6 Care of the product ................................................................................................................................ 4
4 Group delay .............................................................................................................................. 46
5 Time domain measurements .................................................................................................. 46
6 Reverse measurements on two port devices ......................................................................... 50
7 Powering active devices using the built-in bias-Ts ................................................................ 51
4 Reference plane extension and de-embedding .................................................................................. 51
5 Saving data ........................................................................................................................................... 54
6 Loading data ......................................................................................................................................... 54
To prevent possible electrical shock, fire, personal injury, or damage to the product, carefully read this safety
information before attempting to install or use the product. In addition, follow all generally accepted safety
practices and procedures for working with and near electricity.
This instrument has been designed to meet the requirements of EN61010-1 (Safety Requirements for
Electrical Equipment for Measurement, Control and Laboratory Use) and is intended only for indoor use in a
Pollution Degree 1 environment (no pollution, or only dry non-conductive pollution) in the temperature range
15 °C to 35 °C, 20 % to 80 % relative humidity (non-condensing).
The following safety descriptions are found throughout this guide:
A WARNING identifies conditions or practices that could result in injury or death.
A CAUTION identifies conditions or practices that could result in damage to the product or equipment to
which it is connected.
WARNING
To prevent injury or death use the product only as instructed and use only the power supply
provided. Protection provided by the product may be impaired if used in a manner not specified
by the manufacturer.
1.1Symbols
These safety and electrical symbols may appear on the product or in this guide.
SymbolDescription
Earth (ground) terminal
This terminal can be used to make a measurement ground
connection. It is not a safety or protective earth.
Chassis terminal
Possibility of electric shock
CAUTION
Appearance on the product indicates a need to read these
safety instructions.
Do not dispose of this product as unsorted municipal waste.
1.2Maximum input/output ranges
WARNING
To prevent electric shock, do not attempt to measure or apply signal levels outside the
specified maxima below.
The table below indicates the maximum voltage of the outputs and the overvoltage protection range for
each input on the VNA. The overvoltage protection ranges are the maximum voltages that can be applied
without damaging the instrument.
ConnectorMaximum operating voltage
(output or input)
Ports 1 and 2+10 dBm (about 710 mV RMS)+20 dBm (about 2.2 V RMS)
Bias tees 1 and 2±15 V DC250 mA
Trigger and reference in±6 V pk
Trigger and reference out0 V to +5 VDo not apply a voltage
WARNING
Signals exceeding the voltage limits in the table below are defined as "hazardous live" by EN
61010.
Signal voltage limits of EN61010
± 70 V DC33 V AC RMS± 46.7 V pk max.
WARNING
To avoid equipment damage and possible injury, do not operate the instrument outside its rated
supply voltages or environmental range.
CAUTION
Exceeding the overvoltage protection range on any connector can cause permanent damage to
the instrument and other connected equipment.
Overvoltage or overcurrent
protection
CAUTION
To prevent permanent damage, do not apply an input voltage to the trigger or reference output
of the VNA.
1.3Grounding
WARNING
The instrument's ground connection through the USB cable is for functional purposes only. The
instrument does not have a protective safety ground.
WARNING
To prevent injury or death, never connect the ground of an input or output (chassis) to any
electrical power source. To prevent personal injury or death, use a voltmeter to check that there
is no significant AC or DC voltage between the instrument's ground and the point to which you
intend to connect it.
CAUTION
Applying a voltage to the ground input is likely to cause permanent damage to the instrument,
the attached computer, and other equipment.
CAUTION
To prevent measurement degradation caused by poor grounding, always use the high-quality
USB cable supplied with the instrument.
To prevent injury or death, only use the adaptor supplied with the product. This is approved for
the voltage and plug configuration in your country.
Power supply options and ratings
Ext DC power supply
Model nameUSB connection
VoltageCurrentTotal power
USB 2.0.
PicoVNA 106
WARNING
Containment of radio frequencies
The instrument contains a swept or CW radio frequency signal source (300 kHz to 6.02 GHz at
+6 dBm max.) The instrument and supplied accessories are designed to contain and not radiate
(or be susceptible to) radio frequencies that could interfere with the operation of other
equipment or radio control and communications. To prevent injury or death, connect only to
appropriately specified connectors, cables, accessories and test devices, and do not connect to
an antenna except within approved test facilities or under otherwise controlled conditions.
Compatible with
USB3.0.
12 to 15 V DC1.85 A pk22 W
1.5Environment
WARNING
To prevent injury or death, do not use the VNA in wet or damp conditions, or near explosive gas
or vapor.
CAUTION
To prevent damage, always use and store your VNA in appropriate environments.
StorageOperating
Temperature–20 °C to +50 °C+15 °C to +35 °C
HumidityUp to 80% RH (non-condensing)Up to 80% RH (non-condensing)
Altitude2000 m
Pollution degree2
CAUTION
Do not block the air vents at the back or underside of the instrument as overheating will
damage.
Do not insert any objects through the air vents as internal interference will cause damage.
The product and accessories contain no user-serviceable parts. Repair, servicing and calibration require
specialized test equipment and must only be performed by Pico Technology or an approved service provider.
There may be a charge for these services unless covered by the Pico warranty.
WARNING
To prevent injury or death, do not use the product if it appears to be damaged in any way, and
stop use immediately if you are concerned by any abnormal behavior.
CAUTION
To prevent damage to the device or connected equipment, do not tamper with or disassemble
the instrument, case parts, connectors, or accessories.
When cleaning the product, use a soft cloth dampened with a solution of mild soap or detergent
in water. Do not allow liquids to enter the instrument's casing.
WARNING
To avoid equipment damage, do not block the ventilation ports on the instrument.
CAUTION
Take care to avoid mechanical stress or tight bend radii for all connected leads, including all
coaxial leads and connectors. Mishandling will cause deformation of sidewalls, and will
degrade performance. In particular, note that test port leads should not be formed to tighter
than 5 cm (2") bend radius.
To prevent measurement errors and extend the useful life of test leads and accessory
connectors, ensure that liquid and particulate contaminants cannot enter. Always fit the dust
caps provided and use the correct torque when tightening. Pico recommends: 1 Nm (8.85 inch
lb) for supplied and all stainless steel connectors, or 0.452 Nm (4.0 inch-lb) when a brass or
gold-plated connector is interfaced.
Obtain the PicoVNA 2 software installer from the disk supplied or from www.picotech.com/downloads.
Run the installer (right-click and Run as administrator) and ensure that the installation was successful.
Connect the PicoVNA 106 unit to the computer and wait while Windows automatically installs the driver.
In case of difficulties, refer to Software installation
for more details.
2.2Loading the calibration kit(s)
If the device to be tested is ‘insertable’ (one female and one male connector), two kits are required.
Otherwise a single kit is required. See diagrams below:
Run the PicoVNA 2 software
In the main menu, select Tools > Calibration kit
Click Load P1 kit, select the data for your Port 1 kit and then click Apply
Click Load P2 kit, select the data for your Port 2 kit and then click Apply
Select the calibration kit(s) required depending on the device to be tested.
Note: if testing a non-insertable DUT with, for example, female connectors, use a single female kit for ports 1
and 2.
The bandwidth setting used during calibration largely determines the available dynamic range during the
measurement. The table below shows suggested bandwidth and power settings to use during calibration for
different types of measurement.
MeasurementCalibration
bandwidth
Fastest speed10 kHzNone+0 dBmSet bandwidth to 140 kHz during measurement
Best accuracy and
~100dB dynamic range
General use, fast speed,
~90dB dynamic range
Best dynamic range10 HzNone+6 dBmLeave bandwidth unchanged during measurement.
100 HzNone–3 dBmSet bandwidth to 100 Hz during measurement
1 kHzNone+0 dBmSet bandwidth to 1 kHz during measurement
Calibration
averaging
Calibration
power
Comments
Refer to “Calibration for best dynamic range –
minimizing the effect of crosstalk”.
2.6Running in demo mode
Demo mode allows you to explore the user interface software without the need to have an instrument
running.
To enter demo mode, run the PicoVNA 2 software with no instrument connected.
Click Go to demo in the dialog that appears.
PicoVNA 2 will then offer you a selection of demonstration measurements.
The PicoVNA 106 is a PC-driven vector network analyzer capable of operation over the range of 300 kHz to 6
GHz. It can perform direct measurements of forward and reverse parameters with up to 118 dB of dynamic
range. The test frequency can be set with a resolution of 10 Hz or less. A simplified block diagram of the
instrument is shown below:
Simplified block diagram of the PicoVNA 106
The architecture is based on a four-receiver ("Quad RX") arrangement using a bandwidth of up to 140 kHz.
Couplers 1 and 2 are wideband RF bridge components which provide the necessary directivity in both
directions. Signal detection is by means of analog-to-digital converters used to sample the IF signal. The
sample data is processed by the embedded controller to yield the I and Q components. The detection
system operates with an IF of 1.3 MHz and employs a patented circuit technique to yield fast speeds with
very low trace noise.
The instrument's software runs on a personal computer and communication with the instrument is through
the USB interface. The software carries out the mathematical processing and allows the display of
measured parameters in many forms, including:
frequency domain
time domain
de-embedding utility
measuring output power at the 1 dB gain compression point
measuring AM to PM conversion
A vector network analyzer is used to measure the performance of circuits or networks such as amplifiers,
filters, attenuators, cables and antennas. It does this by applying a test signal to the network to be tested,
measuring the reflected and transmitted signals and comparing them to the test signal. The vector network
analyzer measures both the magnitude and phase of these signals.
4.2Structure of the VNA
The VNA consists of a tunable RF source, the output of which is split into two paths. The signal feeds to the
couplers are each measured by their respective reference receivers through power dividers. In the forward
mode, the test signal is passed through a directional coupler or directional bridge before being applied to the
DUT. The directional output of the coupler, which selects only signals reflected from the input of the DUT, is
connected to the Port1 receiver where the signal’s magnitude and phase are measured. The rest of the
signal, the portion that is not reflected from the input, passes through the DUT to the Port2 receiver where its
magnitude and phase are measured. The measurements at the Port1 and Port2 receivers are referenced to
the measurements made by the Ref1 and Ref2 receivers so that any variations due to the source are
removed. The Ref1 and Ref2 receivers also provide a reference for the measurement of phase.
Simplified vector network analyzer block diagram
In reverse mode, the test signal is applied to the output of the DUT, and the Port2 receiver is used to
measure the reflection from the output port of the DUT while the Port1 receiver measures the reverse
transmission through the DUT.
Vector network analyzers have the capability to measure phase as well as magnitude. This is important for
fully characterizing a device or network either for verifying performance or for generating models for design
and simulation. Knowledge of the phase of the reflection coefficient is particularly important for matching
systems for maximum power transfer. For complex impedances the maximum power is transferred when
the load impedance is the complex conjugate of the source impedance (see figure).
Matching a load for maximum power transfer
Measurement of phase in resonators and other components is important in designing oscillators. In
feedback oscillators, oscillation occurs when the phase shift round the loop is a multiple of 360° and the
gain is unity. It is important that these loop conditions are met as close as possible to the center frequency
of the resonant element to ensure stable oscillation and good phase noise performance.
The ability to measure phase is also important for determining phase distortion in a network. Phase
distortion can be important in both analog and digital systems. In digital transmission systems, where the
constellation depends on both amplitude and phase, any distortion of phase can have serious effects on the
errors detected.
4.4S-parameters
The basic measurements made by the vector network analyzer are S (scattering) parameters. Other
parameters such as H, Y and Z parameters may all be deduced from the S-parameters if required. The
reason for measuring S-parameters is that they are made under conditions that are easy to produce at RF.
Other parameters require the measurement of currents and voltages, which is difficult at high frequencies.
They may also require open circuits or short circuits that can be difficult to achieve at high frequencies, and
may also be damaging to the device under test or may cause oscillation.
Forward S-parameters are determined by measuring the magnitude and phase of the incident, reflected and
transmitted signals with the output terminated with a load that is equal to the characteristic impedance of
the test system (see figure below).
The measured parameters are presented in a file similar to the one below. The format is as follows:
Header lines: these start with a ! symbol and give general information such as time and date.
Format line: this starts with a # symbol and gives information about the format of the data.
o First field gives the frequency units, in this case MHz
o Second field indicates the parameters measured, in this case S-parameters
o Third field indicates the format of the measurement, in this case MA meaning magnitude and angle.
Others formats are RI, meaning real and imaginary, and DB, meaning log magnitude and angle.
Data lines. The number of columns of data depends on the parameters that have been measured.
o A 1-port measurement measures the reflected signal from the device under test and usually produces
three columns. If the format is MA (magnitude and angle), the first column is the measurement
frequency, the second is the magnitude of S
second column is the real part of S
and the third column is the imaginary part of S11.
11
and the third is the angle of S11. If the format is RI, the
11
o When a reflection and transmission measurement is made there are five columns of data. Column 1
is the measurement frequency, columns 2 and 3 contain S
imaginary data, and columns 4 and 5 contain S
magnitude and angle or real and imaginary data.
21
magnitude and angle or real and
11
o If a full 2-port measurement is made, there will be nine columns of data. Column 1 contains frequency
information, columns 2 and 3 S
data, 4 and 5 S21 data, 6 and 7 S12 data, and 8 and 9 S22 data.
The PicoVNA 106 can generate full set of 2-port parameters but you can choose to export either 1-port .s1p
or full 2-port .s2p S-parameter files to suit most RF and microwave circuit simulators.
Part of a typical 2-port S-parameter file is shown below. The header shows that the frequency units are MHz,
the data format is Magnitude and Angle and the system impedance is 50 Ω. Column 1 shows frequency, 2
and 3 S
! 06/09/2005 15:47:34
! Ref Plane: 0.000 mm
# MHZ S MA R 50
!
3 0.00776 16.96 0.99337 -3.56 0.99324 -3.53 0.00768 12.97
Input and output parameters, S11 and S22, are often displayed on a polar plot or a Smith chart. The polar plot
shows the result in terms of the complex reflection coefficient, but impedance cannot be directly read off
the chart. The Smith chart maps the complex impedance plane onto a polar plot. All values of reactance and
all positive values of resistance, from 0 to ∞, fall within the outer circle. This has the advantage that
impedance values can be read directly from the chart.
The Smith chart
4.6Calibration and error correction
Before accurate measurements can be made, the network analyzer needs to be calibrated. In the calibration
process, well-defined standards are measured and the results of these measurements are used to correct
for imperfections in the hardware. The most common calibration method, SOLT (short, open, load, through),
uses four known standards: a short circuit, an open circuit, a load matched to the system impedance, and a
through line. These standards are usually contained in a calibration kit and their characteristics are stored
on the controlling PC in a Cal Kit definition file. Analyzers such as the PicoVNA 106 that have a full Sparameter test set can measure and correct all 12 systematic error terms.
Another six sources exist in the reverse measurement
not shown).
4.7Other measurements
S-parameters are the fundamental measurement performed by the network analyzer, but many other
parameters may be derived from these including H, Y and Z parameters.
4.7.1Reflection parameters
The input reflection coefficient Γ can be obtained directly from S11:
ρ is the magnitude of the reflection coefficient i.e. the magnitude of S
ρ = |S11|
Sometimes ρ is expressed in logarithmic terms as return loss:
return loss = –20 log(ρ)
VSWR can also be derived:
VSWR definition
11:
4.7.2Transmission parameters
Transmission coefficient T is defined as the transmitted voltage divided by the incident voltage. This is the
same as S
If T is less than 1, there is loss in the DUT, which is usually referred to as insertion loss and expressed in
decibels. A negative sign is included in the equation so that the insertion loss is quoted as a positive value:
If T is greater than 1, the DUT has gain, which is also normally expressed in decibels:
4.7.3Phase
The phase behavior of networks can be very important, especially in digital transmission systems. The raw
phase measurement is not always easy to interpret as it has a linear phase increment superimposed on it
due to the electrical length of the DUT. Using the reference plane function the electrical length of the DUT
can be removed leaving the residual phase characteristics of the device.
Operation on phase data to yield underlying characteristics
4.7.4Group delay
Another useful measurement of phase is group delay. Group delay is a measure of the time it takes a signal
to pass through a network versus frequency. It is calculated by differentiating the phase response of the
device with respect to frequency, i.e. the rate of change of phase with frequency:
The linear portion of phase is converted to a constant value typically, though not always, representing the
average time for a signal to transit the device. Differences from the constant value represent deviations from
linear phase. Variations in group delay will cause phase distortion as a signal passes through the circuit.
When measuring group delay the aperture must be specified. Aperture is the frequency step size used in the
differentiation. A small aperture will give more resolution but the displayed trace will be noisy. A larger
aperture effectively averages the noise but reduces the resolution.
The 1 dB gain compression point of amplifiers and other active devices can be measured using the power
sweep. The small signal gain of the amplifier is determined at low input power, then the power is increased
and the point at which the gain has fallen by 1 dB is noted.
The 1 dB gain compression is often used to quote output power capability
4.7.6AM to PM conversion
Another parameter that can be measured with the VNA is AM to PM conversion. This is a form of signal
distortion where fluctuations in the amplitude of a signal produce corresponding fluctuations in the phase of
the signal. This type of distortion can have serious effects in digital modulation schemes where both
amplitude and phase accuracy are important. Errors in either phase or amplitude cause errors in the
constellation diagram.
4.7.7Time domain reflectometry (TDR)
Time domain reflectometry is a useful technique for measuring the impedance of transmission lines and for
determining the position of any discontinuities due to connectors or damage. The network analyzer can
determine the time domain response to a step input from a broad band frequency sweep at harmonically
related frequencies. An inverse Fourier Transform is performed on the reflected frequency data (S
the impulse response in the time domain. The impulse response is then integrated to give the step
response. Reflected components of the step excitation show the type of discontinuity and the distance from
the calibration plane.
A similar technique is used to derive a TDT (Time Domain Transmission) signal from the transmitted signal
data (S
provides a more detailed treatment of TDR and TDT.
). This can be used to measure the rise time of amplifiers, filters and other networks. The following
The traditional TDR consists of a step source and sampling oscilloscope (see figure below). A step signal is
generated and applied to a load. Depending on the value of the load, some of the signal may be reflected
back to the source. The signals are measured in the time domain by the sampling scope. By measuring the
ratio of the input voltage to the reflected voltage, the impedance of the load can be determined. Also, by
observing the position in time when the reflections arrive, it is possible to determine the distance to
impedance discontinuities.
Traditional TDR setup
4.7.7.1.1Example: shorted 50 ohm transmission line
Simplified representation of the response of a shorted line.
For a transmission line with a short circuit (figure above) the incident signal sees the characteristic
impedance of the line so the scope measures Ei. The incident signal travels along the line to the short circuit
where it is reflected back 180° out of phase. This reflected wave travels back along the line canceling out the
incident wave until it is terminated by the impedance of the source. When the reflected signal reaches the
scope the signal measured by the scope goes to zero as the incident wave has been canceled by the
reflection. The result measured by the scope is a pulse of magnitude Ei and duration that corresponds to the
time it takes the signal to pass down the line to the short and back again. If the velocity of the signal is
known, the length of the line can be calculated:
where v is the velocity of the signal in the transmission line, t is the measured pulse width and d is the length
of the transmission line.
4.7.7.1.2Example: open-circuited 50 ohm transmission line
Simplified representation of the response of a open line
In the case of the open circuit transmission line (figure above) the reflected signal is in phase with the
incident signal, so the reflected signal combines with the incident signal to produce an output at the scope
that is twice the incident signal. Again, the distance d can be calculated if the velocity of the signal is known.
4.7.7.1.3Example: resistively terminated 50 ohm transmission line
Simplified representation of the response of a resistively terminated line
4.7.7.1.4Reactive terminations and discontinuities
Reactive elements can also be determined by their response. Inductive terminations produce a positive
pulse. Capacitive terminations produce a negative pulse.
Simplified representation of the response of a reactively terminated line
Similarly, the position and type of discontinuity in a cable, due to connectors or damage, can be determined.
A positive pulse indicates a connector that is inductive or damage to a cable, such as a removal of part of
the outer screen. A negative-going pulse indicates a connector with too much capacitance or damage to the
cable, such as being crushed.
Simplified representation of the response of a line discontinuity
4.7.7.2Time domain from frequency domain
An alternative to traditional TDR is where the time domain response is determined from the frequency
domain using an Inverse Fast Fourier Transform (IFFT). Several methods are available for extracting time
domain information from the frequency domain. The main methods are lowpass and bandpass.
4.7.7.2.1Lowpass method
The lowpass method can produce results that are similar to the traditional TDR measurements made with a
time domain reflectometer using a step signal, and can also compute the response to an impulse. It
provides both magnitude and phase information and gives the best time resolution. However, it requires that
the circuit is DC-coupled. This is the method supported by the PicoVNA 106.
The lowpass method uses an Inverse Fourier Transform to determine the impulse response in the time
domain from the reflection coefficient measured in the frequency domain. The DC component is
extrapolated from the low-frequency data to provide a phase reference. Alternatively, if the DC termination is
known it can be entered manually. Once the impulse response is computed, the step response may be
determined from the time integral of the impulse response. In the step response mode the trace is similar to
that of a TDR, except that there is no step at t = 0. When the time domain response is derived from the
frequency information the value at t = 0 is the impedance of the transmission line or load immediately
following the calibration plane. The value is referenced to 50 Ω, the characteristic impedance of the system.
For example, an open circuit would appear as a value of +1 unit relative to the reference value and a short
circuit would appear as a value of –1 unit relative to the reference value (see example TDR plots above).
To facilitate the use of the Inverse Fourier Transform to compute the time domain response, the samples in
the frequency domain must be harmonically related and consist of 2
in the PicoVNA 106 makes available special 512, 1024, 2048 and 4096-frequency-point calibrations with a
stop frequency of up to 6000 MHz. The resulting alias-free range is a function of the number of frequency
points (N) and the total frequency span. It is given by the expression:
So, the available ranges on the PicoVNA 106 are approximately 100 ns, 171 ns, 341 ns and 683 ns.
The transform returns twice the number of points of the calibration in the time domain. Therefore the above
ranges provide time resolutions of approximately 98ps to 84ps.
n
points. For this reason, the TDR facility
4.7.7.2.2Bandpass method
The bandpass method provides only magnitude information so it is not possible to distinguish between
inductive and capacitive reactances. Also, the time resolution is only half as good as in the lowpass mode.
However, the method can be used for circuits where there is no DC path and hence is suitable for ACcoupled circuits such as bandpass filters. This method is not currently supported by the PicoVNA 106.
4.7.7.3Windowing
The bandwidth of the network analyzer is limited by the frequency range, so the frequency domain data will
be truncated at the bandwidth of the analyzer. Also the analyzer gathers data at discrete frequencies. The
result of the sampled nature of the data and the truncation in the frequency domain is to produce a sin(x)/x
response when transformed to the time domain. This appears as ringing on both the displayed impulse
response and the step response. To overcome this problem, a technique known as windowing can be
applied to the frequency domain data before implementing the Inverse Fourier Transform.
The windowing function progressively reduces the data values to zero as the edge of the frequency band is
approached, thus minimizing the effect of the discontinuities. When the modified data is transformed, the
ringing is reduced or removed depending on the selected windowing function. However, the windowing
function reduces the bandwidth and so increases the width of the pulse in impulse response mode and
slows the edge in step response mode. A balance must be made between the width of the pulse, or speed of
the edge, and the amount of ringing to be able to determine closely spaced discontinuities. The PicoVNA
106 allows you to choose a rectangular window (no bandwidth reduction), a Hanning window (raised
cosine), or a Kaiser–Bessel window. The order of the Kaiser–Bessel window is configurable.
4.7.7.4Aliasing
The sampled nature of the data means it is subject to the effects of aliasing. The result is repetition of timedomain response at the effective sampling rate in the frequency domain. This limits the maximum time
delay and hence maximum cable length that can be observed. In the PicoVNA 106 this is 683ns
(approximately 138m of cable).
Refer to the Quick Start Guide above for initial instructions, then return here for more detail.
5.1Minimum requirements
The recommended minimum requirements to operate the VNA are as follows.
PC or laptop
Pentium 4 (2 GHz) or equivalent
2 GB of RAM
200 MB of hard disk storage available on the C: partition
Windows 7, 8 or 10
Minimum display resolution of 1280 x 720
USB port
The performance of the software is influenced by the performance of the PC and video adaptor installed in
it. It is important that an adaptor with good graphics performance is used. As a general guide, it is
recommended that an adaptor with at least 64 MB of memory is used.
5.2Software installation
Follow the Quick Start Guide to install the software from the disk or from www.picotech.com. The installer
will copy the program and the USB driver to your computer. You need administrative privileges in order to run
the installer.
The installer creates a support directory at C:\User\Public\Documents\PicoVNA2. This directory contains
the following files:
xxx-log.txtThe status log file. ‘xxx’ is the serial number
DefCal.calDefault calibration data (last used calibration)
UsersGuide.pdfThis User's Guide
Support\Folder with data files to support the software
5.2.1Typical error messages
On Windows 7 machines it is common to see the following error message:
It is safe to click Ignore to continue the installation.
When the VNA is powered on, the front-panel channel activity indicators will flash to indicate that the
controller has started correctly.
5.4Calibration kit parameters
The minimum requirements to carry out a 12-term calibration (full error correction) depend on the device to
be tested. For example, the most accurate calibration is for ‘insertable’ devices, and this requires a total of
six standards: three of the four in each of the male and female cal standards.
An ‘insertable’ device is one that has connectors of different sexes at its ports. On the other hand, a
calibration for a non-insertable device can be carried out using only three standards by using the “unknown
through” calibration method.
The calibration kits parameters can be inspected using the Calibration Kit Parameters window (see below)
found under the Tools menu. From this the kit editor can be launched to modify and create new kits as
discussed later in the section.
The ‘unknown thru’ calibration method only requires that the ‘thru’ adaptor be reciprocal: that is, have S
.
S
12
=
21
Calibration Kit window. The short/open offsets are in mm in air.
Open circuit (2 pieces, one male and one female)
Short circuit (2 pieces, one male and one female)
Matched termination (2 pieces, one male and one female)
Through connection test cable(s)
For insertable DUTs the requirement is for two calibration kits, one of each sex. Generally, it is required that
the matched termination should be of good quality and, as a guide, should have a return loss of better than
40 dB. However, the PicoVNA 106 allows terminations with relatively poor return loss values to be used and
still maintain good accuracy. This is discussed in Using a matched termination
.
5.4.2Non-insertable DUT
Open circuit (1 piece)
Short circuit (1 piece)
Matched termination (1 piece)
Either a characterized through connection adaptor (1 piece) or any uncharacterized reciprocal adaptor
Through connection test cable(s)
For non-insertable DUTs only a single calibration kit is required. In addition, a reciprocal but otherwise
unknown through adaptor, or a fully characterized through adaptor, is required. These are supplied with all
Pico standard kits.
5.4.3Open circuit model
The open circuit capacitance model used is described by the equation below, where Freq is the operating
frequency. Generally, with typical open circuit standards, the effect is small, amounting to no more than a
few degrees of phase shift at 6 GHz.
= C0 + C1Freq + C2Freq2 + C3Freq
C
open
In addition, an offset length (sometimes referred to as offset delay) can be entered as well as the loss of the
offset line.
3
5.4.4Short circuit model
The short circuit inductance is modeled by an inductance component and in addition, a non-zero offset
length can be entered together with the loss of the offset line.
5.4.5Short and open without models
The PicoVNA 106 supports short and open standards defined by data only. In this case the data is supplied
in the form of a 201-frequency-points table. Each frequency point has three comma-separated entries:
frequency (in MHz), real part of the reflection coefficient and the imaginary part of the reflection coefficient.
5.4.6Calibration kit editor
As already mentioned, the calibration kit editor can be used to create or edit an existing calibration kit. The
figure below shows the editor window. A typical example is to create a new kit using an existing kit as a
template to speed the process. So, the process would be to first load the existing calibration kit from the
Calibration Kit Parameters
required. Finally, click Save Kit to save the new kit under a new name.
window. Type the new kit name in the name box and modify the parameters as
In the above example, if the existing kit loaded had load data or through data and you want to replace this
with new data, uncheck the appropriate box and then re-check it.
Calibration Kit Editor
The calibration kits optionally supplied with the PicoVNA 106 provide an economical solution while retaining
good measurement accuracy. They are supplied with SMA or precision PC3.5 (SMA-compatible) connectors.
Refer to the PicoVNA 106 Data Sheet for details.
5.4.7Using a matched termination with poor return loss or
unmodeled short and open
A successful calibration can be carried out without the need for a good-quality matched load. In order to
retain accuracy, it is necessary to provide the instrument with accurate performance data of the matched
load to be used. The data needs to be in a fixed format thus:
Frequency (MHz)
1.0-1.7265E-037.7777E-05
30.995-1.6588E-033.3093E-04
60.99-1.4761E-035.9003E-04
90.985-1.4653E-031.0253E-03
120.98-1.3841E-031.2608E-03
150.975-1.1924E-031.5800E-03
240.96-1.0884E-031.9085E-03
300.95-8.7216E-042.1355E-03
330.945-7.0326E-042.4109E-03
360.94-5.7006E-042.6790E-03
S11 (real)
S11 (imaginary)
There must be 201 data lines. Typically these should
cover the band 1MHz to 6.00GHz. No empty or
comment lines are allowed.
Table: format for characteristics of matched load
In the case when the models for the open and short are not known, it is possible to enter measured data in
the same format as shown above. This approach can give good results if the open and short can be
measured accurately, particularly at the higher frequencies where it is usually difficult to model components
accurately.
When supplied, the data for the through connection adaptor must be in the format shown below. The data
must be a full set of S-parameters with no empty or comment lines. It is recommended that the data spans
the full frequency range from 1 MHz to 6000 MHz.
Table: Format for the characteristics of the through connector. These must be a full set of S-parameters
(real and imaginary).
To add matched load, short and open, or through adaptor data to a calibration kit, follow the steps below:
Load kit using the Kit Editor (see Calibration Kit)
Check the Load Data Available box and similarly the boxes for the Thru and Short and Open circuits in the
Kit Editor parameters window.
If the existing kit already has load, short and open, or through data, uncheck and recheck the appropriate
box. If this is not done, the existing data will be kept and copied to the new kit.
If needed, manually enter the rest of the kit parameters. Ensure that the correct offset is entered.
Click Save Kit
When prompted, select the data file containing the matched load or the through adaptor data in the format
shown above.
Save the kit for future use by clicking the Save Kit button (see Calibration Kit).
Note: When a kit is loaded, any available matched load or through adaptor data that is associated with the
kit will be automatically loaded.
The calibration kits available for the PicoVNA 106 come complete with matched load, short and open, and
through adaptor data. Copy these files to your computer for easy access.
It is critically important that the correct kit data, with the correct serial number, is loaded.
The PicoVNA 2 software allows you to program the measurement parameters and plots the measurement
results in real time. The main window includes a status panel that displays information including calibration
status, frequency sweep step size and sweep status. The Help menu includes a copy of this manual.
6.1The PicoVNA 2 main window
The PicoVNA 2 main window is shown below. It is dominated by a large graphics area where the
measurement results are plotted together with the readout of the markers. One, two or four plots can be
displayed simultaneously. The plots can be configured to display the desired measurements.
User interface window
6.1.1Display setup
Setting up the display is carried out through the Display Set Up window which is called up from the main
window by clicking Display. The window is shown below. The typical sequence to set up the display is as
follows:
Set the number of channels to be displayed by clicking the appropriate radio button under Display
Channels
Select the desired active channel from the drop-down list (can also be selected by clicking on a marker in
the main window on the desired display channel)
Select the channel to set up by clicking the appropriate radio button under Select
Choose the desired parameter to display on this channel from the drop-down list under Parameter / Graph
Type
Choose the desired graph type from the drop-down list under Parameter / Graph Type
Select the vertical axis values from the Vertical Axis section. Optionally, click Autoscale to automatically
set the sensitivity and reference values. Note that reference position 1 is at the top (see second figure
below).
Click Apply to apply the selected values
Repeat the above steps for each display needed
Note: The Active Channel must be one of the displayed channels.
The Display Set Up window is used to set up the measurements displa
The colors of the main graphics display can be changed to suit individual preferences. This can be done by
selecting the Color Scheme item from the Tools menu. To set a color, click the color preview box next to
the item name.
Once you have set up a color scheme, you can save and recall it as a Cal and Status setting using the File
menu.
Editing graph parameters using the mouse
The figure above shows how the mouse can be used to quickly adjust reference position, reference value
and vertical scale sensitivity.for the graph. Drag the indicated values up and down to adjust, or type a new
value where the cursor indicates.
6.1.2Data markers
It is possible to display up to eight markers on each display. They are set up by clicking on the Markers
button (see figure below). There are four possible marker modes as follows:
Active marker: The active marker is the marker used for comparison when the delta marker mode (switched
on by selecting a reference marker) is on. One of the displayed markers must be chosen as the active
marker.
Reference marker: The reference marker causes the delta marker mode to be switched on. The value
difference between the active marker and the reference markers is shown on the right hand marker display
panel.
Fixed marker: A fixed marker cannot be moved and its position is not updated with subsequent
measurement values. It provide a fixed reference point. Only a reference marker can be made a fixed
marker. Once a marker is fixed, it cannot be moved until it is unfixed.
Normal marker: The value of a normal marker is displayed on the right-hand marker readout panel and in
lower resolution readouts below each measurement plot.
Any marker (except a fixed marker) can be moved to a new position by left clicking on it (on any displayed
channel) and dragging it to a new position.
The markers set up form provides a Peak / Minimum Search facility. This places marker 1 at either the peak
or minimum value on the displayed trace on the active channel when the corresponding Find button is
pressed.
The Markers Set Up dialog is used to display measurement markers
Change the marker type by right-clicking on any marker on the active channel. Note that only the reference
marker can be fixed.
The peak / minimum search facility provides a means of placing additional markers to indicate the 3 or 6 dBbandwidth. If either the 3 dB or 6 dB band box are selected, then clicking Find will place markers 2 and 3 on
the frequency points either side of marker 1 which are 3 dB or 6 dB relative to it. Note that for best accuracy
a sufficient number of sweep points should be used. This will ensure a fine enough resolution to allow
accurate determination of the band points.
6.1.3Measurement enhancement
The measurement enhancement options are displayed (see figure below) by clicking Enhancement in the
main UI window. The options available are as follows.
Averages (1 to 255, on a point by point basis)
Trace Smoothing (0 to 10%)
Bandwidth (140 kHz to 10 Hz)
Port 1 Level (+6 dBm to –20 dBm, 0.1 dB resolution)
CW sweep time per point (500 to 65 000 μs/point)
Reference Plane Extension (manual entry or automatic)
Effective dielectric constant of device under test (manual entry to correct plane extension values)
De-embedding (specify embedding networks at ports 1 and or 2)
Impedance conversion for devices that are not 50 Ω
Operation32
The measurement enhancement window
The Bandwidth setting refers to the receiver bandwidth. Maximum sweep speed is achieved with the highest
(140 kHz) setting. On the other hand, the widest dynamic range (lowest noise floor) is achieved with the
lowest value, 10 Hz. Note that the bandwidth setting used during calibration determines the maximum
dynamic range achievable during measurements. So, consider this when carrying out a calibration. For
example, if you need to carry out measurement over more than, say 90 dB dynamic range, then use a 500 Hz
or less bandwidth setting when calibrating.
The Port 1 Level sets the test signal level. The default value is +3 dBm as this gives best overall
measurement accuracy. However, it may be necessary, particularly when measuring active devices (e.g.
amplifiers) to reduce the test level. For maximum dynamic range, then use the highest power setting. For
best measurement accuracy it is recommended that the calibration is carried out at the same test level as it
is intended to use for the measurement. Whenever the test level is different to that used for the calibration, a
‘?’ will be added to the calibration status indicator on the Status Panel (Fig. 6.1)
The Reference Plane facility allows the reference plane of each parameter measurement to be arbitrarily
moved away from the calibration plane. The value entered applies to the measurement parameter (S
or S22) displayed on the active channel. Note that the same plane value will be used for all other
S
12
11
, S21,
measurements on that same parameter regardless if they are on the active channel or not.
The Auto Reference automatically moves the reference plane. It uses the measurement on the active
channel. This feature is particularly useful, for example, when measuring microstrip devices and it is
necessary to remove the effect of the connecting input and output lines. It takes the effective dielectic
constant value entered to correct the displayed value. Refer to Reference plane extension and de-embedding
for more details.
Note: The reference plane must be at 0 mm for the Auto Ref function to work correctly. Also, Enhancement
window changes only take place when the instrument is sweeping.
The Effective Dielectric of the device under test can be entered so that the displayed Reference Plane
extension values (shown on the Enhancement Window) are corrected accordingly when the Auto Ref button
is clicked. The default value is 1.0 and the maximum value allowed is 50.0.
Note: The reference plane extension value shown in the main window
on the markers display panel on the
right is the reference plane extension as shown in the Enhancement window.
The de-embedding facility is explained in detail in Reference plane extension and de-embedding.
The System Z
Conversion facility allows measurements, which are always taken in 50 Ω, to be converted to
0
another impedance selected by the user. This feature can be useful, for example, for measuring 75 Ω
devices. The value of Z
entered must be real (purely resistive) and must be within the range of 10 Ω to 200
0
Ω. Whenever this facility is selected, an indicator is displayed on the top right corner of the graphics display
as shown in the second figure below. Note that when requested, impedance conversion will performed on
the live measurement and any stored memory trace.
There are two possible ways of using the System Z
Conversion facility. For example, 75 Ω devices can be
0
measured using the techniques illustrated below.
Possible techniques for measuring 75 Ω devices.
Impedance matching pads can be used to measure a connectorized device.
A discrete device mounted on a 50 Ω test jig is somewhat simpler to measure.
The steps necessary for each of the two techniques illustrated in the figure above are as follows:
75 Ω device with connectors
i. Connect 50 Ω to 75 Ω impedance matching networks (e.g. matching pads) at the ends of the cables
connected to ports 1 and 2.
ii. In the Enhancement window, check the Convert System Zo box
iii. Check External Zo match to indicate external matching networks in use
iv. Enter 75 in the Convert System Zo value box and click Apply
v. Proceed to calibrate using a 75 Ω calibration kit
vi. Connect the DUT and start the measurement
75 Ω device mounted on 50 Ω test jig
i. In the Enhancement window, uncheck the Convert System Zo box
ii. Calibrate at the ends of the test cables using a 50 Ω calibration kit
iii. Apply de-embedding to remove test jig effects. See Calibration kit
for some suggestions.
iv. In the Enhancement window, check the Convert System Zo box
v. Uncheck the External Zo match box (in this case mathematical impedance conversion is done by the
software)
vi. Enter 75 in the Convert System Zo value box and click Apply
vii. Connect the DUT and start the measurement
System impedance chosen is displayed on the top right corner
Note: S-parameters are interrelated, so, when using the Z
matching networks) without a full set of S-parameters available (e.g. only an S
conversion facility (and no external impedance
0
calibration) the program
11
will assume values for the unavailable parameters as shown in the following table. A warning will be
displayed in such cases.
S
11
S
12
S
21
S
22
10–6, j0.010–6, j0.010–6, j0.010–6, j0.0
Table: Values assumed for parameters not available during Z0 conversion
6.1.4Memory facility
The current displayed data on each channel can be stored in memory. Also, each channel can be stored
independently of all others. The Memory Set Up window is used to store the data and this window can be
displayed by clicking Memory in the main window.
The Memory Set Up window is used to store data into memor
Once the data is stored, it can be displayed by clicking Display Data and Memory in the main window.
There are three vector math functions available: sum, subtraction and division. The selected function is used
when you select the Display Memory Math function on the main window.
The trace hold is used to store the maximum or minimum values on the memory trace. Trace hold is not
available when group delay is displayed.
6.1.5Limit lines facility
The limit lines facility allows six segments to be defined for each displayed graph. By taking advantage of
the overlapping capability (see below) a maximum of 11 segments can be created The set up window,
shown below, is displayed by clicking Limit Lines in the main window.
Overlapping segments
All valid segments entered are loaded in sequence (i.e. segment 1 first) with the each segment loaded
having priority over the previous segment. This feature allows overlapping segments to be loaded. For
example, if segment 1 is specified to cover, say, 400 to 800 MHz, then a second segment can be specified to
a section of this band, for example, 500 to 600 MHz. This would result in a total of three segments—that is,
400 to 500, 500 to 600 and 600 to 800 MHz—even though only two were specified. An example of a complex
11-segment template is shown in the first plot below.
Alarm
An alarm facility is provided with the limit lines. This provides audible warning during a sweep if any
measurement exceeds the limits set. A visible indication of the last measurement and measurement
channel in error is provided on the status panel where normally the calibration type is displayed. In addition a
symbol is drawn on the trace indicating the last error point detected as shown in the second plot below. The
alarm is available for all graph types except Smith plots.
The Limit Lines Set Up allows at least six segments per graph
It is possible to synchronize each measurement sweep to an external trigger. Simply click the appropriate
radio button in the main window and ensure that a trigger signal is connected to the instrument’s rear panel
Trigger terminal.
The instrument supports either positive or negative edge trigger depending on the radio button selected on
the main panel. The input impedance is 10 kΩ.
Trigger selection radio button on main panel
When the Manual trigger option is selected, the instrument will wait until the Manual button is pressed
before starting a sweep.
6.1.8Sweep trigger output
The rear panel Trigger Output terminal provides a 3 V logic output with the rising edge synchronized to the
start of the measurement sweep. The signal goes to 0 V at the end of the sweep. The output resistance is
about 500 Ω.
6.1.9Measurement start / stop
The measurement Start / Stop buttons (see figure) are used to start or stop the instrument’s sweep mode
(measurement mode). This is necessary as functions which require reprogramming the instrument can only
take place when the instrument is idle. The instrument status is shown in the Status Panel as described in
the previous section.
The Start / Stop Measurement buttons control the sweep status
Note that when the sweep is stopped, the test signal frequency is held at the frequency point at the time the
stop command is received by the instrument. In the case of triggered sweep, by default, at the end of the
sweep, the frequency is held at the last frequency point until the next sweep trigger event is received. This
can be changed from the Tools > Diagnostics menu.
6.1.10PC data link interruption
The data flow between the VNA and its controlling PC can be interrupted by external factors. If the software
cannot restore the link, a message similar to this will appear:
Warning message when the link with the PC is interrupted
Restart the software using the selection in the drop-down menu under Tools
Switch the VNA off and on again (using the switch on the back) when prompted to do so
Wait until the front panel lights have stopped flashing
Click OK to complete the software restart
Recalibrate the instrument
You should rarely see a ‘No Response’ message. If it happens often, check that the PC is not running other
applications and that the VNA software is not running as a background task when the sweep is on.
6.2Calibration
The instrument must be calibrated before any measurements can be carried out. This is done by loading a
previous calibration (see File menu) or carrying a fresh calibration by clicking Calibration in the main
window, which brings up the Calibration window as shown here:
Instrument calibration is carried out through the Calibration window. Before starting calibration select the
referred enhancement settings (bandwidth and averages).
Note: The frequency sweep is set by entering the start, stop and selecting the number of sweep points.
Alternatively, by entering the centre frequency and span after clicking on the Centre/Span format option
box.
The table below summarizes the calibration types available together with the standards required to
complete the calibration. For best overall accuracy, particularly when measuring low isolation devices with
poor return loss values, a 12-term calibration should be performed.
Minimum
calibration
standards
required
S
11
Matched load
Open
Short
S
21
Through
connection
Termination (see
text)
S11 + S
21
Matched load
Open
Short
Through connection
12 terms (insertable
DUT)
Matched load (x 2)
Open ( x 2)
Short (x 2)
Through cable
12 terms or 8 terms*
(non-insertable DUT)
Matched load (x 1)
Open ( x 1)
Short (x 1)
Through adaptor (x
error correction
Frequency response
with isolation and
source match
correction
12 terms (insertable
DUT)
S11, S21, S12, S22 using
12-term error
correction
12 terms or 8 terms*
(non-insertable DUT)
S11, S21, S12, S22 using
12-term error
correction
Table: Calibration types supported.
* The unknown through calibration (8 error terms) requires only a reciprocal through adaptor.
Here is the basic calibration sequence:
Instrument calibration sequence
The calibration process involves connecting each standard in turn and clicking. An asterisk will appear once
it has been measured so that the next standard can be done.
Note: For best results, ensure that the instrument is fully warmed up before carrying out a calibration.
It is important to be aware of the difference between ‘insertable’ and ‘non-insertable’ devices and the impact
on measurement and calibration technique. The figure above illustrates the difference between an insertable
device and non-insertable devices. The key issue is that with non-insertable devices an adaptor may be
required during the measurement as shown. In order to obtain accurate measurement data, the effect of the
adaptor needs to be removed from the measurements. Some of the possible ways of doing this with the
PicoVNA 106 are as follows:
(B) 8-Term (unknown through method)Calibration automatically
removes adaptor effect
(C) Any except 12-term or 8-termDe-embeddingAccurate but requires prior knowledge of
(D) Any except 12-term or 8-termReference plane extensionQuick and easy but errors due to loss of
Accurate but requires kit with through
adaptor standard. Only one calibration kit is
required.
Accurate and easiest method as it does
not require a characterized through
standard
adaptor characteristics
adaptor remain
Table: Techniques for dealing with non-insertable DUTs
The preferred method is method (B) in the table above. This requires only a reciprocal through adaptor. Note
that with this method the isolation calibration is done automatically by the software using measurements
taken during the short, open and load steps.
Note that only the 12-term non-insertable DUT calibration and 8-term unknown through methods support a
non-zero length through connection. All other calibrations (S
or S11+S21 or full 12-term insertable DUT)
21
require a through connection of zero length. In effect, this means that the calibration port terminals should
be of opposite sexes. In other words, it should be possible to connect the terminals together without the use
of an adaptor. Consequently, the DUT must be an insertable device. If this is not the case, an adaptor will be
needed during the measurement and its effect will need to be removed by either moving the reference plane
or by using the de-embedding facility as indicated in the table above.
When performing just an S
calibration it is possible to complete the calibration without doing the isolation
21
calibration. Simply click Apply Cal after performing the through calibration. The isolation calibration corrects
errors due to crosstalk (see Calibration and error correction
) and should be used when measuring insertion
losses larger than about 40 dB. The terminations to use during the isolation calibration can, as a guide, be
50 Ω loads. In some circumstances, such as when testing a highly reactive device (e.g. filter beyond cut-off),
a short or an open circuit may be more appropriate or for best results two actual DUTs with 50 Ω loads at
their unused ports.
6.2.1Changing the frequency sweep settings without
recalibrating
If the start or stop frequency or number of sweep points is changed when the instrument has a valid
calibration, the user is given the choice to either keep or delete the existing calibration. If the user chooses to
keep the calibration, a new set of calibration error terms will be automatically generated by interpolation to
fit in with the new sweep parameters. In this case, a “?” is added to the calibration status bar to indicate that
operating parameters have changed from those used in calibration.
If it is required to change the frequency sweep parameters without recalibrating, then simply enter the new
values (see Set Sweep Frequency values under Calibration
) and click Apply. Once the new values are sent to
the instrument, just close the window (click Close Window) to exit. Note that this process will delete allmemory traces and the display data may be invalid until a fresh measurement sweep is performed.
Some care needs to be exercised when using interpolation, particularly at low frequencies, say below 20
MHz. For example, if starting with a wide band sweep with large frequency steps, say 500 kHz or larger, then
interpolating down to a narrow band of, for example, 1MHz to 10MHz may lead to larger than expected
errors.
The calibration for S11 measurements performs a three term error correction calibration. Note that if the
device to be tested has a female connector, then a female calibration kit should be used for best results. The
2. Set the bandwidth and test power (Enhancement button)
3. Set the frequency range and measurement steps (Calibration button)
4. Select S
5. Connect adaptor and test cable to port 1 of the instrument
6. Connect each standard in turn and click appropriate Standard button (in Calibration window)
7. When all 3 Standards are done click Apply (in Calibration window)
8. If desired, for later use, save calibration (File > Save cal)
9. Connect device to be tested and click Start
Tips:
For best linearity and dynamic range combination use a test power level of 0 dBm
For best accuracy calibrate using the same bandwidth you intend to use for your measurements
You can remeasure any standard at any stage before completing the calibration. Just reconnect the
standard and click again on the appropriate Standard button before completing the calibration
calibration (in Calibration window)
11
6.2.3Calibration steps for S21 measurements
The simple S21 calibration is a frequency response calibration. Sometimes it is referred to as normalization
and only corrects for response characteristics of instrument and external connections. The typical steps are
as follows:
1. Set the bandwidth and test power (Enhancement button)
2. Set the frequency range and measurement steps (Calibration button)
3. Select S
4. Connect adaptors and test cable 2 to port 1 of the instrument
5. Connect ends of test cable together (the ‘through’ connection) and select Through (in Calibration
window)
6. Connect 50 Ω load to the ends of test cables (to perform the isolation step) and select Isolation (in
Calibration window)
7. Click Apply (in Calibration window)
8. If desired, for later use, save calibration (File > save cal)
9. Connect device to be tested and click Start
Tips:
For best dynamic range, use a test power level of +6 dBm and calibrate using the same bandwidth you
intend to use for your measurements
For best accuracy (linearity) use a test power level of –3 dBm and calibrate using the same bandwidth
you intend to use for your measurements
calibration (in Calibration window)
21
6.2.4Calibration steps for S11 and S21 measurements
The 'S11 + S21' calibration provides three term error correction for S11 measurements and Source match
correction for S
5. Connect each standard (short, open and load) in turn and click appropriate Standard button (in
Calibration window)
6. Connect ends of test cables together and click Through
7. Connect 50 Ω load to the ends of test cables (to perform the isolation step) and select Isolation (in
Calibration window)
8. Click Apply (in Calibration window)
9. If desired, for later use, save calibration (File > Save Cal)
10.Connect device to be tested and click Start
Tips:
For best linearity and dynamic range combination, use a test power level of 0 dBm
For best dynamic range use a test power level of +6 dBm and calibrate using the same bandwidth you
intend to use for your measurements – particularly at the isolation calibration step
6.2.5Calibration steps for all S-parameters measurements
(insertable DUT)
This calibration provides full error correction for all S-parameters. Typical steps are as follows:
2. Set the bandwidth and test power (Enhancement button)
3. Set the frequency range and measurement steps (Calibration button)
4. Select ’All –Insertable DUT’ calibration (in Calibration window)
5. Connect each standard (short, open and load) in turn and click appropriate Standard button (in
Calibration window)
6. Click Isolation select the first method on the left (isolation is measured with 50 Ω loads on each
calibration port which is the same as the load step in 5 above)
7. Connect ends of test cables together and click Through
8. Click Apply (in Calibration window)
9. If desired, for later use, save calibration (File > Save Cal and Status)
10.Connect device to be tested and click Start
Tips:
For best linearity and dynamic range combination use a test power level of 0 dBm. Use the same
bandwidth as you will use during measurements.
For best dynamic range use a test power level of +6 dBm and calibrate using the same bandwidth
you intend to use for your measurements.
6.2.6Calibration steps for all S-parameters measurements
(non-insertable DUT)
This calibration provides full error correction for all S-parameters. It requires a calibration kit with a
characterized through connection. Typical steps are as follows:
6.2.7Calibration for best dynamic range – minimizing the effect
of crosstalk
Instrument crosstalk is a limiting factor when making large dynamic range measurement. This is particularly
the case at higher frequencies, say above 4 GHz. The reason is that some of the crosstalk is dependent on
the loading at the test ports. Therefore, the isolation calibration process can only compensate it fully when
the terminations are left unchanged from those used at the isolation calibration step.
Enhanced isolation calibration
The PicoVNA 106 provides an enhanced isolation calibration option. This method makes crosstalk
measurements at the short, open and load calibration steps. In this way it attempts to more closely model
the effect of port termination on the internal crosstalk components of the instrument.
The enhanced isolation calibration helps to model the crosstalk more accurately
It is important to note that for best dynamic range, when using the enhanced isolation calibration method,
each of the short, open and load steps need to be made at the same or lower resolution bandwidth that will
be used for the measurement. So, for the ultimate range, each calibration step will need to be done using 10
Hz bandwidth. This is the downside of the enhanced isolation calibration (slower overall calibration process)
compared to traditional isolation calibration, where only the isolation step need be taken at the lowest
bandwidth setting.
Achieving the ultimate dynamic range using conventional isolation calibration
In cases when two identical DUTs are available, the ultimate dynamic range can be achieved using a
conventional crosstalk (isolation) calibration step as shown in the figure below. In this approach the correct
termination is presented at each port during the crosstalk calibration step. In this way its effect can be
removed accurately over the entire measurement band. Note that when using this technique, only the
isolation step need be performed at the lowest resolution bandwidth. The other calibration steps can be
performed at higher bandwidth settings to speed up the process.
The measurement result can be displayed by selecting the S
as described in Display setup
. Note that the measured phase is relative to the calibration reference plane as
discussed in Reference plane extension and de-embedding
parameter and an appropriate display graph
11
. The reference plane can be shifted at any time
from the Enhancement window. Note that changes to the reference plane only take place when the
instrument is sweeping.
6.3.2Insertion loss / gain
To carry out insertion loss measurements (S21) the VNA must be calibrated with the test cables in place,
either S
between Ports 1 and 2 of the VNA as indicated in the figure below.
For best results, the arrangement shown on the right hand side of the figure should be used whenever
possible. When using an S
the other hand, when using a 12-term calibration, this will minimize repeatability / cable flexing errors
associated with the connecting cables.
calibration only, both S11 and S21 or full 12-term. The device to be tested (DUT) is then connected
21
calibration this will minimize errors introduced by the load return loss. On
11+S21
Connect DUT between Ports 1 and 2 to carry out S21
measurements. For best results use the arrangement shown on
Displaying the results
The measurement result can be displayed by selecting the S
and described in Reference plane extension and de-embedding
parameter and an appropriate display graph
21
. Note that the measured phase is relative to
the calibration reference plane as discussed in that section. The reference plane can be shifted at any time
from the Enhancement window. Note that changes to the reference plane only take place when the
instrument is sweeping.
6.3.3Complete 2-port measurement
In order to measure all four s-parameters a 12-term calibration needs to be completed. The arrangement
shown on the right hand side of the figure above is likely to yield best results in terms of repeatability by
virtue of using only one test cable, reduces the effects of cable flexing.
Displaying the results
The measurement result can be displayed by selecting a different parameter for each of the possible four
display graphs, as described in the previous section. Note that the measured phase is relative to the
calibration reference plane as discussed in Reference plane extension and de-embedding
plane can be shifted (independently for each parameter) at any time from the Enhancement window. Note
that changes to the reference plane only take place when the instrument is sweeping.
. The reference
Maximizing dynamic range
Refer to Calibration for best dynamic range – minimizing the effect of crosstalk
Group delay is defined as the rate of change of phase with frequency:
In relatively non-dispersive components such as transmission lines, group delay is the transit time through
the line. However, some components such as filters can exhibit negative group delays so care is needed
when attaching an interpretation to group delay.
The PicoVNA 106 calculates the group delay by dividing the phase change between adjacent sweep points
and dividing by the size of the sweep step. It is usual to apply some degree of trace smoothing to remove
very rapidly changing perturbations from the trace. Care should be exercised to ensure that genuine sharp
group delay variations are not masked by the smoothing.
Displaying the results
Group delay of any S-parameter can be measured. The result can be displayed by selecting the required
parameter and group delay graph from the Display window as described in Display setup
.
6.3.5Time domain measurements
The time domain facility allows the display of the time domain response of a network under test. For
example, time domain reflectometry (TDR) measurements can be made by first carrying out an S
calibration using 1024 sweep points. Similarly, time domain transmission (TDT) measurements can be
made by first completing an S
flowcharts below.
calibration using 1024 sweep points. The steps necessary are shown in the
Note that carrying out time domain measurements requires a lot of mathematical processing and therefore
each sweep will be noticeably slower when displaying time domain.
Examples of TDR measurements using the PicoVNA 106
The trace below shows the time domain response of a 50cm, 50 Ω coaxial cable with an open circuit
termination. The trace goes to +1 relative to the reference indicating a reflection coefficient of +1 for an
open circuit. The window used is rectangular.
Measured 50 cm line terminated in an open circuit.
The trace below is the same as above except that the ringing either side of the transition has been reduced
by the use of a fifth order Kaiser–Bessel window. This reduces the ringing but also slows the rise time.
Same as previous figure but using the Kaiser–Bessel window.
The type of window, the order of the Kaiser–Bessel window, and the time span over which the signal is
displayed can be selected in the TDR options window, shown below.
Time Domain Options window allows measurement setu
Note: To set a time range either starting or ending beyond 161.66ns, use the Enter T1, T2 facility. However,
the displayed total time span must be less than 166.66ns.
The plot below shows the same cable terminated with a short circuit. The window is fifth-order Kaiser–
Bessel. This time the trace goes to –1 relative to the reference, indicating a reflection coefficient of –1 for
the short circuit.
Measured response of 50 cm shorted cable using Kaiser-Bessel fifth-order window
The trace below shows the effect of increasing the order of the Kaiser–Bessel window to 10. The ripple has
been completely removed but the slope of the edge has been further reduced.
Measured response of 50cm shorted cable using tenth-order Kaiser-Bessel window.
A more complicated example:
The trace below shows the response of a 30cm, 50 Ω line followed by 30cm of 25Ω line terminated in a
short circuit. The window is third order Kaiser–Bessel. The trace shows the multiple reflections from the
discontinuity of impedance at the connection between the lines and the short circuit termination.
Measured response of multiple reflections. See text for details.
The last example is the same 50 Ω / 25 Ω cable combination but this time the termination is an open circuit.
The response is also displayed over a longer period.
Measured response of multiple reflections. See text for details.
Time domain transmission (TDT) is similar to the TDR technique except that the transmitted signal is
observed. Traditionally, this is accomplished using a step source and a sampling scope, as with the TDR, but
the transmitted signal at the output of the network is observed rather than the reflected signal at the input to
the network. This technique is useful for measuring the step response or rise time of amplifiers, filters and
other networks.
Examples:
Expected responses from simple RC networks
Measured TDT for 100pF series capacitor
Measured TDT for 100pF shunt capacitor
6.3.6Reverse measurements on two port devices
In order to measure the reverse parameters (S12 and S22), it is necessary to complete a 12-term calibration
first (select ‘insertable’ or ‘non-insertable’ DUT on calibration window as shown in Display setup
calibration options measure only forward parameters. After the 12-term calibration is completed, simply
select the reverse parameter(s) to be required on any displayed channel and start the measurement.
6.3.7Powering active devices using the built-in bias-Ts
The PicoVNA 106 includes two bias-Ts, which can be used to provide DC bias to the measurement ports 1
and 2. The bias-Ts are rated at 250 mA and can support DC voltages up to 15 V. The DC injection terminals
are type SMB, male, and are located on the back panel. This facility can be used, for example, to provide DC
bias to an active device being measured.
CAUTION
To avoid causing permanent damage to the internal biasing circuit, do not exceed the voltage
and current ratings.
6.4Reference plane extension and de-embedding
The reference plane extension facility on the PicoVNA 106 allows you to shift the measurement reference
plane away from the value set during calibration. This can be useful in removing the effect of
interconnecting cables or microstrip lines from measurements. The instrument allows independent
reference plane extensions on each of the measurement parameters (S
An example of an application requiring the use of reference plane extension is shown below. In this, it is
desired to measure the S
remove the effect of the interconnecting line to the input of the device, the following procedure may be
followed:
of a device mounted on a microstrip test jig with SMA connectors. In order to
11
, S22, S12 or S21).
11
Perform an S11 calibration at the end of the N to SMA adaptor on Port 1
Connect the test jig without the DUT mounted on it
Display the phase of the S11 on active display channel
Click Auto Ref in the Enhancement window
Click Apply in the Enhancement window
The above steps will move the reference plane to the end of the microstrip line. This can be verified by
noting that the displayed phase is close to 0° over the entire measurement band. Imperfections associated
with the microstrip line and coaxial connector, such as loss and dispersion, will mean that some residual
phase will remain. However, with careful design and employing good RF practice for the construction of the
jig, this error should remain small.
After the above steps are completed, the DUT can be mounted on the jig and its S
parameter measured.
11
Example of S11 measurement requiring reference plane extension
Note: The reference plane extension moves the reference plane for each parameter measurement
independently. So, if required for example, different values can be used for S
extension value entered, applies to the active channel measurement parameter (either reflection or
transmission).
In the example above, correction was applied to the S11 phase but not S21. An often-used way to correct the
phase is by using a calibration jig with length of microstrip line equal to the sum of the two sections of
S
21
line used either side of the DUT jig (see figure below). Proceed as follows to make S
11
and S
21
measurements of the DUT.
Reference plane extension for S
correction
11
Perform a 12 term calibration (exclude test jig). Ensure that the test cable has connectors of different sex
at each end. Adaptors may be needed to connect the DUT.
Connect the input port of the test jig without the DUT mounted on it to Port 1
Display the phase of the S11 on the active display channel
Click Auto Ref in the Enhancement window
Click Apply in the Enhancement window
Normalization for S
correction
21
Connect the through microstrip test line between Ports 1 and 2 of the VNA
Display the phase of S21 on a non-active channel (keep active channel for S11)
Start the measurement and store data on the S21 channel only to memory (use the memory window)
Select Data / Memory for the math function in the Memory window
Select the Memory Math display in the main window
Correcting S21 and S11 phase measurements. Reference plane extension corrects S11 measurements and
normalization to a test line corrects S21.
The above steps will allow the DUT's S
and S21 (or S22 and S12) parameters to be measured with the right
11
phase correction. In addition, the loss of the microstrip line will be accounted for. The same approach can
be used to measure S
and S22. Note, however, that there will be an error on both measurements due to the
12
imperfections of the microstrip line and connector interface. With careful design of the jig these can be kept
acceptably small but further accuracy can be achieved by making use of the de-embedding facility described
below.
A typical measurement jig, as shown below, includes input and output networks which introduce errors to
the measured values of the device under test (DUT). For best measurement accuracy, these networks can be
specified (in the form of 2 port s-parameter files) and then used to extrapolate the DUT’s characteristics.
De-embedding allows the effects of the test jig’s input and output networks to be
removed.
The PicoVNA 106 allows you to specify S-parameter files (must be full 2-port data) for the input and output
networks as shown in the figure above so that the de-embedding takes place automatically as the
instrument measures the test jig. After first calibrating as usual, follow the steps below to enable deembedding.
1. Select the S-parameter file(s) that represent the embedding network(s) by clicking on the embedding
network check box(es) as shown in Measurement enhancement
the input network as shown in the figures in Reference plane extension and de-embedding
. Check box Port 1 Network represents
, and Port 2Network represents the output network. The files selected must be full 2-port S-parameter files in
Touchstone format.
2. Click on the radio button in the Measurement enhancement
window to enable de-embedding.
Once the above steps are completed, starting the measurement will display de-embedded results.
The de-embedding facility relies on S-parameter data for the input or output network (or both) being
available. This data must be in the form of 2-port S-parameter files in Touchstone format.
Measured data can be saved to a file by selecting File > Save Measurements in the main menu. Various
formats are available as shown. In all cases, frequency is saved in megahertz. Note that only the
Touchstone format can later be read back into the instrument’s memory trace.
The Save Measurements window is used to save data
Note: For true compatibility with the Touchstone format, only 1-port or full 2-port S-parameters should be
saved. For example, selecting S
If required, the data can be saved with the memory math function applied as described earlier under Memory
facility. In order to do this, check the Apply Memory Math box. Note that the memory math display function
on the main window
When saving data in Touchstone format, ensure that you provide the file name extension when entering the
file name. Typically, for 1-port networks, the extension “.s1p” is used and “.s2p” for 2-port networks. This
will help when reading back the data files since, by default, only files with these extensions will be
displayed.
Note: Data will be saved with any system Z0 conversion applied.
must be set otherwise the Apply Memory Math check box will be disabled.
and S21 (but not S12 and S22) is not Touchstone compliant.
11
6.6Loading data
Measured data (or data from a circuit simulator) can be read into the instrument’s memory trace(s). This
can be done by selecting File > Load Measurement in the main menu. The file containing the data (in
Touchstone) format is selected by clicking Select Data File.
The data will be read from the file and copied to the appropriate display channel(s). So, for example, assume
you read a data file holding full 2-port data. Further, you have only two channels on display showing, say, S
and S21, so only the S11 and S21 data from the data file read will be copied to the memory traces of the
displayed channels. Note: system impedance conversion will apply if turned on in the Measurement
You can plot the graphics displayed on the main window using the File menu. A printer set-up window will
appear from you can choose the desired printer and set its properties. If required, you can add a label to the
plotted graphics by clicking File > Print / Save Graphics Label.
A label can be added when plotting or saving graphics
A similar plotting facility exists on the P1dB
and AM to PM utilities' control windows.
6.8Saving graphics
The graphics shown on the main window can be saved in .bmp, .png, .gif, .tif or .jpg formats. This allows
measurement results to be directly pasted into most electronic documents. The facility to save the graphics
can be found under the main File menu. After clicking, a dialog box will appear allowing you to select the
name of the file, its location and format from a drop-down box. As described in the previous section, a label
can be added by clicking File > Print / Save Graphics Label.
The save graphics facility is not available on the P1dB
can be captured by pressing the Alt+PrtScn key combination. The image can then be pasted to the chosen
document from the Edit menu.
and AM to PM utilities. Instead, the graphics on these
This utility allows the instrument to act as a simple signal generator with variable output power. The VNA
measurement sweep must be stopped first and the control window, shown below, called from the Utilities
menu:
The Signal Generator utility control window
6.10Output power at the 1 dB gain compression point
utility
This utility allows the measurement of the power output at the 1 dB gain compression point (P
devices such as amplifiers. The measurement can be done at a single frequency or over the entire frequency
plan specified at the last S-parameter measurement calibration. Start the utility from the Utilities menu in
the main window.
calibration
P
1dB
Calibration minimizes errors by removing small variations associated with the instrument’s hardware. The
procedure is simple, as shown below.
Ensure that an S21 (or S11 + S21, or 12-term) calibration has been carried out
Connect Port 1 to Port 2 as shown on the left-hand side of the figure below
Enter Input Attenuation and Output Attenuation values (or select Read from file)
Enter the test frequency (or select Use sweep plan) and click Calibrate
test
P
1dB
The basic connection arrangement is shown on the right hand side of the figure below. Note that the input
and output attenuators should be carefully selected to ensure that the DUT compresses whilst preventing
the power at Port 2 of the instrument exceeding the nominal limit of +10 dBm. It is recommended that the
following guidelines are used to estimate the value of the input and output attenuators needed.
P
1dB(DUT)
– G
(DUT)
–1 + A
= –5 ± 2 dBm
tt1
) of active
1dB
where:P
1dB(DUT)
G
(DUT)
A
tt1
= output power of DUT at the 1 dB gain compression point
Basic connection guide for P1dB measurements. Calibration connection is shown on the left.
The instrument makes the measurement by setting the signal source (Port 1) frequency to the chosen value
and then stepping its power from –20 to 0dBm in 1 dB steps. The gain at each power setting is recorded.
On completion of the power sweep, a second order curve is fitted over a narrow section centered on the
point closest to the 1 dB gain compression point. The coefficients of this curve allow the actual P
point to
1dB
be calculated.
Note: Choose the input attenuator with care. Ensure that there is no gain compression at the start of the
power sweep (–20 dBm at Port 1) and that at least 0.7 dB of gain compression is reached at the end of the
sweep (0 dBm at Port 1). A ‘?’ will be displayed if insufficient compression has been achieved.
After the attenuator values have been established and the DUT is in place (and powered up as appropriate),
enter the values into the P
directly on the P
value, it is important to enter an accurate value that takes into account all losses in the
1dB
control window (Fig. 6.34). Note that the output attenuation value impacts
1dB
output path, including any connecting cable that may have been used.
Clicking Start will perform the test, plot the gain and output power curves, and compute the P
1dB
. This,
together with the linear gain, will be displayed in the text boxes to the right of the Start button. The results
can then be printed (the window as displayed will be printed) or saved as a text file by clicking Print or Save.
When measuring P
values from a file. The data is held in a simple text file with one line for each frequency point. The format
must be as follows:
using the frequency sweep plan, it is possible to read the input and output attenuation
1dB
Frequency (MHz), magnitude (dB), phase (degrees)
Note: The number of lines in the file must match the number of sweep points in the sweep plan.
6.11AM to PM conversion utility
This utility allows the measurement of the AM to PM conversion factor of a DUT. Generally it is used for
evaluating the linearity of active devices such as amplifiers. The utility is started from the main Utilities
menu, shown below:
Figure: The AM to PM measurement utility control window
In order to use this facility an S21 calibration (or S11+S21, or 12-term) must have been carried out. For best
results, some averaging (e.g. 16) should be used. Further, a second through calibration is suggested to
remove residual phase variations. The steps are summarized as follows.
AM to PM utility (calibration)
Perform a normal S21 calibration (or S11+S21, or 12-term); see left-hand connection diagram in Quick start
guide
Call up AM to PM Utility (window shown above)
Enter frequency required (Test Freq) in megahertz
Click Calibrate (connection as on left-hand side of figure below)
AM to PM utility (test)
Connect DUT with attenuators as shown on right hand side of the figure below
Enter attenuator values, input power at which result is required and measurement title
Power up DUT if necessary
Click Start
On completion of the AM to PM test, a graph of AM to PM as a function of input power at the DUT input will
be plotted. In addition, the AM to PM factor at the specified input power entered will be displayed in the text
box in the Measure section of the window.
Figure: Calibration (left) and test connections for AM to PM test
Note: For best AM-PM results apply some averaging (e.g. 16) and carry out an AM-PM calibration (left hand
side of figure). A ‘?’ will displayed if the requested P
for readout is outside the available range.
in
6.12Compare data utility
The compare data utility provides a quick and simple way to compare two sets of full S-parameter
measurements taking into account the instrument’s measurement uncertainty and optionally, the uncertainty
associated with the reference measurement. Typically this facility can be used to measure a verification
(reference) DUT and compare the measurement values produced by the PicoVNA 106 VNA with those
supplied with the verification DUT. This is a simple and quick way of determining the adequacy of the
calibration and calibration kit to be used.
The compare data utility can be found in the utility drop-down menu. This brings up the dialog shown below.
For the compare utility to work, you need to follow these steps:
Perform a full S-parameter calibration
Measure the reference DUT
Load the reference measurement of the DUT (supplied with the DUT) using Load Measurement (this
must be a full s-parameter measurement)
Launch the compare data utility
Load the PicoVNA 106 VNA uncertainty file (usually in the file DefUnc.dat)
Load the reference measurement uncertainty file (this may be ignored in most cases where reference
measurements are believed to be highly accurate)
Click on the ‘Compare’ button to perform the comparison and display the results
Data comparison dialo
Defining uncertainties
Measurement uncertainty is defined by means of text file as illustrated below. The definition is made up of
several segments. Each segment refers to reflection [REFLECTION] or transmission [TRANSMISSION] with
an entry for the applicable range in dB followed by the frequency range (in MHz). After the frequency range
entry, the magnitude uncertainty in dB is specified followed by the corresponding phase uncertainty in
degrees.
The uncertainty definition is made up of several reflection and transmission
se
ments. A reflection segment is highlighted above.
It is possible to define the uncertainty by a polynomial. To do this, follow the [MAGDB] keyword with the
keyword [POLY]. Then, the uncertainty can be define by means of 3 coefficients, say, K
, K1, and K2. The
0
uncertainty for given measured absolute magnitude value in dB, M, is given by:
The same approach can be used to defining the phase uncertainty. That is, add the keyword [POLY] after the
[PHASE] keyword.
The data compare utility resolves the total combined uncertainty as follows:
In the above, UI is the uncertainty associated with the PicoVNA 106 VNA and UR is that provided with the
reference DUT.
6.13Closing down the software
It is recommended that a formal shut down of the user interface window is carried out before the VNA is to
be switched off. This allows the calibration and status to be saved and the instrument’s log file to be
updated. The sequence is shown below:
Formally closing down the software saves the current calibration
It is recommended that the instrument is checked annually for safety (chassis grounding, fan operation,
clear ventilation grilles and operator markings) and compliance with the stated electrical specification. The
table below shows the parameters that should be checked as part of the calibration process. Note that the
ventilation inlets should be checked as described later.
A known mismatch at ports
1 and 2 (–16 dB or worse
return loss)
Mismatched attenuator (> 10
dB attenuation and –16 dB or
worse return loss)
51 points sweep
0.3–6000 MHz
1kHz BW
+3 dBm test level
51 points sweep
0.3–6000 MHz
1kHz BW
+3 dBm test level
12 term
12 term
12 term
We recommended that you compare the measured results with the values provided with the standards and
verify that they are within the combined uncertainty of the instrument and the provided measurements. The
frequency should be set to agree with those available(s) for the standard used. The recommended test
arrangement is shown below. The results should be within the instrument’s quoted uncertainty as detailed in
the following section. Allowance should also be made for the uncertainty of the standard reference values.
Figure: Performance verification arrangement
Tip: A data compare utility is provided in the PicoVNA 2 software that can be used to compare the
measurements, taking into account the uncertainty of the instrument.
7.1Measurement uncertainty
The measurement uncertainty figures below are based on calibration (12 term, insertable device, with –3
dBm test power and using 10 Hz bandwidth) using the premium PC3.5 mm calibration kits optionally
supplied with the instrument. The figures for S
less than 0.2. Similarly, the figures for S
and S22 assume the DUT has a value of S21 or S12 of less than 0.2.
11
and S12 assume that the DUT has a value of S11 or S22 of
21
Other external factors such as connector and cables effects are excluded.
Check that all ventilation grilles are clear of any debris, dust or any other material that may impede the flow
of air. Particularly, check the vents in the bottom panel of the instrument. It is advisable to brush these to
remove any gradual build up of dust.
Failure to clean the ventilation grilles may lead to overheating and eventual failure of the instrument.
Front panel connectors
Routinely inspect the Port 1 and Port 2 N-type connectors for signs of damage or dirt. Use connector-saver
adaptors (male to female through) where frequent connection and disconnection are likely.
The instrument’s performance specification is given below. Unless otherwise stated, the figures apply with
10 Hz resolution bandwidth, at –3 dBm test power, at an ambient temperature of 23 ± 1°C and 60minutes
after power up.
Measuring functions
Measuring parametersS11, S21, S22, S
P
(power at 1 dB gain compression)
1dB
AM-PM conversion factor
Error correction12 term
8 term (unknown through calibration)
S
(1 port correction)
11
(normalize, normalize + isolation)
S
21
(source match correction + normalize + isolation)
S
21
Averaging, smoothing, Hann and Kaiser–Bessel
filtering on time-domain measurements,
Electrical length compensation (manual)
Electrical length compensation (auto)
De-embed (2 embedding networks may be specified)
Impedance conversion
Display channels4 channels (CH1, CH2, CH3, CH4)
Traces2 traces / channel
Display formatsAmplitude (logarithmic and linear), phase, group
delay, VSWR, real, imaginary, Smith chart, polar, time
domain
Memory traceOne per channel
Limit lines6 segments per channel (overlap allowed)
Markers8 markers
Marker functionsNormal, ∆ marker, fixed marker, peak / min, 3 dB and
6 dB bandwidth
12
Signal source characteristics
Frequency range300 kHz to 6.02 GHz
Frequency setting resolution10 Hz
Frequency accuracy±10 ppm (23 ± 3°C)
Frequency temperature stability±0.5 ppm/°C (15 to 35°C)
Harmonics (–3 dBm output level)–20 dBc
Non-harmonic spurious (typical)–40 dBc
Phase noise (10 kHz)–90 dBc/Hz (0.3 MHz to 1000 MHz)
–80 dBc/Hz (1000 MHz to 4000 MHz)
–76 dBc/Hz (> 4000 MHz)
Output power+6 to –20 dBm (+3 to –20 dBm for F > 4GHz)
Power setting resolution0.1 dB (nominal)
Output power accuracy±2.0 dB
Reference input frequency10 MHz ±6 ppm
Reference input level0 ±3 dBm
Reference output level0 ±3 dBm
10 Hz bandwidth
16 averages
Test ports terminated as during isolation calibration
step
Dynamic range (dB)
BandTypMax
0.3 MHz to 10 MHz–110–100
10 MHz to 4 GHz–118–108
4 GHz to 6 GHz–110–100
See figure below
Bandwidth 20Hz
16 averages
Test ports terminated as during the isolation
calibration step. Isolation calibration refreshed as
described in 6.2.7.
Temperature stability (typical)0.02 dB/°C (f < 4 GHz)
0.04 dB/°C (f ≥ 4 GHz)
Trace noise (mdB RMS)
Full band
Test level 0dB
201 point sweep
BandwidthTypMax
10 kHz0.82
70 kHz35
140 kHz510
Test port characteristics
Load match (uncorrected)16 dB typ.
Source match (uncorrected)16 dB typ (uncorrected)
40 dB min (48 dB typical)
Directivity (corrected, using PC3.5 cal kit)40 dB min (47 dB typical)
Crosstalk (dB, corrected)
Test ports terminated with short circuits.
Value is average displayed noise level.
BandTypMax
0.3kHz–2MHz–110–90
2 MHz–4 GHz–110–90
4 GHz–6 GHz–100–90
Main test ports maximum input level
+10 dBm
(1 dB compression)
Main test ports maximum input level
+20 dBm
(no damage)
Main test ports connectorsType N (female)
Bias-T maximum current250 mA
Bias-T maximum DC voltage+15 V
Bias-T current protectionBuilt-in resettable fuse
Bias-T DC port connectorsSMB (female on front panel)
Sweep trigger input voltageLow: –0.1 to +1.0 V
Frequency range0.3 to 6020 MHz
Input power sweep range–20 to 0 dBm
Input power sweep step1 dB (nominal)
P1dB calculation method
2nd order curve fit
Display formatGraphical, gain and output power
Accuracy0.5 dB (typical)
AM to PM utility
Frequency range0.3 to 6020 MHz
Input power sweep range–20 to 0 dBm
Input power sweep step1 dB (nominal)
AM to PM point calculation method
2nd order curve fit
Display formatGraphical, phase conversion (deg / dB)
Accuracy (Port 2 power +5 to –20 dBm)1° (typical)
Signal generator utility
Frequency range0.3 to 6020 MHz
Output power–20 to +3 dBm
Setting resolution0.1 dB
Output power accuracy+2.0 dB max
Group delay
Range (180° maximum phase shift per frequency
step)
where ∆f is the aperture frequency
Aperture frequencyFrequency sweep step size
Accuracy
Data handling
Calibration dataStore / Recall on disk
Calibration kit dataStore / Recall on disk
Print measured data (graphics)To any printer installed on host PC
Save measured data (graphics)To disk
Measured dataStore on disk
Measured data (Touchstone format)Store on disk
Measured data (Touchstone format)Recall to memory trace from disk
Statement of Volatility: No user data, calibration data or user settings are stored on the device.
Miscellaneous
PC data interfaceUSB
PC minimum requirementsPentium 4 (3 GHz) or equivalent
1 GB RAM
200 MB hard disk storage on C: partition
Windows 7, 8 or 10
Display resolution of 1280 x 720
External dimensions (L x W x H)286 x 174 x 61 mm
Weight1.85 kg
Temperature range (operating)15 °C to 35 °C
Temperature range (storage)–20 °C to 50 °C
Humidity80% max. (non-condensing)
Power sourceDC, 12 to 15 V, 1.85 A max.
The product and accessories contain no user-serviceable parts. Repair, servicing and
calibration require specialized test equipment and must only be performed by Pico Technology
or an approved service provider.
SymptomPossible CauseSolution
Instrument does not power up
PicoVNA 2 software unable to
communicate with the instrument
Instrument sweeping but display not
refreshing
‘Last Calibration not found’ message
on power up
Diagnostics Tests (under Tools
menu) fail
Error reading data files
Power not applied
Incorrect supply
Driver not installed
Link interrupted
Data link interruptedRestart instrument and software
C:
\User\Public\Documents\PicoVNA
2 directory deleted or corrupted
Data corruptionRestart instrument and software.
Invalid format
Too many lines
Leading space(s)
Check DC connection
Check external supply
See Switching on
Restart instrument and software
Restore folder. Set up display and
calibrate. Exit the software using File> Exit menu command. This will save
the current calibration in a file named
defaultcal.cal.
Ensure that test cable used is in good
condition.
Check for correct format / ‘#’ line
Number of lines must be < 1000
Remove leading spaces from data
lines
Troubleshooting guide68
Diagnostics tests
It is possible to run self-check tests on the instrument. This facility (Diagnostic Tests) is available from the
Tools menu shown above. In order to complete the tests a low loss cable is required to link Port 1 to Port 2.
The tests carry out the following checks.
Synthesizers: test that they remain in lock over the frequency range
Test signal: test the level range and step size
Receiver levels: test that the receiver is operating at normal signal levels
Receiver crosstalk: test that raw crosstalk remains below limit
Receiver DC offset: test that this is at normal level
Figure: The Diagnostics Tests perform internal checks on key components
If any of the tests returns an error, check connectors and linking cable. If this does not resolve it, restart the
instrument and the software. After pressing reset, wait until the front-panel channel activity indicators have
stopped flashing to continue with the tests.
Calibration error terms and raw receiver data
The diagnostic tests dialog (figure above) also provides the facility for retrieving the calibration error terms
and raw receiver data. The latter can be helpful for users wishing to carry out their own calibration
procedure.
Back up/restore EEPROM
This facility allows the internal ROM (read-only memory) of the instrument to be backed up or restored. This
facility should only be required by service or repair personnel.
Pico Technology warrants upon delivery, and for a period of three years unless otherwise stated from the
date of delivery, that the Goods will be free from defects in material and workmanship.
Pico Technology shall not be liable for a breach of the warranty if the defect has been caused by fair wear
and tear, willful damage, negligence, abnormal working conditions or failure to follow Pico Technology's
spoken or written advice on the storage, installation, commissioning, use or maintenance of the Goods or (if
no advice has been given) good trade practice; or if the Customer alters or repairs such Goods without the
written consent of Pico Technology.
Calibration 4, 14, 38
Calibration for best dynamic range – minimizing the effect
of crosstalk 43
Calibration kit parameters 23
Calibration steps for all s-parameters measurements
(insertable DUT) 42
Calibration steps for all s-parameters measurements
(non-insertable DUT) 42
Calibration steps for S11 and S21 measurements 41
Calibration steps for S11 measurements 41
Calibration steps for S21 measurements 41
Closing the software 61
H
Humidity 3
I
Insertion loss/gain measurement 45
Installing the software 22
Introduction 10
L
Limit lines facility 35
Loading data 54
M
Main window 27
Maintenance
for performance 62
for safety 63
Matched termination with poor return loss or unmodeled
Short and Open 25
symbols 1
Saving data 54
Saving graphics 55
Servicing 4
Signal generator utility 56
S-parameters 11
Specifications 64
Status panel 36
Structure of the VNA 10
Sweep trigger output 37
Switching on the VNA 23
T
TDR
bandpass method 20
lowpass method 20
Temperature 3
Time domain measurements 46
Triggered sweep 37
Troubleshooting guide 68