totalize functions can
not be used in conjunction with the
Statistics functions and parameters
like block and pacing. Nor does Auto
Trigger work the normal way. An Auto
Once is performed instead before the
start of a measurement in order to
calculate suitable trigger levels once.
This mode enables you to totalize (count) the
number of trigger events on Channel A.
Aux- iliary calculated parameters are
A-B
and A/B. Start/Stop is manually controlled
by toggling the key
HOLD/RUN, and the
counting regis- ters are reset by pressing
RESTART.
This mode enables you to totalize (count) the
number of trigger events on Channel B.
Aux- iliary calculated parameters are A-B
and A/B. Start/Stop is manually controlled
by toggling the key
HOLD/RUN, and the
counting regis- ters are reset by pressing
RESTART.
This mode enables you to calculate the sum
of trigger events on Channel A and Channel
B. Auxiliary parameters are
A and B.
Start/Stop is manually controlled by toggling
the key HOLD/RUN, and the counting
registers are reset by pressing
RESTART.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

TOT A-B MAN
This mode enables you to calculate the
difference between trigger events on Channel
A and Channel B. Auxiliary parameters are A
and B. Start/Stop is manually controlled by
toggling the key HOLD/RUN, and the
counting registers are reset by pressing
RESTART.
Applications
The TOT A-B MAN makes it possible, for
instance, to make differential flow measurements in control systems.
Example: the number of cars in a parking lot
equals the number of cars passing the entrance
(A) gate, minus the ones passing the exit (B)
gate.
TOT A/B MAN
This mode enables you to calculate the ratio
of trigger events on Channel A and Channel
B. Auxiliary parameters are A and B.
Start/Stop is manually controlled by toggling
the key HOLD/RUN, and the counting registers are reset by pressing RESTART
Totalize & Arming
By using Arming together with Totalize you
can open and close the gate with an external
signal applied to one of the channels A, B or
E. In this way you can realize a host of func-
tions like TOT A START/STOP by B, TOT
A-B Gated by E and TOT B Timed by A,
simply by selecting channel, slope and delay
time for Start/Stop.
Unlike the manual Totalize functions, the
armed variants resemble the other measurement functions inasmuch as they allow block
and pacing control. Consequently all the Sta-
tistics functions are available. A new result is
displayed after each stop condition.
The comprehensive Arming features can be
found under
SETTINGS Arm.
In order to set up the Totalize functions
above, do the following:
—Select Totalize from the MEAS FUNC
menu and then A.
— Connect the signal to be measured to
Input A.
— Set the trigger level for Input A
manually to a suitable value.
—
Connect the control signal to Input B.
—
Set the trigger level for Input B
manually to a suitable value.
— Go to the Arming menu (SETTINGS
Arm)
and set the seven parameters:
— Arm on Sample/Block
Decide if each event or each block
of events
(STATISTICS mode) shoul
d be
armed.
— Start Channel
Select
B.
— Start Slope
Select POS (marked by a rising
edge symbol).
— Start Delay
Decide if you need to insert a delay
(10 ns - 2 s) between the control signal
and the actual opening of the gate.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Decide if you need to insert a delay (10
ns - 2 s) during which the gate will not
respond to the control signal on the
Stop Channel. The main application is
to prevent relay contact bounces from
closing the gate prematurely.
—
Stop Channel
Select POS (marked by a rising edge
—Select Totalize from the MEAS FUNC
— Connect the signals to be measured to In-
— Set the trigger levels for Inputs A and B
manually to suitable values.
—
Connect the control signal (TTL levels) to
— Go to the Arming menu (SETTINGS
Arm) and set the seven parameters:
— Arm on Sample/Block
Decide if each event or each block of
events (STATISTICS mode) should be
armed.
—
Start Channel
Select
E.
—
Start Slope
Select POS (marked by a rising edge
—
Start Delay
Decide if you need to insert a delay (10
ns - 2 s) between the control signal and
the actual opening of the gate.
— Stop Delay
Decide if you need to insert a delay (10
ns - 2 s) during which the gate will not
respond to the control signal on the Stop
Channel. The main application is to
prevent relay contact bounces from
closing the gate prematurely.
Select E.
—
Stop Slope
Select NEG (marked by a falling edge
symbol).
■ TOT B Timed by A
—
Select Totalize from the MEAS FUNC
—
Connect the signal to be measured to Input
B.
—
Set the trigger level for Input B manually
to a suitable value.
—
Connect the control signal to Input A.
—
Set the trigger level for Input A manually
to a suitable value.
—
Go to the Arming menu (SETTINGS
Arm)
and set the six parameters:
— Arm on Sample/Block
Decide if each event or each block of
events
(STATISTICS mode) should be armed.
— Start Channel
Select
A.
— Start Slope
Select POS (marked by a rising edge
symbol).
— Start Delay
Decide if you need to insert a delay (10
ns - 2 s) between the control signal and
the actual opening of the gate.
— Stop Delay
Set the measurement time between 10
ns and 2 s.
— Stop Channel
Select Time.
With this function you can synchronize the
start of an accurate gate time to an external
event.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Press MEAS FUNC Volt. The counter can
measure the input voltage levels V
MAX , VMIN
and VPP on DC-input voltages and on repetitive
signals between 1 Hz and 400 MHz.
The default low frequency limit is 20 Hz but
can be changed via the SETTINGS
The voltage is determined
by making a series of trigger
leve settings and sensing
when the counter triggers.
Miscellaneous menu between 1 Hz and 50
kHz. A higher low-frequency limit means
faster measurements.
The voltage capacity is -50 V to +50 V in two
automatically selected ranges.
For LF signals the measurement has "voltmeter
performance", i.e. an accuracy of about 1 % of
the reading.
You can select any one of the parameters to be
the main parameter that is displayed in large
digits and with full resolution, while the others
are displayed simultaneously at the bottom of
the display in smaller characters.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

When the waveform (e.g. sinusoidal, triangular, square) of the input signal is known, its
crest factor, defined as the quotient (QCF) of
the peak (V
p) and RMS (Vrms) values, can be
used to set the constant K in the mathematical
function K*X+L. The display will then show
the actual Vrms value of the input signal,
assuming that Vpp is the main parameter.
EXAMPLE: A sine wave has a crest factor of
1.414 ( ), so the constant in the formula above will be 0.354.
Press MATH/LIM and after that Math→
Math(Off) →K*X+L Press K= and enter
0.354 via the NUMERIC ENTRY keys.
Check that the L constant is set to its
default setting 0. Confirm your choices
with the softkeys below the display. If
the input is AC coupled and V
pp
selected, the display will now show the
RMS value of any sine wave input.
If the sine wave is superimposed on a DC
voltage, the RMS value is found as: 0.354*Vpp
+ VDC. If VDC is not known it can be found as:
To display the rms value of a sine wave super-
imposed on a DC voltage, follow the example
above, but set L = VDC.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

[CNT-90 XL option 28 only]
I
NTRO DUCTI ON
The option 28, named Pulsed RF option, allows the CNT-90X L
counter to measure pulsed RF signal characteristics. A pulsed signal
can be defined by some parameters, as described below.
Frequency in pulse (FP): also known as carrier frequency or
frequency in burst is the signal frequency within the pulse.
Pulse Width (PW): it is the pulse duration.
Pulse Repetition Interval (PRI): it is the pulse period of repetition.
Pulse Repetition Frequency (PRF): it is the reciprocal of the PRI.
Pulse Power level (Pon) is the signal level and is showed in dBm.
S
ETTING S
To be able to measure pulsed signal main characteristics, the
CNT-90XL option 28 has a special set of measurement settings.
Start Dela y: internal signals may need some time to be properly
established. Start delay is useful to skip initial signal transie nt
response to make sure that measurement starts when signal is stable.
Measurement time is the time during which the measurement is
actually done. NOTE that measurement time must be shorter than the
pulse width with some margin.
Pulse Sensitivity setting ; High/Medium/Low, corresponds to the
trigger level selected for the internal pulse envelope detector signal.
This setting depends on the RF signal power level.
In most cases, best values to use for start delay and
measurement
time are respectively 10% and 80% of pulse width.
NOTE: Measurement time should end min. 40 ns before end of pulse!
Example: For a 100ns pulse, the recommended start delay is 10 ns
and Meas. Time is 50ns
Sensitivity
Pon<
-8dBm
HIGH
sensitivity
-8dBm < Pon<
-3dBm
MEDIUM
sensitivity
Pon>
-3dBm
LOW
sensiti vity
settings:
NEED ED
S
ETTING S
Depending on selected measurement, some parameters need to be
properly defined to get a correct result. The following table
summarizes needed settings for each measurement function.
Manual Acq & Center freq.
Start Delay
Measurement Time
Sensitivity
Frequency in Pulse X X X X
Pulse Width X X
Pulse repetition interval X X
Power in pulse X X X
4-29
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

ME ASUREMEN TS
If Option 28 is installed in CNT-90XL, the Pulsed RF measurements
are found by pressing the MEAS key and selecting Pulsed RF:
The various Pulsed RF parameters are thereafter displayed:
Width (Pulse Width and Duty Factor)
Power On (the power in Pulse during On time)
F
REQUENCY IN PULSE
Select Frequency measurement via the menu
-
MEAS
→
Pulsed RF
→
Freq in Pulse
→
C
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
-
-
-
(this function is also available via the
- MEAS
→
Repetition
→
PRI →C menu).
Set corresponding masureent settings in the following menus:
-
SETTINGS → Pulsed RF
4-29
SETTINGS P ulsed RF Start Delay
SETTINGS P ulsed RF Meas Time
SETTINGSPulsed RFSensitivity
And finally select Manual acquisition with a center frequency that
is close to expected frequency (within 500 MHz)
- SETTINGS
→
Misc → Input C Acq → Center frequency
PRI
Select Pulse Repetition Interval measurement via the
- MEAS →Pulsed RF →Repetition →PRI →C.
Set corresponding measurement settings in the following menus:
(this function is also available via the
- MEAS
→
Frequency in Pulse →Freq in Burst →C menu).
Set corresponding masureent settings in the following menus:
-
SETTINGS → Pulsed RF

And finally select Manual acquisition with a center frequency that is
- SETTINGS
→
Misc
→
Input C Acq
→
Center frequency
- SETTINGS → Pulsed RF → Sensitivity
PRF
Select Pulse Repetition Frequency measurement via th e
- MEAS Pulsed RF Repetition PRF C.
Set corresponding measurement settings in the following menus:
-
SETTINGSPulsed RFSensitivity.
- SETTINGS Misc Input C Acq Center frequency
P
ULSE WIDTH POS
Select Positive Pulse Width measurement via the
- MEAS →Pulsed RF →Width →Pos →C.
Set corresponding measurement settings in the following menus:
-
SETTINGS →Pulsed RF →Sensitivity.
SETTINGS →Misc →Input C Acq →Center frequency
P
ULSE WIDTH NEG
Select Negative Pulse Width measurement via the
- MEAS
→
Pulsed RF
→
Width
→
Neg
→
C.
This measure corresponds to pulse off width, or the time between
pulses.
Set corresponding measurement settings in the following menus:
- SETTINGS Pulsed RF Sensitivity.
close to expected frequency (within 500 MHz)
-
SETTINGSMiscInput C AcqCenter frequency
DUTY
F
ACTO R POS
Select Positive duty factor measurement via the
- MEAS Pulsed RF Width Duty Factor Pos C.
Set corresponding measurement settings in the following menu s:
- SETTINGS Pulsed RF Sensitivity.
- SETTINGS
MiscInput C AcqCenter frequency
Positive Duty Factor corresponds to the pulse width divided by the
Pulse Repetition Interval.
DUTY
F
ACTO R NEG
Select Negative duty factor measurement via the
- MEAS Pulsed RF Width Duty Factor Neg C.
Set corresponding measurement settings in the following menu s:
- SETTINGS Pulsed RF Sensitivity.
- SETTINGS
MiscInput C AcqCenter frequency
The Negative Duty Factor corresponds to the negative pulse width
divided by the Pulse Repetition Interval.
4-29
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

The exceptions are Frequency and Period
This chapter explains how you can control
the start and stop of measurements and what
you can obtain by doing so. The chapter
starts by explaining the keys and the
functions behind them, then gives some
theory, and ends with actual measurement
examples.
This parameter is only applicable to the
functions
Frequency and Period Average.
Increasing the measurement time gives more
digits, i.e. higher resolution, but fewer meas
urements per second. T
he default value is
200 ms but can be changed via
SETTINGS
Meas Time
between 20 ns and 1000 s.
The default value gives 11 digits on the display and 4 to 5 measurem
ents each second.
Varying the measurement time is a
hardware-based averaging method in contrast
to the software-based mean value function
that can be found in the STAT/PLOT menu.
The measurement time changes in 1/2/5 steps
if you use the arrow keys for stepping. By
using the numeric entry keys you can set any
value within the specified range with a
resolution of 10 ns.
To quickly select the lowest measurement time, enter 0. The counter
will select 20 ns automatically.
Gate Indicator
The GATE LED is on when the counter is
busy counting input cycles.
Single Measurements
SINGLE is implicitly the normal measure-
ment mode, which means that the counter
shows the results from a single input cycle.
Single or Average is not relevant for V
max
,
Vmin or Vpp measurements.
Pressing HOLD completes the current
measurement and freezes the result on the
display.
Pressing
RESTART initiates a new
measurement.
If you are performing a statistics
measurement and press HOLD, the pending
sample will be finished. Then the
measurement will stop, and you can, for
instance, watch the graphic representation of
the samples taken so far.
Pressing RESTART starts a new
measurement from sample 1, and the
measurement will stop when the preset
number of samples has been taken.
Arming gives you the opportunity to start
and stop a measurement when an external
qualifier event occurs.
Start and stop of the arming function
can independently be set to positive
slope, negative slope, or it can be turned
off. A delay between 10 ns and 2 s can
be applied to the start arming channel to
facilitate certain measurements. The
resolution is 10 ns.
Input E on the rear panel is the normal
arming input, but also input A and input B
can be used. The frequency range for input E
is 80 MHz, whereas it is 160 MHz for the
other inputs.
All the versatile arming functions can
be reached under
SETTINGS Arm.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
5-2

Arming is somewhat complicated yet gives
the flexibility to perform a measurement on a
specific portion of a complex signal, like a
frequency measurement on the color burst
contained in a composite video signal.
Other examples of arming can be found later
in this chapter, starting on page 5-9.
Start arming acts like an External Trigger
on an oscilloscope. It allows the start of the
ac- tual measurement to be synchronized to
an external trigger event.
In a complex signal, you may want to
select a certain part to perform
measurements on. For this purpose, there is
an arming delay function, which delays the
actual start of measurement with respect to
the arming pulse, similar to a "delayed
timebase" in an oscilloscope.
You can choose to
delay start arming by a
preset time.
Start arming can be used for all functions except Frequency Burst, Ratio and Volt. If
you use start arming to arm an average measurement, it only con
trols the start of the first
sample.
Stop arming prevents the stop of a measurement until the counter detects a level shift on
the arming input. Combining Start and Stop
Arming results in an "external gate" function
which determines the duration of the
measurement.
Stop arming can be used for all functions except
Frequency Burst, Ratio, Volt and
Rise/Fall Time.
Stop Delay can only be used for realizing the
function Timed Totalize in the CNT-91(R).
5-3
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Process
Basic Free-running Measurements
Since these counters use the reciprocal counting technique, they a
lways synchronize the
start and stop of the actual measuring
period to the input signal trigger events. A
new mea- surement automatically starts when
the previ- ous measurement is finished
(unless
HOLD is on). This is ideal for
continuous wave signals.
The start of a measurement takes place
when the following conditions have been
met (in order):
The counter has fully processed the previ-
All preparations for a new measurement
are made.
The input signal triggers the counter's
measuring input.
The measurement ends when the input signal
meets the stop trigger conditions. That happens directly after the following events:
The set measurement time has expired (ap-
plies to Frequency and Period Average
measurements only).
The input signal fulfils the stop trigger
conditions, normally when it passes the
trigger window the second time.
Resolution as Function of
The quantization error and the number of digits on the display mainly define the resolution
of the counter, that is the least-significant digit
displayed.
As explained on page 4-10 under
Reciprocal Counting, the calculated
frequency f is:
while the relative rms quantization error Eq =
+100ps/tg.
The counter truncates irrelevant digits so that
the rms quantization resolution cannot change
the LSD (least-significant digit) more than 5
units. This occurs when the displayed value is
99999999, and the quantization error is worst
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
5-4

case. The best case is when the displayed
value is 10000000. Then the quantization resolution corresponds to 0.5 LSD units.
± 1 unit in 99999999 (=1E8) means 10
times more relative resolution than ± 1
unit in 10000000 (=1E7), despite the
same number of digits.
A gradual increase of the measurement time
reduces the instability in the LSD caused by the
quantization uncertainty. At a specific
measurement time setting, the counter is justified to display one more digit. That one additional digit suddenly gives ten times more display resolution, but not a ten times less
quantization uncertainty. Consequently, a
measurement time that gives just one more
display digit shows more visual uncertainty in
the last digit.
For a stable LSD readout, the maximum measurement time selected should be one that still
gives the required number of digits. Such optimization of the measurement time enables the
total resolution to be equal to the quantization
resolution.
Measurement Time and Rates
The set measurement time decides the length of
a measurement if Frequency or Period Average
is selected.
This is important to know when you want to
make fast measurements, for example when
you are using the statistics features, or when
you are collecting data over the GPIB bus.
The so-called "dead time", that is the time
between the stop of one measurement and
the start of the next one in the course of a
block measurement, can be below 2 µs.
A block is a collection of consecutive measurements, the results of which are stored in
local memory for statistics or plotting purposes (STAT/PLOT menu) or for later transfer to a controller over one of the data communication links (GPIB, USB or
ETHERNET).
Additional controls over start and stop of
measurements
Free-running measurements may be easy to
understand, but measurements can get more
complex.
Besides input signal triggering, the start of a
measurement is further controlled by the following elements:
— Manual RESTART, if HOLD is selected.
— GPIB triggering (<GET> or *TRG), if bus
triggering is selected.
—
External arming signal, if Start Arming is
selected.
—
Expired start arming delay, if Arming
Delay is selected.
In addition to expired measurement time and
stop signal triggering, the stop of measurement
is further controlled by:
— External arming signal triggering, if Stop
Arming is selected.
GPIB triggering is described in the Programmer's Handbook.
Now let's look deeper into the concept of
arming.
What is Arming?
Arming is a pretrigger condition ("qualifier")
that must be fulfilled before the counter allows
a measurement to start.
5-5
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

Arming can also be used to qualify the stop of
— A selected part of a complex waveform
a measurement. This is called "stop arming" as
opposed to the more common "start arming".
When you use arming, you disable the normal
free-run mode, i.e. individual measurements
must be preceded by a valid start arming signal
transition.
If you use start arming and stop arming tog
ether you get an exte
rnally controlled mea-
surement time, a s
o-called "External Gate".
The counters have a manual start arming function called
HOLD. Here you manually arm the
start of each individual measurement by
pressing the
RESTART key.
Use this manual arming mode to measure single-shot pheno
mena, which are either triggered
manually or occur at long intervals. Another
reason for using this manual arming could
simply be to allow sufficient time to write
down individual results.
■ When Do I Use Start Arming?
A synchronization signal starts the
measurement when start arming is
used.
Start arming is useful for measurements of fre-
quency in signals, such as the following:
Single-shot events or non-cyclic signals.
Pulse signals where pulse width or pulse
positions can vary.
Signals with frequency variations versus
signal.
Signal sources that generate complex wave
forms like pulsed RF, pulse bursts, TV line
signals, or sweep signals, usually also produce
a sync signal that coincides with the start of a
sweep, length of an RF burst, or the start of a
TV line. These sync signals can be used to arm
the counter. See Fig. 5-1.
When Do I Use Stop Arming?
You normally use stop arming together with
start arming. That means that the external
gating signal controls both the start and the
stop of the measurement. Such a gating signal
can be used to force the counter to measure the
frequency of a pulsed RF signal. Here the
position of the external gate must be inside a
burst. See Fig. 5-2.
Start and stop arming together is
used for burst signal gating.
Note that burst measurements with access to
an external sync signal are performed in the
normal Frequency mode, whereas burst
measurements without an external sync signal
are performed in the self-synchronizing
Frequency Burst mode.
In time interval measurements, you can
use the stop arming signal as a sort of
"external trigger Hold Off signal." Here you
block stop triggering during the external
period. See Fig. 5-3.
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017
5-5

Using arming as an external Hold
Off.
Input E is the normal arming input. It is
suitable for arming (sync) signals that have
TTL levels. The trigger level is fixed at
1.4V and cannot be changed. The trigger
slope can be set to positive or negative.
The Input E connector can be found on the
rear panel of the instrument.
Input A or Input B can also be used as
arming input for all single channel measurements and d
ual channel measurements
where the arming signal is one of the meas
uring signa
ls. This input is more suitable
if your arming signal does not have TTL
levels. All input controls such as AC/DC,
Trigger Level, 50/ 1 Metc. can be
used to condition the arming signal.
Using the measuring signal as arming
signal
When performing time or frequency measurements on complex signals having a unique
trigger point, input B arming can be used to
make the measuring signal itself "auto-arm"
the counter, e.g. to measure the frequency of a
signal after it has reached a specified voltage
limit (= set trigger level), see Fig. 5-4.
— Connect the signal to input A.
— Press
INPUT A and adjust the settings to
suit the interesting part of the signal.
— Press INPUT B and adjust the settings so
that the unique trigger point can be detected. Normally
DC coupling and Manual
trigger level should be preferred.
— Activate start arming with or without delay
on input B via the
SETTINGS menu.
The signal on input A will be internally connected to input B, so no ext
ernal signal tap is
necessary.
■ When Do I Use Arming With Delay?
You can delay the start arming point with respect to the arming signal. Use this function
when the external arming signal does not coincide with the part of the signal that you are
interested in.
The time delay range is 20 ns to 2 s with a setting resolution of 10 ns.
■ Getting The Whole Picture
The flowchart in Fig. 5-5 illustrates how arming a trigger hold off enables precise control of
the start and stop of the actual measurement
when you operate the counter from the front
panel. If you control the counter via the GPIB
or USB, read more about bus arming and triggering under the heading "How to use the trigger system" in the Programmer's Handbook.
Auto-arming using the trigger level
on B as qualifier.
5-5
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

The arming logic needs a setup time of about
5 nanoseconds before the counter is really
armed; see Fig. 5-6.
Time from active external control
edge until measurement is armed:
When arming delay is selected, the setup time
is different; see Fig. 5-7. It illustrates the effect of the 100 ns delay resolution.
Time from expired time delay until
measurement is armed:. -60 to
+40 ns.
Fig. 5-7 shows that a start trigger signal may
be detected although it appears 60 nanoseconds before the programmed time delay has
expired. The start trigger signal must come 40
nanoseconds after the programmed time
delay has expired to guarantee correct start of
the measurement.
Introduction to Arming
Examples
The following arming examples are available:
#1 Measuring the first pulse in a burst
#2 Measuring the second pulse in a burst
#3 Measuring the time between pulse #1 and #4
in a burst
#4 Profiling
Examples 1 and 2 measure the pulse width of a
selected positive pulse in a burst. You can,
however, also measure the period, rise time, or
duty factor by changing FUNCTION, and you
can measure on a negative pulse by changing
trigge
r slope.
If you do not know the basic parameters of the
signal to be measured, we recommend to use
an oscilloscope for monitoring. Then you can
estimate roughly how to set trigger slope,
arming slope and arming delay.
#1 Measuring the First Burst
Synchronizing the measurement
so that the pulse width of the first
pulse is measured.
In the first example we will measure the width
of pulse #1 in a repetitive pulse burst. In this
example, a synchronization signal (SYNC)
with TTL levels is also available. See Fig. 5-8.
5-9
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017

However, the quick and simple method
described first does not employ arming at all
but rather draws on the fact that a counter of
this type tends to self-synchronize its internal
processes to the input signal.
Our task is to synchronize the start of the
measurement (start trigger) to the leading
edge of the first pulse. Depending on the
signal timing, this can be easy, difficult, or
very difficult.
■ A. Auto Synchronization Without
Arming
If we are lucky, we can manage without using
the arming function at all. Often, the counter
can automatically synchronize the measurement start to the triggering of the first pulse.
The conditions for success are that the PRF is
not too high, preferably below 50 Hz and certainly not abo
ve 150 Hz. The duration of a
pulse burst (between first and last pulse)
should be substantially less than the distance
to the next burst, and the number of pulses in
the burst should be more tha
n 100 to avoid
occasional miscounts.
Do the following steps to perform auto syn-
chronization without arming:
Connect the burst signal to input A.
Adjust the manual sensitivity and trigger
level until the burst signal triggers the
counter correctly.
Use the MEAS/FUNC key to select Pulse
Width A.
Use Pacing Time to select a value that
approaches the time between the bursts.
Absolute synchronization will not be guaranteed in this way, but there is a high
probability that auto-synchronization will
work anyway. However, occasional
erroneous values will be displayed. To
achieve guaranteed synchronization, use the
■ B. Synchronization Using Start Arming
The SYNC signal can be directly used to arm
the measurement. This requires that the leading
edge of the SYNC signal occurs more than 5
nanoseconds before the leading edge of the
first pulse in the burst. See Fig. 5-9.
Synchronization using start arming.
Do the following steps to perform synchroni-
zation using start arming:
Connect the burst signal to input A.
Adjust the trigger level to match the burst
signal under study.
Select Start Arm Delay = 0 and Start Chan
E.
Use MEAS/FUNC to select Pulse Width A.
If there is no (or too little) time difference be-
tween the arming signal and the first pulse in
the pulse burst, arming must be combined with
a delay. See example C.
■ C. Synchronization Using Start Arming
With Time Delay
If the pulse bursts have a stable repetition frequency, you synchronize the measurement using Start Arming with Time Delay. Here you
use the SYNC pulse belonging to a preceding
burst to synchronize the start of measurement.
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Set the time delay to a time longer than the
duration of a pulse burst and shorter than the
repetition time of the pulse bursts.
See Fig. 5-10.
Synchronization using start arming
with time delay.
Use the same test setup as in the preceding ex-
ample but enter a suitable Start Arm Delay.
#2 Measuring the Second Burst
Pulse
The next task is to measure the width of the
second pulse in the pulse train from example 1.
How can we now synchronize the measurement start to the start of the second pulse? In
this case auto-synchronization, without the use
of the arming function, cannot work.
Auto-synchronization can be used only to synchronize on the fir
st trigger event in a burst.
Depending on the SYNC signal's position relative to the burst, and the duration of the
SYNC signal, the measurement can be performed with or wit
hout using arming delay.
If the trailing edge of the SYNC signal occurs
after the leading edge of the first pulse but before the second pu
lse in the pulse burst, then
normal start arming without delay can be used.
Select triggering on positive slope on input A
and negative slope on input E. The slope for
the active arming channel is set in the
SETTINGS Arm Start Slope menu. This
example is shown in the following figure:
If the SYNC-pulse timing is not so suitable as
in the above measurement example, then
Fig. 5-11 If the trailing edge of the sync signal
appears before the second pulse
use arming without delay.
arming must be used combined with a time
delay; see the following figure:
Use arming with delay if the
trailing edge of the sync signal
appears too late to be useful.
Use the same test setup as in the preceding ex-
ample but enter a suitable Start Arm Delay.
The set delay time must be set to expire in the
gap between pulse #1 and #2.
5-11
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#3 Measuring the Time Between
Burst Pulse #1 and #4
In the previous examples, the synchronization
task has been to identify the start of a measurement and to perform a single-shot time interval measurem
ent. Now, we will complicate
the picture even more. In our next example we
will not only arm the start, but also the stop of
a measurement. We will measure the time bet
ween the first and t
he fourth pulse in the
pulse burst. We still have the SYNC signal
available, see Fig. 5-13.
Measuring a time interval inside a
burst.
The measurement function is not Pulse Width
Abut
Time Interval A to A where the settings
for input B are used for controlling the stop
conditions. The desired start and stop trigger
points are marked in the preceding illustration. Our task is now to arm both the
start and the stop of this measurement. The
start arming is already described in example
#1, i.e., synchronize measurement start to the
leading edge of the first pulse. The challenge
is to synchronize the stop of the measurement,
i.e., to arm the stop. If we do nothing, the time
interval measured will be the time between
the first and the second pulse. We must thus
delay the stop. This can be done in different
ways.
■ A. Using Trigger Hold Off to Delay the
Stop a Certain Time
Trigger Hold Off is used to inhibit stop triggering during a preset time. The Hold Off
period starts synchronously with the start
trigger event. The Hold Off time should be set
to expire somewhere between pulse number 3
and 4, see Fig. 5-14.
If Hold Off expires between pulses
three and four, the correct time interval is
measured.
Use the same test setup as in the preceding
examples. Then proceed as follows:
Use the MEAS/FUNC key to select
Press INPUT B and choose positive slope
and a suitable trigger level.
Press SETTINGS Trigger Hold Off (On)
and enter a suitable Hold Off time.
Make sure the start arming conditions from
example #1 are maintained, i.e. no arming
delay.
■ B. Using Stop Arming (i.e., External Hold
So far in our examples, the sync signal has been
used exclusively as a start arming signal; i.e.,
we have been concerned only about the leading
edge of the sync signal, and not its duration.
However, the sync signal can also be used as an
External Trigger Hold Off when you select stop
arming on the trailing edge of the sync signal.
If the duration of the sync pulses can be
externally varied, we can select a duration that
expires in the gap between pulse #3 and #4.
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Using both start and stop
arming to select the part of the
burst that is of interest.
Use the same test setup as in the preceding ex-
ample. Then proceed as follows:
— Press
SETTINGS Arm and select Stop
Chan E
and negative Stop Slope.
— Measure.
Profiling means measuring frequency versus
time. Examples are measuring warm-up drift
in signal sources over hours, measuring the
linearity of a frequency sweep during seconds,
VCO switching characteristics during milli-
seconds, or the frequency changes inside a
"chirp radar" pulse during microseconds.
These counters can handle many profiling
measurement situations with some limitations.
Profiling can theoretically be done manually,
i.e., by reading individual measurement re-
sults and plotting in a graph. However, to
avoid getting bored long before reaching your
800th or so measurement result, you must use
some computing power and a bus interface. In
profiling applications, the counter acts as a
fast, high-resolution sampling front end, stor-
ing results in its internal memory. These re-
sults are later transferred to the controller for
analysis and graphical presentation. The
TimeView™ software package greatly simpli-
You must distinguish between two different
types of measurements called free-running and
■ Free-Running Measurements
Free-running measurements are performed over
a longer period, e.g., to measure the sta-bility
over 24 hours of oscillators, to measure initial
drift of a generator during a 30-minute warm-up
time, or to measure short-term sta-bility during 1
or 10s. In these cases, measure-ments are
performed at user-selected intervals in the range
2 µs to 1000 s. There are several different ways
of performing the measurements at regular
intervals.
Measurements using the statistics features
for setting the "pacing time"
By setting the pacing time to 10 s for example,
measurements are automatically made at 10 s
intervals until the set number of samples has
been taken. The range is 2 - 2*109 .Use
HOLD/RUN and RESTART if you want to stop
after one full cycle. You can watch the trend or
spread on the graphic display while the
measurement is proceeding.
Using a controller as a "pacer"
As an alternative, the timer in the controller can
be used for pacing the individual measure-ments.
This allows for synchronization with external
events, for instance a change of DUT when
checking a series of components.
Using external arming signals
External arming signals can also be used for
"pacing." For example with an arming signal
consisting of 10 Hz pulses, individual measurements are armed at 100 ms intervals.
Letting the counter run free
When the counter is free-running, the shortest
delay between measurements is approximately 4
µs (internal calibration OFF) or 8 µs (internal
calibration ON) plus set measurement time. For
example, with a measurement time of 0.1 ms,
5-13
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the time between each sample is ap-
■ Repetitive Sampling Profiling
The measurement setup just described will not
work when the profiling demands less than 4
s intervals between samples.
How to do a VCO step response profiling
with 100 samples during a time of 10 ms.
This measurement scenario requires a repeti-
tive input step signal, and you have to repeat
your measurement 100 times, taking one new
sample per cycle. And every new sample
should be delayed 100s with respect to the
previous one.
The easiest way to do this is by means of
a controller, e.g. a PC, although it is
possible but tedious to manually set and
perform all 100 measurements.
The following are required to setup a meas
urement:
A repetitive input signal (e.g., frequency
An external SYNC signal (e.g., step voltag
e input to VCO).
Use of arming delayed by a preset time
(e.g., 100, 200, 300s
).
See Fig. 5-16 and Fig. 5-17.
When all 100 measurements have been made,
the results can be used to plot frequency versus time. Note that the a
bsolute accuracy of
the time scale is dependent on the input signal
itself. Although the measurements are armed
at 100 s 100 ns intervals, the actual start of
measurement is always synchronized to the
first input signal trigger event after arming.
The TimeView™ software package will do
this measurement quickly and easily.
Setup for transient profiling of a
VCO.
Results from a transient profiling
measurement.
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5-13

Introduction
Three different ways to process a measuring
result are available: Averaging, Mathematics
and Statistics. They can be used separately or
all together.
In addition to postprocessing you can also
monitor the measurement results in real time
by setting limits and deciding how to react
when they are crossed.
Averaging
Hardware averaging by means of counting
clock pulses during several full input signal
cycles is only used for the measurement functions Frequency and Period Average. The
parameter to be set by the operator in this case
is Meas Time under SETTINGS, and the range
is 20 ns to 1000 s. Longer measuring times
mean higher resolution.
The other functions employ single cycle measuring, and the method to get average results
is to utilize the statistics features described
later.
Mathematics
The counter can use five
mathematical expressions to process the
measurement
result before it is displayed:
1. K*X+L
2. K/X+L
3. (K*X+L)/M
4. (K/X+L)/M
5. X/M-1
Press MATH/LIM Math to enter the first
mathematics submenu. See page 2-14 how to
enter the constants K, L and M and how to
select the formula that best suits your need.
The default values of K, L and M are chosen
so that the measurement result is not affected
directly after activating
Math. Recalling the
default setting will restore these values as
well.
If you want to observe the deviation from a
certain initial frequency instead of the absolute frequenc
y itself, you can do like this:
Recall the default settings by pressing
USER OPT Save/Recall Recall
Setup Default.
Connect the signal to be measured to
Press AUTO SET to let the counter find
the optimum trigger conditions on its
If the current display value is suitable
for your purpose, then press X
0
. It will
then be transferred to the constant L.
You can repeat pressing
X
0
until you are
satisfied. The constant will be updated
with the latest measurement result.
Instead of using X0you can enter any numerical value from the front panel. Let's
assume that 10 MHz is your reference
frequency. The mantissa is marked by
text inversion for immediate editing.
Press
1 0 ± EE 6.
Confirm by pressing EXIT/OK. Now the
constant L is updated and displayed as
Press Math and choose the expression
K*X+L by pressing the softkey below it.
Now the display will show the deviation
from the value you have just entered.
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By changing the constant K you can scale the
result instead.
Use the expression X/M-1 if you want the result to be displayed as a relative deviation.
Statistics
Statistics can be applied to all
measuring functions and can also be applied
to the result from Mathematics.
The available statistics functions are as follows:
X MAX: Displays the maximum value within a
sa
mpled population of N x
i
-values.
X MIN: Displays the minimum value within a
sampled population of N xi-values.
XP-P: Displays the peak-to-peak deviation
within a sampled population of N
x
i
values.
MEAN: Displays the arithmetic mean value
(x
of a sampled population of N x
i
values and is calculated as:
ST DEV: Displays the standard deviation (s) o
a sampled population of N xi-values
and is calculated as:
It is defined as the square root of the
variance.
A DEV: Displays the Allan deviation (σ) of a
sampled population of N xi-values and
is calculated as:
It is defined as the square root of the
Allan variance.
The number N in the expressions above can
assume any value between 2 and 2*109.
Allan Deviation vs. Standard
Deviation
The Allan Deviation is a statistic used for
characterizing short-term instability (e.g.
caused by jitter and flutter) by means of samples (measure
ments) taken at short intervals.
The fundamental idea is to eliminate the
influence of long-term drift due to aging,
temperature or wander. This is done by
making consecutive comparisons of adjacent
samples.
The Standard Deviation, which is probably a
more familiar statistic, considers the effects
of all types of deviation, as all samples in the
population are compared with the total mean
value.
As you can
see, both the Allan Deviation and
the Standard Deviation are expressed in the
same units as the main parameter, e.g. Hz or
s.
Press No. of samples and enter a new
value by means of the numerical keys or
the
UP/DOWN arrow keys, if you want to
change the default value of 100.
Proceed in the same way for No. of bins
if you want to present the measurement
results graphically in a histogram.
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Note that the six statistic measures are
calculated and displayed
simultaneously only in the non-graphic
presentation mode under STAT/PLOT.
Use the same key for toggling
between the three modes Numerical -
Histogram - Trend.
Press Pacing time and enter a new value
if you want to change the default value 20
ms. The range is 2s - 500 s. The pacing
parameter sets the sampling interval.
Activate the set pacing time by pressing
Pacing Off. The status is changed to
Pacing On. Status Pacing Off means that
the set number of samples will be taken
with minimum delay.
Press HOLD/RUN to stop the measuring
Press RESTART to initiate one data cap-
Toggle STAT/PLOT to view the measurement result as it is displayed in the different presentation modes.
Note that you can watch the intermediate results update the display
continually until the complete data
capture is ready.
This is particularly valuable if the
collection of data is lengthy.
When using statistics, you must take care that
the measurements do not take too long time to
perform. Statistics based on 1000 samples
does not give a complete measurement result
until all 1000 measurements have been made,
although it is true that intermediate results are
displayed in the course of the data capture.
Thus it can take quite some time if the setting
of the counter is not optimal.
Here are a few tips to speed up the
Do not use a longer measuring time than
necessary for the required resolution.
Remember to use a short pacing time, if
your application does not require data
collection over a long period of time.
If AUTO trigger is ON, the counter
makes an "AUTO Once" and uses
the found trigger level as fixed
settings until all samples are
captured. Thus the use of auto
trigger does not reduce capture
speed.
Determining Long or Short
Time Instability
When making statistical measurements, you
must select measuring time in accordance
with what you want to obtain: Jitter or very
short time (cycle to cycle) variations require
that the samples be taken as Single
measurements.
If average is used (Freq or Period Average
only), the samples used for the statistical calculations ar
e already averaged, unless the set
measuring time is less than the period time of
the input signal (up to 160 MHz). Above this
frequency prescaling by two is introduced
anyhow, and as a consequence a certain
amount of averaging. This can be a great ad-
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vantage when you measure medium or long
time instabilities. Here averaging works as a
smoothing function, eliminating the effect of
jitter.
The signal in Fig. 6-1 contains a slower variation as well as jitter. When measuring jitter
you should use a limited number of samples,
so that the slow variation does not become
noticeable or alternatively use the dedicated
statistic measure for this kind of
measurement, the Allan deviation.
To measure the slower variation you calculate
Max, Min or Mean on a long series of averaged samples. Here averaging eliminates the
jitter in each sample and the long measuring
time and large number of samples means that
the measurement can record very slow variations. The maximum pacing time is 500 s, the
maximum measuring time for each sample is
1000 s, and the maximum number of samples
is 2*109, which in effect means that a single
data capture could theoretically span up to
3*1012s, or more than 95000 years.
Statistics and Mathematics
The counter allows you to perform mathematical operations on the measured value before
it is presented to the display or to the bus. See
Page 6-2 to get an overview of the four available equations.
Any systematic measurement uncertainty can
be measured for a particular measurement
setup, and the needed correction constants can
be entered into these equations. Statistics will
then be applied to the corrected measured
value.
The standard deviation can be used to calculate the confidence limits of a measurement.
Where:
s
x = standard deviation
k = 1 for a confidence level of 68.3% (1-
k = 2 for a confidence level of 95.5% (2
k = 3 for a confidence level of 99.7% (3
A measurement of a time interval of 100 s is
used to illustrate how the confidence limits
are calculated from the measurement result.
Use the statistics to determine the mean value
and standard deviation of the time interval.
Take sufficient samples to get a stable
reading. Assume further that the start and stop
trigger transitions are fast and do not
contribute to the measurement uncertainties.
MEAN value = 100.020 s and a STD DEV
= 50 ns, then the 95.5% confidence limits =
±2sx = ±2 * 50 ns = ±100 ns.
The 3- limit will then be ±3 * 50 ns =
±150 ns
Statistics provides an easy method of determining the short term timing instability, (jitter) of pulse parameters. The jitter is usually
specified with its rms value, which is equal to
the standard deviation based on single meas
urements. T
he counter can then directly
measure and display the rms jitter.
Otherwise, the standard deviation of mean
values can be measured. The rms value is a
good measure to quantify the jitter, but it
gives no information about the distribution of
the measurement values.
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To improve a design, it might be necessary to
analyze the distribution. Such measurements as
well as trend analysis can be performed by
means of the built in graphic capability - toggle the
STAT/PLOT key to see the two graphic
presentation modes.
Even higher versatility can be exploited with a
controller and the optional TimeView™
Frequency and Time Analyzing Software
Package.
The Limits Mode makes the counter an efficient alarm condition monitor with high flexibility as to the report possibilities.
Press MATH/LIM
Limits to enter the first
You can set two levels by entering the
submenus named Lower Limit resp. Upper
Limit. Any numerical value can be entered using scientific notation. The active keys are the
digits 0-9, the decimal point, the change sign
(±) and the softkey designated EE for toggling
between the mantissa and the exponent.
Typos are erased by pressing the left arrow
key. Confirm by pressing ENTER.
Press Limit Behavior to set how the counter
will react on limit crossings. The following
choices exist:
• Off
No action taken. LIM indicator is OFF. In all
other behavior modes, the LIM indicator is
ON
and
non-flashing, unless the limits set in
the Limit Mode menu have been crossed.
• Capture
The measurements are compared with the
limits set under Lower Limit and Upper
Limit, and the LIM symbol will be flashing
when the active Limit Mode has set the
LIM flag.
Only samples meeting the test criterion will
be part of the population in
statistics presentations.
• Alarm
The measurements are compared with the
limits set under Lower Limit and Upper
Limit, and the LIM symbol will be flashing
when the active Limit Mode has set the
LIM flag.
All samples, i.e. also those outside the limits,
will be part of the population in statistics
presentations.
• Alarm_stop
The measurements are compared with the
limits set under Lower Limit and Upper
Limit, and the LIM symbol will be flashing
when the active Limit Mode has set the
LIM flag.
The measurement process will stop, and
the value that caused the limit detector to
trigge can be read on the display.
Only samples taken before the alarm condition
will be part of the population in statistics
presentations.
The alarm conditions can also be detected via
the SRQ function on the GPIB. See the Programmer's Handbook.
The Limit Mode offers three choices:
USER MANUAL ● CNT 9x Series ● Rev.20 December 2017