Identical X and Y amplitude/timing responses
Adjustable gain scaling, α
DC-coupled throughout, 3 dB bandwidth of 2 GHz
Fully differential inputs, may be used single ended
Low noise, high linearity
Accurate, temperature stable gain scaling
Single-supply operation (4.5 V to 5.5 V @ 130 mA)
Low current power-down mode
16-lead LFCSP
APPLICATIONS
Wideband multiplication and summing
High frequency analog modulation
Adaptive antennas (diversity/phased array)
Square-law detectors and true rms detectors
Accurate polynomial function synthesis
DC capable VGA with very fast control
GENERAL DESCRIPTION
The ADL5391 draws on three decades of experience in
advanced analog multiplier products. It provides the same
general mathematical function that has been field proven to
provide an exceptional degree of versatility in function synthesis.
VW = α × (VX × VY)/ 1 V + V
The most significant advance in the ADL5391 is the use of a
new multiplier core architecture, which differs markedly from
the conventional form that has been in use since 1970. The
conventional structure that employs a current mode, translinear
core is fundamentally asymmetric with respect to the X and Y
inputs, leading to relative amplitude and timing misalignments
that are problematic at high frequencies. The new multiplier
core eliminates these misalignments by offering symmetric
signal paths for both X and Y inputs. The Z input allows a signal
to be added directly to the output. This can be used to cancel a
carrier or to apply a static offset voltage.
The fully differential X, Y, and Z input interfaces are operational
over a ±2 V range, and they can be used in single-ended fashion.
The user can apply a common mode at these inputs to vary
from the internally set V
= α × (VX × VY)/1 V + VZ
W
Z
/2 down to ground. If these inputs
POS
Multiplier
ADL5391
FUNCTIONAL BLOCK DIAGRAM
YMNS YPLSGADJ
XPLS
XMNS
ENBL
VMID
COMM VPOS
ADL5391
W = αXY/1V+Z
Figure 1.
are ac-coupled, their nominal voltage will be V
interfaces each present a differential 500 Ω input impedance up to
approximately 700 MHz, decreasing to 50 Ω at 2 GHz. The gain
scaling input, GADJ, can be used for fine adjustment of the gain
scaling constant (α) about unity.
The differential output can swing ±2 V about the V
common-mode and can be taken in a single-ended fashion as
well. The output common mode is designed to interface directly
to the inputs of another ADL5391. Light dc loads can be ground
referenced; however, ac-coupling of the outputs is recommended
for heavy loads.
The ENBL pin allows the ADL5391 to be disabled quickly to a
standby mode. It operates off supply voltages from 4.5 V to
5.5 V while consuming approximately 130 mA.
The ADL5391 is fabricated on Analog Devices proprietary, high
performance, 65 GHz, SOI complementary, SiGe bipolar IC
process. It is available in a 16-lead, Pb-free, LFCSP and operates
over a −40°C to +85°C temperature range. Evaluation boards
are available.
ZMNS
ZPLS
WPLS
WMNS
06059-001
/2. These input
POS
/2
POS
Rev. 0
Information furnished by Analog Devices is believed to be accurate and reliable. However, no
responsibility is assumed by Anal og Devices for its use, nor for any infringements of patents or ot her
rights of third parties that may result from its use. Specifications subject to change without notice. No
license is granted by implication or otherwise under any patent or patent rights of Analog Devices.
Trademarks and registered trademarks are the property of their respective owners.
= 5 V, TA = 25°C, ZL = 50 Ω differential, ZPLS = ZMNS = open, GADJ = open, unless otherwise noted. Transfer function: W =
POS
XY/1 V + Z, common mode internally set to 2.5 V nominal.
Table 1.
Parameter Conditions Min Typ Max Unit
MULTIPLICAND INPUTS (X, Y) XPLS, XMNS, YPLS, YMNS
Differential Voltage Range Differential, common mode = 2.5 V 2 V p-p
Common-Mode Range For full differential range 0 2.5 V
Input Offset Voltage DC 20 mV
vs. Temperature −40°C to +85°C ±20 mV
Differential Input Impedance f = dc 500 Ω
f = 2 GHz 150 Ω
Fundamental Feedthrough, X or Y
f = 1 GHz −35 dB
Gain X = 50 MHz and 0 dBm, Y = 1 V 0.5 dB
X = 1 GHz and 0 dBm, Y = 1 V −1.33 dB
DC Linearity X to output, Y = 1 V 1 % FS
Scale Factor X = Y = 1 V 1 V/V
CMRR ±1 V p-p, Y = 1 V, f = 50 MHz 42.1 dB
SUMMING INPUT (Z) ZPLS, ZMNS
Differential Voltage Range Common mode from 2.5 V down to COMM 2 V p-p
Common-Mode Range For full differential range 0 2.5 V
Gain From Z to W, f ≤ 10 MHz, 0 dBm, X = Y = 1 V 0.1 dB
Differential Input Impedance f = dc 500 Ω
f = 2 GHz 150 Ω
OUTPUTS (W) WPLS, WMNS
Differential Voltage Range No external common mode ±2 V
Common-Mode Output V
Output Noise Floor X = Y = 1 V dc f = 1 MHz −133 dBm/Hz
f = 1 GHz −133 dBm/Hz
X = Y = 0 f = 1 MHz −138 dBm/Hz
f = 1 GHz −138 dBm/Hz
Output Noise Voltage Spectral Density X = Y = 0, f = 1 MHz 26.7 nV/√Hz
Output Offset Voltage Z = 0 V differential
vs. Temperature ±19 mV
Differential Output Impedance f = dc 0 Ω
f = 200 MHz 75 Ω
f = 2 GHz 500 Ω
DYNAMIC CHARACTERISTICS
Frequency Range X, Y, Z to W 0 2 GHz
Slew Rate W from −2.0 V to +2.0 V, 150 Ω 8800 V/μs
Settling Time X stepped from −1 V to +1 V, Z = 0 V, 150 Ω 2.1 ns
Second Harmonic Distortion X (Y) = 0 dBm, Y (X) = 1 V, fund = 10 MHz −60 dBc
Fund = 200 MHz −51 dBc
Third Harmonic Distortion X (Y) = 0 dBm, Y (X) = 1 V, fund = 10 MHz −61.5 dBc
Fund = 200 MHz −51.6 dBc
f = 50 MHz, X (Y) = 0 V, Y (X) = 0 dBm, relative to
condition where X (Y) = 1 V
−42 dB
− 2.5 V
POS
19 mV
Rev. 0 | Page 3 of 16
Page 4
ADL5391
Parameter Conditions Min Typ Max Unit
OIP3
f1= 49 MHz, f = 50 MHz 26.5 dBm
f1 = 999 MHz, f2 = 1 GHz 14 dBm
OIP2 f1 = 49 MHz, f = 50 MHz 45.5 dBm
f1 = 999 MHz, f2 = 1 GHz 28 dBm
Output 1 dB Compression Point X (Y) to W, Y (X) = 1 V, 50 MHz 15.1 dBm
1 GHz 13.2 dBm
Group Delay 200 MHz 0.5 ns
1 GHz 0.7 ns
Differential Gain Error, X/Y f = 3.58 MHz 2.7 %
Differential Phase Error, X/Y f = 3.58 MHz 0.23 Degrees
GAIN TRIMMING (α) GADJ
Nominal Bias Unconnected 1.12 V
Input Range 0 2 V
Gain Adjust Range Input 0 V to 2 V 9.5 dB
REFERENCE VOLTAGE VMID V
Source Current Common-mode for X, Y, Z = 2.5 V 50 mA
POWER AND ENABLE V
Supply Voltage Range 4.5 5.5 V
Total Supply Current Common-mode for X, Y, Z = 2.5 V 135 mA
Disable Current ENBL = 0 V 7.5 mA
Disable Threshold High to Low 1.5 V
Enable Response Time
Disable Response Time
Two-tone IP3 test; X (Y) = 100 mV p-p/tone
(−10 dBm into 50 Ω), Y (X) = 1
, COMM, ENBL
POS
Delay following high-to-low transition until device
meets full specifications
Delay following low-to-high transition until device
produces full attenuation
/2 V
POS
150 ns
50 ns
Rev. 0 | Page 4 of 16
Page 5
ADL5391
ABSOLUTE MAXIMUM RATINGS
Table 2.
Parameter Rating
Supply Voltage V
ENBL 5.5 V
XPLS, XMNS, YPLS, YMNS, ZPLS, ZMNS V
GADJ V
Internal Power Dissipation 800 mW
θJA (With Pad Soldered to Board) 73°C/W
Maximum Junction Temperature 150°C
Operating Temperature Range −40°C to +85°C
Storage Temperature Range −65°C to +150°C
Lead Temperature (Soldering 60 sec) 300°C
5.5 V
POS
POS
POS
ESD CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily accumulate on the
human body and test equipment and can discharge without detection. Although this product features
proprietary ESD protection circuitry, permanent damage may occur on devices subjected to high energy
electrostatic discharges. Therefore, proper ESD precautions are recommended to avoid performance
degradation or loss of functionality.
Stresses above those listed under Absolute Maximum Ratings
may cause permanent damage to the device. This is a stress
rating only; functional operation of the device at these or any
other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute
maximum rating conditions for extended periods may affect
device reliability.
Rev. 0 | Page 5 of 16
Page 6
ADL5391
PIN CONFIGURATION AND FUNCTION DESCRIPTIONS
NBL
XPLS
XMNS
VMID
E
13
14
16
15
PIN 1
INDICATO R
1COMM
2VPOS
ADL5391
3VPOS
4VPOS
5
6
PLS
MNS
W
W
Figure 2. Pin Configuration
Table 3. Pin Function Descriptions
Pin No. Mnemonic Description
1, 7 COMM Device Common. Connect via lowest possible impedance to external circuit common.
2 to 4 V
POS
Positive Supply Voltage. 4.5 V to 5.5 V.
5, 6 WPLS, WMNS Differential Outputs.
8 GADJ Denominator Scaling Input.
9, 10 ZMNS, ZPLS Differential Intercept Inputs. Must be ac-coupled. Differential impedance 50 Ω nominal.
11, 12 YPLS, YMNS Differential X-Multiplicand Inputs.
13, 14 XPLS, XMNS Differential Y-Multiplicand Inputs.
15 ENBL Chip Enable. High to enable.
16 VMID V
/2 Reference Output. Connect decoupling capacitor to circuit common.
POS
12 YMNS
11 YPLS
10 ZPLS
9ZMNS
8
7
GADJ
COMM
06059-002
Rev. 0 | Page 6 of 16
Page 7
ADL5391
V
V
TYPICAL PERFORMANCE CHARACTERISTICS
GADJ = open.
3.0
2.5
2.0
1.5
1.0
)
0.5
DC
(
0
DIFF
–0.5
W
–1.0
–1.5
–2.0
–2.5
–3.0
–2.5 –2.0 –1.5 –1.0 –0.500.51.01.5 2.0 2.5
Y = –2
Y = –1
Y = 0
Y = +1
Y = +2
X
(VDC)
DIFF
Figure 3. Full Range DC Cross Plots
0.20
06059-007
14
12
10
8
6
4
2
0
–2
GAIN (dB)
–4
–6
–8
–10
–12
–14
5
195
100
290
385
480
575
955
860
765
670
FREQUENCY (MHz)
1150
1050
1620
1530
1430
1340
1240
200
150
100
50
–0
–50
–100
–150
–200
2000
1910
1810
1720
Figure 6. Gain and Phase vs. Frequency of X Swept and Y = 1 V, Z = 0 V,
P
= 0 dBm
IN
4
200
PHASE (Degrees)
06059-010
0.15
0.10
0.05
)
DC
(
0
DIFF
W
–0.05
–0.10
–0.15
–0.20
–0.20 –0.15 –0.10 –0.0500.050.100.150.20
Y = –2
Y = –1
Y = 0
Y = +1
Y = +2
X
DIFF
(VDC)
Figure 4. Magnified DC Cross Plots
2.5
2.0
1.5
GAIN (V/V)
1.0
3
2
1
0
GAIN (dB)
–1
–2
–3
–4
1
06059-008
110
220
330
440
FREQUENCY (MHz)
550
660
700
880
990
1100
150
100
50
–0
–50
PHASE (Degrees)
–100
–150
–200
1200
1300
06059-011
Figure 7. Gain and Phase vs. Frequency of Z Inputs, X = 0 V, Y = 0 V,
P
= 0 dBm
IN
2.0
1.5
1.0
0.5
(V)
0
OUTPUT
W
–0.5
X ± INPUT = 1.0V p- p, @ 200MHz
Y ± INPUT = 1. 0V DC DIFFE RENTIAL
0.5
0
–1.02.01.51.00.50–0.5
GADJ (VDC)
Figure 5. Gain vs. GADJ (X = Y = 1)
06059-009
–1.0
–1.5
–2.0
24.533.532.531.530.529.528.527. 526.525.5
TIME (ns)
Figure 8. Large Signal Pulse Response
06059-013
Rev. 0 | Page 7 of 16
Page 8
ADL5391
V
V
(V)
OUTPUT
W
0.20
0.15
0.10
0.05
–0.05
–0.10
–0.15
X ± INPUT = ±100mV p-p, @ 200MHz
Y ± INPUT = 1.0V DC DIFFERENTIAL
0
30
25
20
Y = 1
15
OIP3 (dBm)
10
5
Y = 0.5
–0.20
24.532.531.530.529.528.527.526.525. 5
TIME (ns)
06059-014
Figure 9. Small Signal Pulse Response
10MHz
10dBm/DIV
30MHz
20MHz
10dBm/DIV
200MHz
400MHz
600MHz
06059-094
Figure 10. Harmonic Distortion at 10 MHz and 200 MHz;
0 dBm Input to X (Y) Channels
28
26
24
)
DC
22
(
20
OFFSET
18
16
AVERAGE V
14
12
10
–40–151035608
TEMPERATURE ( °C)
5
06059-015
Figu re 11. X ( Y) Offset Drift vs. Temperature
0
02
FREQUENCY (M Hz)
15001000500
000
06059-016
Figure 12. OIP3 vs. Frequency
Pin 0 dBm, Y = 1 V dc, 0.5 V dc
0.05
0.04
)
DC
(
DIFF
W
0.03
0.02
0.01
–0.01
–0.02
–0.03
–0.04
–0.05
0
–0.050.050.040.030.020. 010–0.01–0.02–0.03–0.04
Y
(VDC)
DIFF
+85°C, X = +1
+85°C, X = –1
–40°C, X = –1
–40°C, X = +1
+25°C, X = –1
+25°C, X = +1
06059-021
Figure 13. Z (W) Offset Over Temperature
45
X = 0V, Y = 1V
40
X = Y = 1V
35
30
SND (nV/ Hz)
25
20
15
FREQUENCY (M Hz)
X = Y = 0V
2000200 400 600 800 1000 1200 1400 1600 1800
06059-019
Figure 14. Noise vs. Frequency
Rev. 0 | Page 8 of 16
Page 9
ADL5391
S22 SE
1.00UFS
S11 DIFF
1.000
201.0000.654 U–36.340 DEG
1001.0000.594 U–92.533 DEG
1901.0000.531 U–94.448 DEG
201.0000.800 U–17.218 DEG
2001.0000.564 U–58.167 DEG
Figure 15. Input S11
S11 SE
3001.000
1.00UFS
S22 DIFF
1.000
201.0000.947 U+170.736 DEG
1001.0000.569 U+58.257 DEG
1901.0000.597 U–69.673 DEG
201.0000.905 U+157.308 DEG
06059-017
2001.0000.663 U–39.468 DEG
3001.000
06059-018
Figure 16. Output S22
Rev. 0 | Page 9 of 16
Page 10
ADL5391
GENERAL DESCRIPTION
BASIC THEORY
The multiplication of two analog variables is a fundamental
signal processing function that has been around for decades.
By convention, the desired transfer function is given by
W = αXY/U + Z (1)
where:
X and Y are the multiplicands.
U is the multiplier scaling factor.
α is the multiplier gain.
W is the product output.
Z is a summing input.
All the variables and the scaling factor have the dimension of volts.
In the past, analog multipliers, such as the
implemented almost exclusively with a Gilbert Cell topology
or a close derivative. The inherently asymmetric signal paths
for X and Y inevitably create amplitude and delay imbalances
between X and Y. In the ADL5391, the novel multiplier core
provides absolute symmetry between X and Y, minimizing
scaling and phasing differences inherent in the Gilbert Cell.
The simplified block diagram of the ADL5391 shows a main
multiplier cell that receives inputs X and Y and a second
multiplier cell in the feedback path around an integrating
buffer. The inputs to this feedback multiplier are the difference
of the output signal and the summing input, W − Z, and the
internal scaling reference, U. At dc, the integrating buffer
ensures that the output of both multipliers is exactly 0, therefore
(W − Z)xU = XY, or W = XY/U + Z (2)
By using a feedback multiplier that is identical to the main
multiplier, the scaling is traced back solely to U, which is
an accurate reference generated on-chip. As is apparent in
Equation 2, noise, drift, or distortion that is common to both
multipliers is rejected to first-order because the feedback
multiplier essentially compensates the impairments generated
in the main multiplier.
The scaling factor, U, is fixed by design to 1.12 V. However, the
multiplier gain, α, can be adjusted by driving the GADJ pin with
a voltage ranging from 0 V to 2 V. If left floating, then α = 1 or
0 dB, and the overall scaling is simply U = 1 V. For VGADJ = 0 V,
the gain is lowered by approximately 4 dB; for VGADJ = 2 V,
the gain is raised by approximately 6 dB.
relationship between α(V/V) and VGADJ.
AD835, were
Figure 5 shows the
The small-signal bandwidth from the inputs X, Y, and Z to
the output W is a single-pole response. The pole is inversely
proportional to α. For α = 1 (GADJ floating), the bandwidth is
about 2 GHz; for α > 1, the bandwidth is reduced; and for α < 1,
the bandwidth is increased.
All input ports, X, Y, and Z, are differential and internally
biased to midsupply, V
/2. The differential input impedance is
POS
500 Ω up to 100 MHz, rolling off to 50 at 2 GHz. All inputs
can be driven in single-ended fashion and can be ac-coupled. In
dc-coupled operation, the inputs can be biased to a common
mode that is lower than V
/2. The bias current flowing out of
POS
the input pins to accommodate the lower common mode is
subtracted from the 50 mA total available from the internal
reference V
equivalent 250 dc resistance to V
1 V below V
/2 at the VREF pin. Each input pin presents an
POS
/2. If all six input pins sit
POS
/2, a total of 6 × 1 V/250 Ω = 24 mA must flow
POS
internally from VREF to the input pins.
Calibration
The dc offset of the ADL5391 is approximately 20 mV but
changes over temperature and has variation from part to part
(see
Figure 4). It is generally not of concern unless the ADL5391
is operated down to dc (close to the point X = 0 V or Y = 0 V),
where 0 V is expected on the output (W = 0 V). For example,
when the ADL5391 is used as a VGA and a large amount of
attenuation is needed, the maximum attenuation is determined
by the input dc offset.
Applying the proper voltage on the Z input removes the W
offset. Calibration can be accomplished by making the appropriate
cross plots and adjusting the Z input to remove the offset.
Additionally, gain scaling can be adjusted by applying a dc
voltage to the GADJ pin, as shown in
Figure 5.
BASIC CONNECTIONS
Multiplier Connections
The best ADL5391 performance is achieved when the X, Y, and
Z inputs and W output are driven differentially; however, they
can be driven single-ended. Single-ended-to-differential
transformations (or differential-to-single-ended transformations)
can be done using a balun or active components, such as the
AD8313, the AD8132 (both with operation down to dc), or the
AD8352 (for higher drive capability). If using the ADL5391
single-ended without ac coupling capacitors, the reference
voltage of 2.5 V needs to be taken into account. Voltages above
2.5 V are positive voltages and voltages below 2.5 V are negative
voltages. Care needs to be taken not to load the ADL5391 too
heavily, the maximum reference current available is 50 mA.
Rev. 0 | Page 10 of 16
Page 11
ADL5391
[
]
–
Matching the Input/Output
The input and output impedance’s of the ADL5391 change over
frequency, making it difficult to match over a broad frequency
range (see
Figure 15 and Figure 16). The evaluation board is
matched for lower frequency operation, and the impedance
change at higher frequencies causes the change in gain seen in
Figure 6. If desired, the user of the ADL5391 can design a
matching network to fit their application.
Most of the data for the ADL5391 was collected by using it as a
fast reacting analog VGA. Either X or Y inputs can be used for
the RF input (and the other as the very fast analog control),
because either input can be used from dc to 2 GHz. There is a
linear relationship between the analog control and the output of
the multiplier in the VGA mode.
Figure 6 and Figure 7 show the
dynamic range available in VGA mode (without optimizing the
dc offsets).
The speed of the ADL5391 in VGA mode allows it to be used as
an amplitude modulator. Either or both inputs can have
modulation or CW applied. AM modulation is achieved by
feeding CW into X (or Y) and adding AM modulation to the Y
(or X) input.
Squaring and Frequency Doubling
Amplitude domain squaring of an input signal, E, is achieved
simply by connecting the X and Y inputs in parallel to produce
an output of E
2
. The input can be single-ended, differential, or
through a balun (frequency range and dynamic range can be
limited if used single ended).
When the input is a sine wave Esin(ωt), a signal squarer behaves
as a frequency doubler, because
2
E
[]
2
tE
)sin(
2
()
(
t
ω−=ω2cos1
)
(3)
Ideally, when used for squaring and frequency doubling, there is
no component of the original signals on the output. Because of
internal offsets, this is not the case. If Equation 3 were rewritten
to include theses offsets, it could separate into three output
terms (Equation 4).
[]
2
E
[]
2
OFSTtEOFSTtE
)sin()sin(
)sin(2)cos(2
=+ω×+ω
2
(4)
⎛
⎜
OFSTOFSTtEt
⎜
⎝
⎞
E
2
⎟
++ω+ω
⎟
2
⎠
where:
The dc component of the output is related to the square of both
the offset (OFST) and the signal input amplitude (E). The offset
can be found in
Figure 4 and is approximately 20 mV. The
second harmonic output grows with the square of the input
amplitude, and the signal bleedthrough grows proportionally
with the input signal. For smaller signal amplitudes, the signal
bleedthrough can be higher than the second harmonic
component. As the input amplitude increases, the second
harmonic component grows much faster than the signal
bleedthrough and becomes the dominant signal at the output.
If the X and Y inputs are driven too hard, third harmonic
components will also increase.
For best performance creating harmonics, the ADL5391 should
be driven differentially.
Figure 17 shows the performance of the
ADL5391 when used as a harmonic generator (the evaluation
board was used with R9 and R10 removed and R2 = 56.2 Ω). If
dc operation is necessary, the ADL5391 can be driven single
ended (without the dc blocks). The flatness of the response over
a broad frequency range depends on the input/output match.
The fundamental bleed through not only depends on the
amount of power put into the device but also depends on
matching the unused differential input/output to the same
impedance as the used input/output.
Figure 18 shows the
performance of the ADL5391 when driven single ended
(without ac coupling capacitors), and
Figure 19 shows the
schematic of the setup. A resistive input/output match were
used to match the input from dc to 1 GHz and the output from
dc to 2 GHz. Reactive matching can be used for more narrow
frequency ranges. When matching the input/output of the
ADL5391, care needs to be taken not to load the ADL5391 too
heavily; the maximum reference current available is 50 mA.
15
–20
–25
–30
–35
–40
–45
GAIN (dBm)
–50
–55
–60
–65
10 100 200 300 400 500 600 700 800 900 1000
Figure 17. ADL5391 Used as a Harmonic Generator
SECOND HARMONIC GAIN
BLEEDTHRU GAI N
THIRD HARMONIC GAIN
FREQUENCY (MHz)
06059-026
The dc component is OFST2 + E2/2.
The input signal bleedthrough is 2Esin(ωt)OFST.
The input squared is E
2
/2[cos(2ωt)].
Rev. 0 | Page 11 of 16
Page 12
ADL5391
X
Y
0
–5
–10
–15
–20
–25
–30
–35
GAIN (dBm)
–40
–45
–50
–55
–60
–65
SECOND HARMONIC G AIN
10 100 200 300 400 500 600 700 800 900 1000
BLEEDTHRU GAI N
THIRD HARMONIC GAIN
FREQUENCY (MHz )
06059-027
Figure 18. Single-Ended (DC) ADL5391 Used as a Harmonic Generator
IN
5dB PAD
21Ω
74Ω
53Ω
53Ω
YIN
74Ω
21Ω
5dB PAD
XM
XP
YM
YP
WP
WM
150Ω
10dB PAD
200Ω
62Ω
06059-028
Figure 19. Setup for Single-Ended Data
Use as a Detector
The ADL5391 can be used as a square law detector. When
amplitude squaring is performed, there are components of the
multiplier output that correlate to the signal bleedthrough and
second harmonic, as seen in Equation 4. However, as noted in
Squaring and Frequency Doubling section, there is also a dc
the
component that is directly related to the offset and the squared
input magnitude. If a signal is split and feed into the X and Y
inputs and a low-pass filter were place on the output, the resulting
dc signal would be directly related to the square of the input
magnitude. The intercept of the response will shift slightly from
part to part (and over temperature) with the offset, but this can
C7
0.1µF
XP
J6
P
C18
0.1µF
0.1µF
J8
C20
0.1µF
TC1-1-13MT3
C4
TC1-1-13MT2
Figure 22. Schematic for ADL5391 Used as Square Law Detector
56.2Ω
56.2Ω
11
XM
R2
12
XP
WP
WM
YM
13
R1
14
YP
be removed through calibration.
of the ADL5391 as a square law detector,
error vs. the input power, and
Figure 20 shows the response
Figure 21 shows the
Figure 22 shows the
configuration used.
0.7
0.6
0.5
0.4
(V)
OUT
V
0.3
0.2
0.1
0
000.70.60.50.40.30.20.1
VIN (V rms)
2
.8
06059-091
Figure 20. ADL5391 Used as Square Law Detector DC Output vs. Square of Input
1.6
1.4
1.2
1.0
0.8
0.6
ERROR (dB)
0.4
0.2
0
–0.2
–301050–5–10–15–20–25
PIN X (dBm)
06059-092
Figure 21. ADL5391Used as a Square Law Detector Error vs. Power Input
R5, R6 Matching resistor.s 24.9 Ω, 0402 resistors
R4 Matching resistor. 100 Ω, 0603 resistor
R8, R11 Can be used for voltage divider or filtering. Open, 0603 resistors
SW1 Enable switch: enable = 5 V, disable = 0 V. SW1 installed
TP1, TP2, TP4, TP5,
TP6, TP7, TP8, TP9
TP13 Red test loop. V
TP12, TP14 Black test loops. COMM
TP3, TP10, TP11 Yellow test loops. GADJ_DC, ENBL_DC, VMID
DUT ADL5391. ADL5391ACPZ
SMA connectors for single-ended, high frequency operation. If J5
and J6 are used, R9, R10, R14, and R15 should be removed. R2 and
R3 should also be populated to match the inputs. If used in broadband
operation, C4, C7, C8, and C2 need to be replaced with 0 Ω resistors.
SMA connectors for broadband differential operation. If these are
used, baluns should be removed and jumped over using 0 Ω
resistors, and C14, C15, C18, and C20 should be removed.
Single-ended-to-differential transformation for high frequency ac
operation. If dc operation is necessary, the baluns can be removed
and jumped over using 0 Ω resistors.
DC block capacitors. 0.1 μF, 0402 capacitors
Not installed, dc block capacitors. Open, 0402 capacitors
Matching resistors. Input impedance to X, Y, and Z inputs are the
same. For the same frequency, R1, R2, and R3 should be the same.
Green test loop.
WP, ZP, YP, XP
WM, ZM, YM, XM
TC1-1-13M+
Mini-Circuits
Open, 0603 resistors
T3 and T4 are populated,
but the Y and Z inputs
are set up for dc operation.