Product specification
Replaces datasheet NE/SA5211 of 1995 Apr 26
IC19 Data Handbook
1998 Oct 07
Page 2
Philips SemiconductorsProduct specification
SYMBOL
PARAMETER
RATING
UNIT
SA521 1Transimpedance amplifier (180MHz)
DESCRIPTION
The SA521 1 is a 28kΩ transimpedance, wide-band, low noise
amplifier with differential outputs, particularly suitable for signal
recovery in fiber optic receivers. The part is ideally suited for many
other RF applications as a general purpose gain block.
FEA TURES
•Extremely low noise:
1.8pA Hz
•Single 5V supply
•Large bandwidth: 180MHz
•Differential outputs
•Low input/output impedances
•High power supply rejection ratio
•28kΩ differential transresistance
APPLICATIONS
•Fiber optic receivers, analog and digital
•Current-to-voltage converters
•Wide-band gain block
PIN CONFIGURATION
D Package
1
GND
2
2
GND
2
3
NC
4
I
IN
5
NC
6
V
CC1
78
V
CC2
TOP VIEW
Figure 1. Pin Configuration
•Medical and scientific Instrumentation
•Sensor preamplifiers
•Single-ended to differential conversion
•Low noise RF amplifiers
•RF signal processing
14
OUT (–)
13
GND
12
OUT (+)
11
GND
10
GND
9
GND
GND
SD00318
2
1
1
1
1
ORDERING INFORMATION
DESCRIPTIONTEMPERATURE RANGEORDER CODEDWG #
14-Pin Plastic Small Outline (SO) Package-40 to +85°CSA5211DSOT108-1
ABSOLUTE MAXIMUM RATINGS
V
CC
T
A
T
J
T
STG
P
D MAX
I
IN MAX
θ
JA
NOTES:
1. Maximum dissipation is determined by the operating ambient temperature and the thermal resistance:
=125°C/W
θ
2. The use of a pull-up resistor to V
JA
Power supply6V
Operating ambient temperature range-40 to +85°C
Operating junction temperature range-55 to +150°C
Storage temperature range-65 to +150°C
Power dissipation, TA=25°C (still-air)
Maximum input current
2
1
1.0W
5mA
Thermal resistance125°C/W
, for the PIN diode is recommended.
CC
1998 Oct 07853-1799 20142
2
Page 3
Philips SemiconductorsProduct specification
SA521 1Transimpedance amplifier (180MHz)
RECOMMENDED OPERATING CONDITIONS
SYMBOLPARAMETERRATINGUNIT
V
CC
T
A
T
J
DC ELECTRICAL CHARACTERISTICS
Min and Max limits apply over operating temperature range at VCC=5V, unless otherwise specified. Typical data apply at VCC=5V and TA=25°C.
SYMBOL
V
IN
V
±
O
V
OS
I
CC
I
OMAX
I
IN
I
IN MAX
NOTES:
1. Test condition: output quiescent voltage variation is less than 100mV for 3mA load current.
Input bias voltage0.550.81.00V
Output bias voltage2.73.43.7V
Output offset voltage0130mV
Supply current202631mA
Output sink/source current
Input current
(2% linearity)
Maximum input current
overload threshold
Supply voltage4.5 to 5.5V
Ambient temperature range-40 to +85°C
Junction temperature range-40 to +105°C
PARAMETERTEST CONDITIONSMinTypMaxUNIT
1
Test Circuit 8,
Procedure 2
Test Circuit 8,
Procedure 4
34mA
±20±40µA
±30±60µA
1998 Oct 07
3
Page 4
Philips SemiconductorsProduct specification
1
SA521 1Transimpedance amplifier (180MHz)
AC ELECTRICAL CHARACTERISTICS
Typical data and Min and Max limits apply at VCC=5V and TA=25°C
Transimpedance amplifiers have been widely used as the
preamplifier in fiber-optic receivers. The SA5211 is a wide bandwidth
(typically 180MHz) transimpedance amplifier designed primarily for
input currents requiring a large dynamic range, such as those
produced by a laser diode. The maximum input current before
output stage clipping occurs at typically 50µA. The SA5211 is a
bipolar transimpedance amplifier which is current driven at the input
and generates a differential voltage signal at the outputs. The
forward transfer function is therefore a ratio of the differential output
voltage to a given input current with the dimensions of ohms. The
main feature of this amplifier is a wideband, low-noise input stage
which is desensitized to photodiode capacitance variations. When
connected to a photodiode of a few picoFarads, the frequency
response will not be degraded significantly. Except for the input
stage, the entire signal path is differential to provide improved
power-supply rejection and ease of interface to ECL type circuitry. A
block diagram of the circuit is shown in Figure 11. The input stage
(A1) employs shunt-series feedback to stabilize the current gain of
the amplifier. The transresistance of the amplifier from the current
source to the emitter of Q
feedback resistor, R
and emitter followers (A3 and A4) is about two. Therefore, the
differential transresistance of the entire amplifier , R
V
(diff)
R
OUT
+
T
I
IN
The single-ended transresistance of the amplifier is typically 14.4kΩ.
The simplified schematic in Figure 12 shows how an input current is
converted to a differential output voltage. The amplifier has a
single input for current which is referenced to Ground 1. An input
current from a laser diode, for example, will be converted into a
voltage by the feedback resistor R
of the open loop gain of the circuit, A
minimizes loading on Q1. The transistor Q4, resistor R7, and V
provide level shifting and interface with the Q15– Q16 differential
pair of the second stage which is biased with an internal reference,
V
. The differential outputs are derived from emitter followers Q
B2
which are biased by constant current sources. The collectors of
Q
12
is approximately the value of the
3
=14.4kΩ. The gain from the second stage (A2)
F
is
T
+ 2RF+ 2(14.4K) + 28.8kW
. The transistor Q1 provides most
F
≈70. The emitter follower Q
VOL
B1
11
(ns)
– Q12 are bonded to an external pin, V
Q
11
SD00334
, in order to reduce
CC2
the feedback to the input stage. The output impedance is about 17Ω
single-ended. For ease of performance evaluation, a 33Ω resistor is
used in series with each output to match to a 50Ω test system.
BANDWIDTH CALCULATIONS
The input stage, shown in Figure 13, employs shunt-series feedback
to stabilize the current gain of the amplifier. A simplified analysis can
determine the performance of the amplifier. The equivalent input
capacitance, CIN, in parallel with the source, IS, is approximately
7.5pF, assuming that C
capacitance.
Since the input is driven by a current source the input must have a
low input resistance. The input resistance, R
incremental input voltage, V
and can be calculated as:
V
R
IN
+
IN
+
I
IN
More exact calculations would yield a higher value of 200Ω.
Thus C
and RIN will form the dominant pole of the entire amplifier;
IN
f
*3dB
Assuming typical values for RF = 14.4kΩ, RIN = 200Ω, CIN = 4pF
+
f
*3dB
The operating point of Q1, Figure 12, has been optimized for the
lowest current noise without introducing a second dominant pole in
the pass-band. All poles associated with subsequent stages have
been kept at sufficiently high enough frequencies to yield an overall
single pole response. Although wider bandwidths have been
achieved by using a cascade input stage configuration, the present
2
solution has the advantage of a very uniform, highly desensitized
frequency response because the Miller effect dominates over the
external photodiode and stray capacitances. For example, assuming
a source capacitance of 1pF, input stage voltage gain of 70, R
–
=0 where CS is the external source
S
, to the corresponding input current, I
IN
R
F
1 ) A
+
2p R
1
2p 4pF 200W
VOL
+
1
INCIN
+ 200MHz
14.4K
71
+ 203W
, is the ratio of the
IN
IN
=
IN
1998 Oct 07
13
Page 14
Philips SemiconductorsProduct specification
SA521 1Transimpedance amplifier (180MHz)
60Ω then the total input capacitance, C
= 4 pF which will lead to
IN
only a 12% bandwidth reduction.
NOISE
Most of the currently installed fiber-optic systems use non-coherent
transmission and detect incident optical power. Therefore, receiver
noise performance becomes very important. The input stage
achieves a low input referred noise current (spectral density) of
2.9pA/√Hz
. The transresistance configuration assures that the
external high value bias resistors often required for photodiode
biasing will not contribute to the total noise system noise. The
equivalent input
quiescent current of Q
noise current is strongly determined by the
RMS
, the feedback resistor RF, and the
1
bandwidth; however, it is not dependent upon the internal
Miller-capacitance. The measured wideband noise was 41nA RMS
in a 200MHz bandwidth.
DYNAMIC RANGE CALCULATIONS
The electrical dynamic range can be defined as the ratio of
maximum input current to the peak noise current:
Electrical dynamic range, D
I
= 60µA and a wideband noise of IEQ=41nA
INMAX
external source capacitance of C
(Max. input current)
D
+
E
(Peak noise current)
DE(dB) + 20log
DE(dB) + 20log
(2Ǹ41 10*9)
(60mA)
(58nA)
In order to calculate the optical dynamic range the incident optical
power must be considered.
For a given wavelength λ;
Energy of one Photon =
Where h=Planck’s Constant = 6.6 ×10
c = speed of light = 3 × 10
c / λ = optical frequency
No. of incident photons/sec=
No. of generated electrons/sec =
where η = quantum efficiency
no. of generated electron hole paris
+
no. of incident photons
P
NI + h @
hs
@ e Amps (Coulombsńsec.)
l
where e = electron charge = 1.6 × 10
h@e
Responsivity R =
hs
l
I + P @ R
, in a 200MHz bandwidth assuming
E
= 1pF.
S
*6
(60 @ 10
)
+ 60dB
hc
watt sec (Joule)
l
-34
Joule sec.
8
m/sec
P
where P=optical incident power
hs
l
P
hs
h @
l
-19
Coulombs
Amp/watt
RMS
for an
Assuming a data rate of 400 Mbaud (Bandwidth, B=200MHz), the
noise parameter Z may be calculated as:
I
EQ
Z +
qB
+
(1.6 @ 10
where Z is the ratio of
*9
41 @ 10
*19
)(200 @ 106)
noise output to the peak response to a
RMS
1
+ 1281
single hole-electron pair. Assuming 100% photodetector quantum
efficiency, half mark/half space digital transmission, 850nm
lightwave and using Gaussian approximation, the minimum required
optical power to achieve 10
+ 12
hc
l
P
avMIN
-9
BER is:
BZ+ 12 @ 2.3 @ 10
*19
200 @ 106(1281) + 719nW +*31.5dBm
+ 1139nW +*29.4dBm
where h is Planck’s Constant, c is the speed of light, λ is the
wavelength. The minimum input current to the SA5211, at this input
power is:
*9
@ 1.6 @ 10
@
*19
Joule
sec
@ q + I
*19
I
avMIN
+ qP
avMIN
+
l
hc1Joule
707 @ 10
2.3 @ 10
= 500nA
Choosing the maximum peak overload current of I
This represents the maximum limit attainable with the SA5211
operating at 200MHz bandwidth, with a half mark/half space digital
transmission at 850nm wavelength.
1998 Oct 07
14
Page 15
Philips SemiconductorsProduct specification
SA521 1Transimpedance amplifier (180MHz)
V
CC1
R
1
R
3
R
12
R
13
V
CC2
Q
INPUT
GND
PHOTODIODE
2
Q
Q
1
1
3
R
2
R
5
R
Figure 12. Transimpedance Amplifier
V
CC
I
C1
R1
INPUT
I
IN
V
IN
I
B
Q1
I
F
R
F
Q2
R3
Q3
R2
V
EQ3
R4
SD00329
Figure 13. Shunt-Series Input Stage
APPLICATION INFORMATION
Package parasitics, particularly ground lead inductances and
parasitic capacitances, can significantly degrade the frequency
response. Since the SA5211 has differential outputs which can feed
back signals to the input by parasitic package or board layout
capacitances, both peaking and attenuating type frequency
response shaping is possible. Constructing the board layout so that
Ground 1 and Ground 2 have very low impedance paths has
produced the best results. This was accomplished by adding a
ground-plane stripe underneath the device connecting Ground 1,
Q
4
+
Q
15
R
14
R
7
4
GND
Q
16
R
15
VB2
2
Q
11
Q
12
OUT–
+
OUT+
SD00328
Pins 8–11, and Ground 2, Pins 1 and 2 on opposite ends of the
SO14 package. This ground-plane stripe also provides isolation
between the output return currents flowing to either V
or Ground
CC2
2 and the input photodiode currents to flowing to Ground 1. Without
this ground-plane stripe and with large lead inductances on the
board, the part may be unstable and oscillate near 800MHz. The
easiest way to realize that the part is not functioning normally is to
measure the DC voltages at the outputs. If they are not close to their
quiescent values of 3.3V (for a 5V supply), then the circuit may be
oscillating. Input pin layout necessitates that the photodiode be
physically very close to the input and Ground 1. Connecting Pins 3
and 5 to Ground 1 will tend to shield the input but it will also tend to
increase the capacitance on the input and slightly reduce the
bandwidth.
As with any high-frequency device, some precautions must be
observed in order to enjoy reliable performance. The first of these is
the use of a well-regulated power supply. The supply must be
capable of providing varying amounts of current without significantly
changing the voltage level. Proper supply bypassing requires that a
good quality 0.1µF high-frequency capacitor be inserted between
V
CC1
and V
, preferably a chip capacitor, as close to the package
CC2
pins as possible. Also, the parallel combination of 0.1µF capacitors
with 10µF tantalum capacitors from each supply, V
CC1
and V
CC2
, to
the ground plane should provide adequate decoupling. Some
applications may require an RF choke in series with the power
supply line. Separate analog and digital ground leads must be
maintained and printed circuit board ground plane should be
employed whenever possible.
Figure 14 depicts a 50Mb/s TTL fiber-optic receiver using the
BPF31, 850nm LED, the SA5211 and the SA5214 post amplifier.
1998 Oct 07
15
Page 16
Philips SemiconductorsProduct specification
SA521 1Transimpedance amplifier (180MHz)
+V
CC
47µF
C1
GND
C2
CC
C9
R3
47k
C11
.01µF
.01µF
pin(s).
D1
LED
100pF
C13
V
LED
1
C
2
PKDET
THRESH
3
GND
A
4
FLAG
5
JAM
6
V
CCD
7
V
CCA
8
GND
D
9
TTL
1011
OUT
(TTL)
OUT
IN
IN
C
C
OUT
IN
NE5214
OUT
IN
R
HYST
R
PKDET
1B
1A
AZP
AZN
1B
8B
1A
8A
R2
220
L2
10µH
C10
µF
10
C12
L3
10µH
10µF
NOTE:
The NE5210/NE5217 combination can operate at data rates in excess of 100Mb/s NRZ
The capacitor C7 decreases the NE5210 bandwidth to improve overall S/N ratio in the DC–50MHz band, but does create extra high frequency noise
on the NE5210 V
.01µF
C4
.01µF
10µH
C7
20
100pF
19
C8
18
17
0.1µF
16
15
14
13
12
GND
GND
9
GND
10
GND
11
OUT
12
13
GND
OUT
14
R4
4k
V
V
NE5210
GND
GND
CC
CC
NC
I
IN
NC
78
6
5
4
3
2
1
Figure 14. A 50Mb/s Fiber Optic Receiver
L1
10µF
R1
100
C3
1.0µF
.01µF
BPF31
OPTICAL
INPUT
SD00330
C5
C6
1998 Oct 07
16
Page 17
Philips SemiconductorsProduct specification
SA521 1Transimpedance amplifier (180MHz)
GND 2
INPUT
NC
NC
1
GND 2
2
3
4
5
14
OUT (–)
13
GND 2
12
OUT (+)
GND 1
11
10
GND 1
VCC1
6
ECN No.: 06027
1992 Mar 13
VCC 2
78
Figure 15. SA5211 Bonding Diagram
Die Sales Disclaimer
Due to the limitations in testing high frequency and other parameters
at the die level, and the fact that die electrical characteristics may
shift after packaging, die electrical parameters are not specified and
die are not guaranteed to meet electrical characteristics (including
temperature range) as noted in this data sheet which is intended
only to specify electrical characteristics for a packaged device.
All die are 100% functional with various parametrics tested at the
wafer level, at room temperature only (25°C), and are guaranteed to
be 100% functional as a result of electrical testing to the point of
wafer sawing only. Although the most modern processes are
utilized for wafer sawing and die pick and place into waffle pack
1998 Oct 07
GND 1
9
GND 1
SD00488
carriers, it is impossible to guarantee 100% functionality through this
process. There is no post waffle pack testing performed on
individual die.
Since Philips Semiconductors has no control of third party
procedures in the handling or packaging of die, Philips
Semiconductors assumes no liability for device functionality or
performance of the die or systems on any die sales.
Although Philips Semiconductors typically realizes a yield of 85%
after assembling die into their respective packages, with care
customers should achieve a similar yield. However, for the reasons
stated above, Philips Semiconductors cannot guarantee this or any
other yield on any die sales.
17
Page 18
Philips SemiconductorsProduct specification
SA521 1Transimpedance amplifier (180MHz)
SO14: plastic small outline package; 14 leads; body width 3.9 mmSOT108-1
1998 Oct 07
18
Page 19
Philips SemiconductorsProduct specification
SA521 1Transimpedance amplifier (180MHz)
NOTES
1998 Oct 07
19
Page 20
Philips SemiconductorsProduct specification
SA521 1Transimpedance amplifier (180MHz)
Data sheet status
Data sheet
status
Objective
specification
Preliminary
specification
Product
specification
Product
status
Development
Qualification
Production
Definition
This data sheet contains the design target or goal specifications for product development.
Specification may change in any manner without notice.
This data sheet contains preliminary data, and supplementary data will be published at a later date.
Philips Semiconductors reserves the right to make chages at any time without notice in order to
improve design and supply the best possible product.
This data sheet contains final specifications. Philips Semiconductors reserves the right to make
changes at any time without notice in order to improve design and supply the best possible product.
[1]
[1] Please consult the most recently issued datasheet before initiating or completing a design.
Definitions
Short-form specification — The data in a short-form specification is extracted from a full data sheet with the same type number and title. For
detailed information see the relevant data sheet or data handbook.
Limiting values definition — Limiting values given are in accordance with the Absolute Maximum Rating System (IEC 134). Stress above one
or more of the limiting values may cause permanent damage to the device. These are stress ratings only and operation of the device at these or
at any other conditions above those given in the Characteristics sections of the specification is not implied. Exposure to limiting values for extended
periods may affect device reliability.
Application information — Applications that are described herein for any of these products are for illustrative purposes only. Philips
Semiconductors make no representation or warranty that such applications will be suitable for the specified use without further testing or
modification.
Disclaimers
Life support — These products are not designed for use in life support appliances, devices or systems where malfunction of these products can
reasonably be expected to result in personal injury . Philips Semiconductors customers using or selling these products for use in such applications
do so at their own risk and agree to fully indemnify Philips Semiconductors for any damages resulting from such application.
Right to make changes — Philips Semiconductors reserves the right to make changes, without notice, in the products, including circuits, standard
cells, and/or software, described or contained herein in order to improve design and/or performance. Philips Semiconductors assumes no
responsibility or liability for the use of any of these products, conveys no license or title under any patent, copyright, or mask work right to these
products, and makes no representations or warranties that these products are free from patent, copyright, or mask work right infringement, unless
otherwise specified.
Philips Semiconductors
811 East Arques Avenue
P.O. Box 3409
Sunnyvale, California 94088–3409
Telephone 800-234-7381
Copyright Philips Electronics North America Corporation 1998
All rights reserved. Printed in U.S.A.
Date of release: 10-98
Document order number:9397 750 04624
1998 Oct 07
20
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