10 MHz to 10 GHz
67 dB TruPwr Detector
Data Sheet
ADL5906
Rev. A Document Feedback
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FEATURES
Accurate rms-to-dc conversion from 10 MHz to 10 GHz
Single-ended ±1.0 dB dynamic range: 67 dB at 2.14 GHz
No balun or external input matching required
Response independent of waveform types, such as
GSM-EDGE/CDMA/W-CDMA/TD-SCDMA/WiMAX/LTE
Logarithmic slope: 55 mV/dB
Temperature stability: 1 dB from −40°C to +125°C
Operating temperature: −55°C to +125°C
Supply voltage: 4.75 V to 5.25 V
Sleep current: 250 µA
Pin compatible with ADL5902 and AD8363
APPLICATIONS
Power amplifier linearization/control loops
Transmitter signal strength indication (TSSI)
RF instrumentation
FUNCTIONAL BLOCK DIAGRAM
TADJ/
PWDN
NIC
VREF
VTGT
CRMS
VRMS
VSET
VTEMP
NIC
RFIN–
RFIN+
NIC
GND1GND2
EPAD
X
2
BIAS AND P OWE R
DOWN CONTROL
1
I
TGT
LI NEAR-I N-dB VGA
(NEGATIVE SLOPE)
I
SQR
26pF
2
VPOS1 V
POS2
3
4
11
10
9
5
6
7
8
16
15
14
13
ADL5906
12
X
2
V
REF
2.3V
TEMPERATURE
SENSOR
G = 5
11287-001
Figure 1.
GENERAL DESCRIPTION
The ADL5906 is a true rms responding power detector that has a
67 dB measurement range when driven with a single-ended 50 Ω
source. The easy to use input makes the ADL5906 frequency
versatile by eliminating the need for a balun or any other form
of external input tuning for operation up to 10 GHz.
The ADL5906 provides a solution in a variety of high frequency
systems requiring an accurate rms measurement of signal power.
The ADL5906 can operate from 10 MHz to 10 GHz and can
accept inputs from 65 dBm to +8 dBm with varying crest factors
and bandwidths, such as GSM-EDGE, CDMA, W-CDMA,
TD-SCDMA, WiMAX, and OFDM-based LTE carriers. In
addition, its temperature stability over the broad temperature
range of −55°C to +125°C makes it ideally suited for a wide array
of communications, military, industrial, and instrumentation
applications.
Used as a power measurement device, VRMS is connected to
VSET. The output is then proportional to the logarithm of the
rms value of the input. In other words, the reading is presented
directly in decibels and is scaled 1.1 V per decade, or 55 mV/dB;
other slopes are easily arranged. In controller mode, the voltage
applied to VSET determines the power level required at the
input to null the deviation from the setpoint. The output buffer
can provide high load currents.
Requiring only a single supply of 5 V and a few capacitors, it is
easy to use and capable of being driven single-ended or with a
balun for differential input drive. The ADL5906 has a low 250 µA
sleep current when powered down by a logic high applied to the
PWDN pin. It powers up within approximately 1.4 µs to its
nominal operating current of 68 mA at 25°C.
The ADL5906 is supplied in a 4 mm × 4 mm, 16-lead LFCSP, and
it is pin compatible with the ADL5902 and the AD8363 TruPwr
rms detectors. This feature allows the designer to create one circuit
layout for projects requiring different dynamic ranges. A fully
populated RoHS-compliant evaluation board is available.
ADL5906 Data Sheet
Rev. A | Page 2 of 32
TABLE OF CONTENTS
Features .............................................................................................. 1
Applications ....................................................................................... 1
Functional Block Diagram .............................................................. 1
General Description ......................................................................... 1
Revision History ............................................................................... 2
Specifications ..................................................................................... 3
Absolute Maximum Ratings ............................................................ 7
ESD Caution .................................................................................. 7
Pin Configuration and Function Descriptions ............................. 8
Typical Performance Characteristics ............................................. 9
Theory of Operation ...................................................................... 16
Square Law Detector and Amplitude Target .............................. 16
RF Input Interface ...................................................................... 17
Temperature Sensor Interface ................................................... 17
VREF Interface ........................................................................... 17
Temperature Compensation Interface ..................................... 18
Power-Down Interface ............................................................... 19
VSET Interface ............................................................................ 19
Output Interface ......................................................................... 19
VTGT Interface .......................................................................... 19
Basis for Error Calculations ...................................................... 20
Measurement Mode Basic Connections.................................. 20
Setting VTADJ ................................................................................ 20
Setting VTGT ................................................................................. 21
Choosing a Value for CRMS ......................................................... 21
Output Voltage Scaling .............................................................. 22
System Calibration and Error Calculation .............................. 24
Using VTEMP to Improve Intercept Temperature Drift ........... 25
Description of Characterization ............................................... 27
Evaluation Board ............................................................................ 28
Evaluation Board Assembly Drawings .................................... 29
Outline Dimensions ....................................................................... 30
Ordering Guide .......................................................................... 30
REVISION HISTORY
10/13—Rev. 0 to Rev. A
Changes to Table 2 ............................................................................ 7
Changes to Ordering Guide .......................................................... 30
3/13—Revision 0: Initial Version
Data Sheet ADL5906
Rev. A | Page 3 of 32
SPECIFICATIONS
VPOS1 = VPOS2 = 5 V, TA = 25°C, single-ended input drive, RT = 60.4 Ω, VRMS connected to VSET, VTGT = 0.8 V, CRMS = 0.1 µF. Negative
current values imply that the ADL5906 is sourcing current out of the indicated pin.
Table 1.
Parameter Test Conditions/Comments Min Typ Max Unit
OVERALL FUNCTION
Frequency Range 10 to 10,000 MHz
RF INPUT INTERFACE RFIN+, Pin RFIN(Pin 14, Pin 15), ac-coupled
Input Impedance
Single-ended drive, 50 MHz
Common-Mode Voltage 2.5 V
100 MHz
±1.0 dB Dynamic Range Continuous wave (CW) input, TA = 25°C 62 dB
Maximum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm 2 dBm
Minimum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm −60 dBm
Deviation vs. Temperature Deviation from output at 25°C, VTADJ = 0.35 V
−40°C < TA < +85°C; PIN = 0 dBm −0.8/+0.2 dB
−40°C < T
A
< +85°C; P
IN
= 45 dBm
dB
−55°C < TA < +125°C; PIN = 0 dBm −1.3/+0.2 dB
−55°C < TA < +125°C; PIN = 45 dBm −1.2/+0.6 dB
Logarithmic Slope −65 dBm < PIN < +10 dBm; calibration at 40 dBm and 0 dBm 59 mV/dB
Logarithmic Intercept −65 dBm < PIN < +10 dBm; calibration at 40 dBm and 0 dBm −64 dBm
700 MHz
±1.0 dB Dynamic Range CW input, TA = 25°C 62 dB
Maximum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm 2 dBm
Minimum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm −60 dBm
Deviation vs. Temperature Deviation from output at 25°C, VTADJ = 0.35 V
−40°C < TA < +85°C; PIN = 0 dBm −0.9/+0.3 dB
−40°C < TA < +85°C; PIN = −45 dBm −0.9/+0.4 dB
−55°C < TA < +125°C; PIN = 0 dBm −1.5/+0.3 dB
−55°C < TA < +125°C; PIN = −45 dBm −1.3/+0.7 dB
Logarithmic Slope
−65 dBm < P
IN
< +10 dBm; calibration at 40 dBm, and 0 dBm
mV/dB
Logarithmic Intercept −65 dBm < PIN < +10 dBm; calibration at 40 dBm and 0 dBm −65 dBm
900 MHz
±1.0 dB Dynamic Range
CW input, T
A
= 25°C
dB
Maximum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm 3 dBm
Minimum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm −60 dBm
Deviation vs. Temperature Deviation from output at 25°C, VTADJ = 0.35 V
−40°C < TA < +85°C; PIN = 0 dBm −0.8/+0.3 dB
−40°C < TA < +85°C; PIN = −45 dBm −0.9/+0.4 dB
−55°C < TA < +125°C; PIN = 0 dBm −1.4/+0.3 dB
−55°C < TA < +125°C; PIN = −45 dBm −1.4/+0.8 dB
Logarithmic Slope −65 dBm < PIN < +10 dBm; calibration at 40 dBm and 0 dBm 59 mV/dB
Logarithmic Intercept −65 dBm < PIN < +10 dBm; calibration at −40 dBm and 0 dBm −65 dBm
Deviation from CW Response
(−45 dBm to −5 dBm)
12.16 dB peak-to-rms ratio (four-carrier W-CDMA) −0.1 dB
11.58 dB peak-to-rms ratio (LTE TM1, one-carrier, 20 MHz
bandwidth)
−0.2 dB
10.56 dB peak-to-rms ratio (W-CDMA) 0.05 dB
7.4 dB peak-to-rms ratio (64 QAM) −0.1 dB
ADL5906 Data Sheet
Rev. A | Page 4 of 32
Parameter Test Conditions/Comments Min Typ Max Unit
1900 MHz
±1.0 dB Dynamic Range CW input, TA = 25°C 66 dB
Maximum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm 6 dBm
Minimum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm −60 dBm
Deviation vs. Temperature
Deviation from output at 25°C, V
TADJ
= 0.35 V
−40°C < TA < +85°C; PIN = 0 dBm −0.8/+0.2 dB
−40°C < TA < +85°C; PIN = −45 dBm −0.8/+0.5 dB
−55°C < TA < +125°C; PIN = 0 dBm −1.4/+0.2 dB
−55°C < TA < +125°C; PIN = −45 dBm −1.2/+0.9 dB
Logarithmic Slope −65 dBm < PIN < +10 dBm; calibration at −40 dBm and 0 dBm 57 mV/dB
Logarithmic Intercept
−65 dBm < P
IN
< +10 dBm; calibration at −40 dBm and 0 dBm
dBm
2140 MHz
±1.0 dB Dynamic Range CW input, TA = 25°C 67 dB
Maximum Input Level, ±1.0 dB
Calibration at −55 dBm, −40 dBm, and 0 dBm
dBm
Minimum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm −60 dBm
Deviation vs. Temperature Deviation from output at 25°C, VTADJ = 0.35 V
−40°C < TA < +85°C; PIN = 0 dBm −0.8/+0.3 dB
−40°C < TA < +85°C; PIN = −45 dBm −0.8/+0.6 dB
−55°C < T
A
< +125°C; P
IN
= 0 dBm
dB
−55°C < TA < +125°C; PIN = −45 dBm −1.2/+0.9 dB
Logarithmic Slope −65 dBm < PIN < +10 dBm; calibration at 40 dBm and 0 dBm 56 mV/dB
Logarithmic Intercept −65 dBm < PIN < +10 dBm; calibration at 40 dBm and 0 dBm −65 dBm
Deviation from CW Response
(−45 dBm to −5 dBm)
12.16 dB peak-to-rms ratio (four-carrier W-CDMA) −0.1 dB
11.58 dB peak-to-rms ratio (LTE TM1, one-carrier, 20 MHz
bandwidth)
dB
10.56 dB peak-to-rms ratio (one-carrier W-CDMA) 0.1 dB
7.4 dB peak-to-rms ratio (64 QAM) −0.1 dB
2600 MHz
±1.0 dB Dynamic Range CW input, TA = 25°C 68 dB
Maximum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm 8 dBm
Minimum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm −60 dBm
Deviation vs. Temperature Deviation from output at 25°C, VTADJ = 0.4 V
−40°C < TA < +85°C; PIN = 0 dBm −0.9/+0.3 dB
−40°C < TA < +85°C; PIN = −45 dBm −1/+0.5 dB
−55°C < TA < +125°C; PIN = 0 dBm −1.4/+0.3 dB
−55°C < TA < +125°C; PIN = −45 dBm −1.4/+0.8 dB
Logarithmic Slope −65 dBm < PIN < +10 dBm; calibration at −40 dBm and 0 dBm 55 mV/dB
Logarithmic Intercept
−65 dBm < P
IN
< +10 dBm; calibration at −40 dBm and 0 dBm
dBm
3500 MHz
±1.0 dB Dynamic Range CW input, TA = 25°C 65 dB
Maximum Input Level, ±1.0 dB
Calibration at −55 dBm, −40 dBm, and 0 dBm
dBm
Minimum Input Level, ±1.0 dB Calibration at −55 dBm, −40 dBm, and 0 dBm −60 dBm
Deviation vs. Temperature Deviation from output at 25°C, VTADJ = 0.45 V
−40°C < TA < +85°C; PIN = 0 dBm −1.5/0 dB
−40°C < TA < +85°C; PIN = −45 dBm −1/+0.3 dB
−55°C < TA < +125°C; PIN = 0 dBm −1.5/0 dB
−55°C < TA < +125°C; PIN = −45 dBm −1.4/+0.4 dB
Logarithmic Slope −65 dBm < PIN < +10 dBm; calibration at −40 dBm and 0 dBm 52 mV/dB
Logarithmic Intercept −65 dBm < PIN < +10 dBm; calibration at −40 dBm and 0 dBm −64 dBm
Data Sheet ADL5906
Rev. A | Page 5 of 32
Parameter Test Conditions/Comments Min Typ Max Unit
5800 MHz
±1.0 dB Dynamic Range CW input, TA = 25°C 57 dB
Maximum Input Level, ±1.0 dB Calibration at −50 dBm, −40 dBm, and 0 dBm 3 dBm
Minimum Input Level, ±1.0 dB Calibration at −50 dBm, −40 dBm, and 0 dBm −54 dBm
Deviation vs. Temperature
Deviation from output at 25°C, V
TADJ
= 1 V
−40°C < TA < +85°C; PIN = 0 dBm −2.4/+0 dB
−40°C < TA < +85°C; PIN = −45 dBm −1.4/-0.2 dB
−55°C < TA < +125°C; PIN = 0 dBm −3.6/+0 dB
−55°C < TA < +125°C; PIN = −45 dBm −2.1/-0.2 dB
Logarithmic Slope −65 dBm < PIN < +10 dBm; calibration at −40 dBm and 0 dBm 42 mV/dB
Logarithmic Intercept
−65 dBm < P
IN
< +10 dBm; calibration at −40 dBm and 0 dBm
dBm
OUTPUT INTERFACE VRMS (Pin 6)
Output Swing, Controller Mode Swing range minimum, RL ≥ 500 Ω to ground 0.05 V
Swing range maximum, R
L
≥ 500 Ω to ground
V
Current Source/Sink Capability 10/10 mA
Rise Time PIN = off to −10 dBm, 10% to 90%, CRMS = 1 nF 0.1 µs
Fall Time PIN = −10 dBm to off, 90% to 10%, CRMS = 1 nF 14.6 µs
SETPOINT INPUT VSET (Pin 7)
Voltage Range Log conformance error ≤ 1 dB, minimum 2.14 GHz 3.92 V
Log conformance error ≤ 1 dB, maximum 2.14 GHz 0.4 V
Input Resistance 72 kΩ
Logarithmic Scale Factor
f = 2.14 GHz
mV/dB
Logarithmic Intercept f = 2.14 GHz −65 dBm
TEMPERATURE COMPENSATION TADJ/PWDN (Pin 1)
Input Voltage Range
0
V
POS
V
Input Bias Current VTADJ = 0.35 V 5 µA
Input Resistance VTADJ = 0.35 V 70 kΩ
VOLTAGE REFERENCE VREF (Pin 11)
Output Voltage PIN = −55 dBm 2.3 V
Temperature Sensitivity 25°C ≤ TA ≤ 125°C −0.12 mV/°C
−55°C ≤ TA ≤ +25°C 0.07 mV/°C
Short-Circuit Current Source/
Sink Capability
25°C ≤ TA ≤ 125°C 4/0.05 mA
−55°C ≤ TA +25°C 3/0.05 mA
Voltage Regulation TA = 25°C, ILOAD = 2 mA −0.4 %
TEMPERATURE REFERENCE
VTEMP (Pin 8)
Output Voltage TA = 25°C, RL ≥ 10 kΩ 1.4 V
Temperature Coefficient −40°C ≤ TA ≤ +125°C, RL ≥ 10 kΩ 4.8 mV/°C
Short-Circuit Current Source/
Sink Capability
25°C ≤ TA ≤ 125°C 4/0.05 mA
−55°C ≤ TA ≤ +25°C 3/0.05 mA
Voltage Regulation
T
A
= 25°C, I
LOAD
= 1 mA
%
RMS TARGET INTERFACE VTGT (Pin 12)
Input Voltage Range 0.2 2.5 V
Input Bias Current VTGT = 0.8 V 8 µA
Input Resistance 100 kΩ
POWER-DOWN INTERFACE
VTADJ/PWDN (Pin 1)
Voltage Level to Enable VPWDN decreasing 1.3 V
Voltage Level to Disable VPWDN increasing 1.4 V
Input Bias Current VPWDN = 5 V 72 µA
VPWDN = 0 V 0.1 µA
Enable Time VPWDN low to VRMS, 10% to 90%, CRMS = 1 nF, PIN = 0 dBm 1.4 µs
Disable Time
V
PWDN
high to V
RMS
, 90% to 10%, C
RMS
= 1 nF, P
IN
= 0 dBm
µs
ADL5906 Data Sheet
Rev. A | Page 6 of 32
Parameter Test Conditions/Comments Min Typ Max Unit
POWER SUPPLY INTERFACE VPOS1, VPOS2 (Pin 3, Pin 10)
Supply Voltage 4.75 5 5.25 V
Quiescent Current TA = 25°C, PIN < −60 dBm 68 mA
TA = 125°C, PIN < −60 dBm 86 mA
Power-Down Current
V
PWDN
> 1.4 V
µA
Data Sheet ADL5906
Rev. A | Page 7 of 32
ABSOLUTE MAXIMUM RATINGS
Table 2.
Parameter Rating
Supply Voltage, VPOS1, VPOS2 5.25 V
Input Average RF Power1 21 dBm
Equivalent Voltage, Sine Wave Input 2.51 V p-p
Internal Power Dissipation 550 mW
θJC2 10.6°C/W
θJB2 35.3°C/W
θJA2 57.2°C/W
Ψ
JT
2
1.0°C/W
ΨJB2 34°C/W
Maximum Junction Temperature 150°C
Operating Temperature Range
(ADL5906ACPZN)
−40°C to +105°C
Operating Temperature Range
(ADL5906SCPZN)
−55°C to +125°C
Storage Temperature Range −65°C to +150°C
Lead Temperature (Soldering, 60 sec) 300°C
1 This is for long durations. Excursions above this level, with durations much
less than 1 second, are possible without damage.
2 No airflow with the exposed pad soldered to a 4-layer JEDEC board.
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.
ESD CAUTION
ADL5906 Data Sheet
Rev. A | Page 8 of 32
PIN CONFIGURATION AND FUNCTION DESCRIPTIONS
PIN 1
INDICATOR
NOTES
1.
NIC = NO I NTERNAL CONNE CTI ON. DO NO T
CONNE CT TO THIS PIN.
2.
THE EXPOSED PAD REQ UIRES A GOOD THERMAL
AND EL E CTRICAL CONNE CTI ON TO THE GROUND
OF THE P RINT E D CIRCUIT BO ARD ( P CB) .
1TADJ/PWDN
2
NIC 3VPOS1 4GND1
11 VREF
12 VTGT
10 VPOS2
9GND2
5
CRMS 6
VRMS 7
VSET 8
VTEMP
15RFIN–
16NIC
14RFIN+
13NIC
TOP VIEW
(Not to Scale)
ADL5906
11287-002
Figure 2. Pin Configuration
Table 3. Pin Function Descriptions
Pin No. Mnemonic Description
1 TADJ/PWDN Temperature Compensation/Shutdown. This is a dual function pin used for controlling temperature slope
compensation at voltages <1.0 V and/or for shutting down the device at voltages >1.4 V. The temperature
compensation voltage is generally set by connecting this pin to VREF through a resistive voltage divider (see
the Setting VTADJ section for additional information). See Figure 46 for an equivalent circuit.
2, 13, 16 NIC No Internal Connection. Do not connect to these pins. These pins are not internally connected.
3, 10 VPOS1,
VPOS2
Power Supply. Because these pins are internally shorted, they must be connected to the same 5 V power
supply. The power supply to each pin must also be decoupled using 100 pF and 100 nF capacitors located as
close as possible to the pins.
4, 9 GND1, GND2 Ground. Connect both GND1 and GND2 to system ground using a low impedance path.
5 CRMS RMS Averaging Capacitor. Connect an rms averaging capacitor between CRMS and ground. See the Choosing
a Value for CRMS section for more information. See Figure 48 for an equivalent circuit.
6 VRMS RMS Output. In measurement mode, this pin is connected to VSET either directly or through a resistor divider
(when the slope is being increased). In controller mode, this pin is used to drive the gain control input of a
voltage variable attenuator (VVA) or variable gain amplifier (VGA). See Figure 48 for an equivalent circuit.
7
VSET
Setpoint Input. In measurement mode, this pin is connected to VRMS either directly or through a resistor
divider. In controller mode, the voltage applied to this pin sets the decibel value of the required RF input
level to balance the automatic power control loop. See Figure 47 for an equivalent circuit.
8 VTEMP Temperature Sensor Output of 1.4 V at 25°C with a Coefficient of 4.8 mV/°C. See Figure 43 for an equivalent circuit.
11 VREF Reference Voltage Output. This voltage reference has a nominal value of 2.3 V. This reference output voltage
can be used to set the voltage to the TADJ/PWDN and VTGT pins. See Figure 44 for an equivalent circuit.
12 VTGT RMS Target Voltage. The voltage applied to this pin sets the target RF input at the output of the VGA that is also the
rms squaring circuit. The recommended voltage for VTGT is 0.8 V. Increasing VTGT above 0.8 V degrades the rms
accuracy of the ADL5906. Reducing VTGT below 0.8 V can improve the rms accuracy for signals with very high crest
factors; however, it reduces the detection range of the ADL5906. See Figure 49 for an equivalent circuit.
14, 15 RFIN+, RFIN RF Inputs. The RF inputs are normally applied single-ended with the RF input signal ac-coupled to RFIN+ and
RFIN− ac-coupled to ground. See Figure 42 for an equivalent circuit.
EPAD The exposed pad on the underside of the device (EPAD) is also internally connected to ground and requires a
good thermal and electrical connection to the ground of the printed circuit board (PCB).
Data Sheet ADL5906
Rev. A | Page 9 of 32
TYPICAL PERFORMANCE CHARACTERISTICS
VPOS1 = VPOS2 = 5 V, single-ended input drive, VRMS connected to VSET, VTGT = 0.8 V, CRMS = 0.1 µF, TA = +25°C (green),
−55°C (light blue), −40°C (blue), +85°C (red), +105°C (orange), and +125°C (black), where appropriate. Error referred to slope
and intercept at indicated calibration points. Input RF signal is a sine wave (CW), unless otherwise indicated.
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
–65 –60 –55 –50 –45 –40 –35 –30 –25 –20 –15 –10 –5 0 5 10
OUTPUT VOLTAGE (V)
100MHz TO 1G Hz
20MHz
10MHz
PIN (dBm)
11287-003
2GHz
3GHz
4GHz
5GHz
6GHz
7GHz
8GHz
9GHz
10GHz
Figure 3. Typical VRMS vs. Input Power (dBm) vs. Frequency
(10 MHz to 10 GHz) at 25°C
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
OUTPUT VOLTAGE (V)
P
IN
(d Bm)
CW
QPSK PEP = 3.8dB
16 QAM P E P = 6. 3dB
64 QAM P E P = 7. 4dB
11287-104
Figure 4. Error from CW Linear Reference vs. Signal Modulation
(QPSK, 16 QAM, 64 QAM), Frequency = 900 MHz, CRMS = 0.1 µF,
Three Point Calibration at 0 dBm, 40 dBm, and 55 dBm
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
OUTPUT VOLTAGE (V)
PIN (dBm)
CW
CDMA 2000 P EP = 11.02dB
1C W-CDMA PEP = 10.56dB
4C W-CDMA PEP = 12.08dB
11287-005
Figure 5. Error from CW Linear Reference vs. Signal Modulation (CDMA 2000,
One-Carrier W-CDMA, Four-Carrier W-CDMA), Frequency = 2.14 GHz,
CRMS = 0.1 µF, Three Point Calibration at 0 dBm, −40 dBm, and −55 dBm
–20dBm
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
0.01 0.1 110
OUTPUT VOLTAGE (V)
FREQUENCY (GHz)
–50dBm
–10dBm
0dBm
–30dBm
–40dBm
11287-006
Figure 6. Typical VRMS vs. Frequency for Six RF Input Levels
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
OUTPUT VOLTAGE (V)
P
IN
(d Bm)
CW
QPSK PEP = 3.8dB
16 QAM P E P = 6. 3dB
64 QAM P E P = 7. 4dB
11287-007
Figure 7. Error from CW Linear Reference vs. Signal Modulation
(QPSK, 16 QAM, 64 QAM), Frequency = 2.14 GHz, CRMS = 0.1 µF,
Three Point Calibration at 0 dBm, −40 dBm, and −55 dBm
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
OUTPUT VOLTAGE (V)
PIN (dBm)
CW
LTE TM1 1CR 20MHz P EP = 11.58dB
11287-008
Figure 8. Error from CW Linear Reference vs. Signal Modulation
(LTE TM1 One-Carrier, 20 MHz), Frequency = 2.14 GHz, CRMS = 0.1 µF,
Three Point Calibration at 0 dBm, −40 dBm, and −55 dBm
ADL5906 Data Sheet
Rev. A | Page 10 of 32
OUTPUT VOLTAGE (V)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
ERRO R ( dB)
OUTPUT VOLTAGE (V)
P
IN
(d Bm)
V
TADJ
= 0.35V
CALIBRATIONAT 0dBm, –40dBm, AND –55dBm
11287-009
–65 –55 –45 –35 –25 –15 –5 5
Figure 9. VRMS and Log Conformance Error vs. Input Level and Temperature at
100 MHz
OUTPUT VOLTAGE (V)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
ERRO R ( dB)
OUTPUT VOLTAGE (V)
PIN (dBm)
VTADJ = 0.35V
CALIBRATIONAT 0dBm, –40dBm, AND –55dBm
11287-010
–65 –55 –45 –35 –25 –15 –5 5
Figure 10. VRMS and Log Conformance Error vs. Input Level and Temperature
at 700 MHz
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
OUTPUT VOLTAGE (V)
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
OUTPUT VOLTAGE (V)
5
PIN (dBm)
VTADJ = 0.35V
CALIBRATIONAT 0dBm, –40dBm, AND –55dBm
11287-011
–65 –55 –45 –35 –25 –15 –5
Figure 11. VRMS and Log Conformance Error vs. Input Level and Temperature
at 900 MHz
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
OUTPUT VOLTAGE (V)
P
IN
(d Bm)
11287-012
V
TADJ
= 0.35V
Figure 12. Distribution of Log Conformance Error with Respect to VRMS at
25°C vs. Input Level and Temperature at 100 MHz
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
OUTPUT VOLTAGE (V)
PIN (dBm)
11287-013
VTADJ = 0.35V
Figure 13. Distribution of Log Conformance Error with Respect to VRMS at
25°C vs. Input Level and Temperature at 700 MHz
OUTPUT VOLTAGE (V)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
ERRO R ( dB)
–65 –55 –45 –35 –25 –15 –5 5
P
IN
(d Bm)
11287-014
V
TADJ
= 0.35V
Figure 14. Distribution of Log Conformance Error with Respect to VRMS at
25°C vs. Input Level and Temperature at 900 MHz
Data Sheet ADL5906
Rev. A | Page 11 of 32
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
OUTPUT VOLTAGE (V)
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
OUTPUT VOLTAGE (V)
–65 –55 –45 –35 –25 –15 –5 5
P
IN
(d Bm)
V
TADJ
= 0.35V
CALIBRATIONAT 0dBm, –40dBm, AND –55dBm
11287-015
Figure 15. VRMS and Log Conformance Error vs. Input Level and Temperature
at 1.9 GHz
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
OUTPUT VOLTAGE (V)
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
OUTPUT VOLTAGE (V)
–65 –55 –45 –35 –25 –15 –5 5
P
IN
(d Bm)
V
TADJ
= 0.35V
CALIBRATIONAT 0dBm, –40dBm, AND –55dBm
11287-016
Figure 16. VRMS and Log Conformance Error vs. Input Level and Temperature
at 2.14 GHz
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
OUTPUT VOLTAGE (V)
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
OUTPUT VOLTAGE (V)
–65 –55 –45 –35 –25 –15 –5 5
P
IN
(d Bm)
V
TADJ
= 0.4V
CALIBRATIONAT 0dBm, –40dBm, AND –55dBm
11287-017
Figure 17. VRMS and Log Conformance Error vs. Input Level and Temperature
at 2.6 GHz
OUTPUT VOLTAGE (V)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
ERRO R ( dB)
–65 –55 –45 –35 –25 –15 –5 5
PIN (dBm)
11287-018
VTADJ = 0.35V
Figure 18. Distribution of Log Conformance Error with Respect to VRMS at
25°C vs. Input Level and Temperature at 1.9 GHz
OUTPUT VOLTAGE (V)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
ERRO R ( dB)
–65 –55 –45 –35 –25 –15 –5 5
PIN (dBm)
11287-019
V
TADJ
= 0.35V
Figure 19. Distribution of Log Conformance Error with Respect to VRMS at
25°C vs. Input Level and Temperature at 2.14 GHz
ERRO R ( dB)
OUTPUT VOLTAGE (V)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15
–5 5
P
IN
(d Bm)
11287-020
V
TADJ
= 0.4V
Figure 20. Distribution of Log Conformance Error with Respect to VRMS at
25°C vs. Input Level and Temperature at 2.6 GHz
ADL5906 Data Sheet
Rev. A | Page 12 of 32
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
OUTPUT VOLTAGE (V)
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
OUTPUT VOLTAGE (V)
–65 –55 –45 –35 –25 –15 –5 5
PIN (dBm)
VTADJ = 0.45V
CALIBRATIONAT 0dBm, –40dBm, AND –55dBm
11287-021
Figure 21. VRMS and Log Conformance Error vs. Input Level and Temperature
at 3.5 GHz
0
0.25
0.50
0.75
1.00
1.25
1.50
1.75
2.00
2.25
2.50
2.75
3.00
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
OUTPUT VOLTAGE (V)
–65 –55 –45 –35 –25 –15 –5 5
P
IN
(d Bm)
V
TADJ
= 1V
CALIBRATIONAT 0dBm, –40dBm, AND –50dBm
11287-022
Figure 22. VRMS and Log Conformance Error vs. Input Level and Temperature
at 5.8 GHz
0
0.25
0.50
0.75
1.00
1.25
1.50
1.75
2.00
2.25
2.50
2.75
3.00
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
OUTPUT VOLTAGE (V)
–45 –35 –25 –15 –5 5
P
IN
(d Bm)
V
TADJ
= 1V
CALIBRATIONAT 0dBm, –20dBm, AND –35dBm
11287-023
Figure 23. VRMS and Log Conformance Error vs. Input Level and Temperature
at 8 GHz
ERRO R ( dB)
OUTPUT VOLTAGE (V)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
P
IN
(d Bm)
11287-024
V
TADJ
= 0.45V
Figure 24. Distribution of Log Conformance Error with Respect to VRMS at
25°C vs. Input Level and Temperature at 3.5 GHz
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–60 –50 –40 –30 –20 –10 010
ERRO R ( dB)
OUTPUT VOLTAGE (V)
PIN (dBm)
11287-025
VTADJ = 1V
Figure 25. Distribution of Log Conformance Error with Respect to VRMS at
25°C vs. Input Level and Temperature at 5.8 GHz
0
0.25
0.50
0.75
1.00
1.25
1.50
1.75
2.00
2.25
2.50
2.75
3.00
–35 –25 –15 –5 5
OUTPUT VOLTAGE (V)
PIN (dBm)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
ERRO R ( dB)
VTADJ = 1V
CALIBRATIONAT 0dBm, –10dBm, AND –20dBm
11287-026
Figure 26. VRMS and Log Conformance Error vs. Input Level and Temperature
at 10 GHz
Data Sheet ADL5906
Rev. A | Page 13 of 32
COUNT
1000
800
600
400
200
0
2.8 3.0 3.22.9 3.1 3.3 3.4 3.5
VRMS (V)
11287-027
REPRE S E NTS 4500 PARTS
Figure 27. Distribution of VRMS, PIN = −10 dBm, 900 MHz
COUNTS
1000
800
600
400
200
0
0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.5
V
RMS
(V)
11287-028
REPRE S E NTS 4500 PARTS
Figure 28. Distribution of VRMS, PIN = −45 dBm, 900 MHz
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
0 5 10 15 20 25 30 35 40 45 50
OUTPUT VOLTAGE (V)
TIME (µs)
RF BURS T PUL S E
0dBm
–10dBm
–20dBm
–30dBm
–40dBm
11287-029
Figure 29. Output Response to RF Burst Input, Carrier Frequency = 2.14 GHz,
CRMS = 1 nF
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
OUTPUT (V)
TIME (ms)
00.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5 5.0
RF BURS T PUL S E
0dBm
–10dBm
–20dBm
–30dBm
–40dBm
11287-030
Figure 30. Output Response to RF Burst Input, Carrier Frequency = 2.14 GHz,
CRMS = 0.1 µF
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
TIME (µs)
0246810 12 14 16 18 20 22
OUTPUT VOLTAGE (V)
0dBm
–10dBm
–20dBm
–30dBm
–40dBm
TADJ/PWDN
PULSE
11287-031
Figure 31. Output Response Using Power-Down Mode for Various RF Input
Levels, Carrier Frequency = 2.14 GHz, CRMS = 1 nF
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
00.5 1.0 1.5 2.0 2.5
OUTPUT VOLTAGE (V)
TIME (ms)
TADJ/PWDN
PULSE
0dBm
–10dBm
–20dBm
–30dBm
–40dBm
11287-032
Figure 32. Output Response Using Power-Down Mode for Various RF Input
Levels, Carrier Frequency = 2.14 GHz, CRMS = 0.1 µF
ADL5906 Data Sheet
Rev. A | Page 14 of 32
0
20
40
60
80
100
120
140
160
180
200
220
240
100 1k 10k 100k 1M 10M
NOISE SPECTRAL DENSITY (nV/√Hz)
FREQUENCY (Hz)
11287-033
Figure 33. Noise Spectral Density of VRMS, PIN = −10 dBm, 35 dBm, and
60 dBm (No Change in NSD vs. PIN), CRMS = 0.1 µF
–5
–4
–3
–2
–1
0
1
2
3
4
5
0.5
0.7
0.9
1.1
1.3
1.5
1.7
1.9
2.1
2.3
2.5
–55 –35 –15 525 45 65 85 105 125
ERRO R ( °C)
VTEMP (V)
TEMPERATURE ( °C)
11287-034
Figure 34. VTEMP and Linearity Error with Respect to Straight Line vs.
Temperature for Typical Device
1.32 1.34 1.36 1.38 1.40 1.42 1.44
COUNT
1000
800
600
400
200
0
VTEMP VOLTAGE (V)
11287-035
REPRE S E NTS 4500 PARTS
Figure 35. Distribution of VTEMP at 25°C, No RF Input
–40
–30
–20
–10
0
10
20
30
40
CHANGE IN V
REF
(mV)
–55 –35 –15 525 45 65 85 105 125
TEMPERATURE ( °C)
11287-036
Figure 36. Change in VREF vs. Temperature with Respect to 25°C,
PIN = −40 dBm
COUNT
1000
800
600
400
200
0
2.25 2.26 2.27 2.28 2.29 2.30 2.31 2.32
V
REF
BIAS V OLTAGE (V)
11287-037
REPRE S E NTS 4500 PARTS
Figure 37. Distribution of VREF at 25°C, No RF Input
0.1
1
10
100
1.20 1.25 1.30 1.35 1.40 1.45
SUPPLY CURRENT ( mA)
VPWDN (V)
V
PWDN
INCREASING
11287-038
V
PWDN
DECREASING
Figure 38. Supply Current vs. VPWDN
Data Sheet ADL5906
Rev. A | Page 15 of 32
50
55
60
65
70
75
80
85
90
–55 –35 –15 525 45 65 85 105 125
SUPPLY CURRENT ( mA)
TEMPERATURE ( °C)
11287-004
Figure 39. Supply Current vs. Temperature
RETURNLOSS (dB)
START10MHz STOP 10GHz1GHz/DIV
30
–20
–10
10
0
11287-040
Figure 40. Return Loss at RF Input Port, 10 MHz to 10 GHz
ADL5906 Data Sheet
Rev. A | Page 16 of 32
THEORY OF OPERATION
The ADL5906 is functionally nearly identical to the ADL5902
but has a broader frequency range (10 MHz to 10 GHz). It is a
true rms responding detector with a 67 dB measurement range
at 2.14 GHz and a greater than 57 dB measurement range at
frequencies up to 5.8 GHz. It is pin compatible with the ADL5902
and AD8363. Transfer function peak-to-peak ripple is 0.3 dB
over the entire dynamic range. Temperature stability of the rms
output measurements provides <±1 dB error typical over the
temperature range of −40°C to +125°C up to 3.5 GHz. The device
accurately measures waveforms that have a high peak-to-rms
ratio (crest factor).
The ADL5906 consists of a high performance automatic gain
control (AGC) loop. As shown in Figure 41, the AGC loop
comprises a wide bandwidth variable gain amplifier (VGA), square
law detectors, an amplitude target circuit, and an output driver.
The nomenclature used in this data sheet to distinguish between
a pin name and the signal on that pin is as follows:
The pin name is all uppercase, for example, CRMS, VSET,
and VRMS.
The signal name or a value associated with that pin is the
pin mnemonic with a partial subscript, for example, CRMS,
VSET, and VRMS.
SQUARE LAW DETECTOR AND AMPLITUDE TARGET
The VGA gain has the form
GSET = GO e
)/(
GNSSET
VV
(1)
where:
GO is the basic fixed gain.
VGNS is a scaling voltage that defines the gain slope (the decibel
change per voltage). The gain decreases with increasing VSET.
The VGA output is
VSIG = GSET × RFIN = GO × RFIN e
)/(
GNSSET
VV
(2)
where RFIN is the ac voltage applied to the input terminals of the
ADL5906.
The output of the VGA, VSIG, is applied to a wideband square law
detector. The detector provides the true rms response of the RF
input signal, independent of waveform. The detector output, ISQR, is
a fluctuating current with a positive mean value. The difference
between ISQR and an internally generated current, ITGT, is integrated
by the parallel combination of CF and the external capacitor
attached to the CRMS pin at the summing node. CF is an on-chip
26 pF filter capacitor, and CRMS, the external capacitance connected
to the CRMS pin, can be used to arbitrarily increase the averaging
time while trading off with the response time. When the AGC
loop is at equilibrium
Mean(ISQR) = ITGT (3)
This equilibrium occurs only when
Mean(VSIG2) = VTGT2 (4)
where VTGT is the voltage presented at the VTGT pin. This pin
can conveniently be connected to the VREF pin through a voltage
divider to establish a target rms voltage, VATG, of ~40 mV rms when
VTGT = 0.8 V.
Because the square law detectors are electrically identical and
well matched, process and temperature dependent variations
are effectively cancelled.
TADJ/PWDN
BAND GAP
REFERENCE
VRMS
VTEMP (1.4V)
VREF (2.3V)
I
SQR
I
TGT
X
2
X
2
G
SET
C
RMS
(EXTERNAL) C
F
(INTERNAL)
V
SIG
VGA
SUMMING
NODE
VSET
C
H
(INTERNAL)
VPOS1/VPOS2
GND1/GND2
RFIN+
RFIN–
TEMPERATURE COMPENSATION
AND BIAS
TEMPERATURE
SENSOR
VTGT
CRMS
V
ATG
=V
TGT
20
11287-041
Figure 41. Simplified Architecture Details
Data Sheet ADL5906
Rev. A | Page 17 of 32
When forcing the previous identity by varying the VGA setpoint, it
is apparent that
RMS(VSIG) = √(Mean(VSIG2)) = √(VATG2) = VATG (5)
Substituting the value of VSIG from Equation 2 results in
RMS(G0 × RFIN e
)/(
GNSSET
VV
) = VATG (6)
When connected as a measurement device, VSET = VRMS. Solving
for VRMS as a function of RFIN,
VRMS = VSLOPE × log10(RMS(RFIN)/VZ) (7)
where:
VSLOPE = 1.12 V/decade (or 56 mV/dB) at 2.14 GHz.
VZ is the intercept voltage.
When RMS(RFIN) = VZ, this implies that VRMS = 0 V because
log10(1) = 0. This makes the intercept the input that forces VRMS =
0 V if the ADL5906 had no sensitivity limit.
In most applications, the AGC loop is closed through the setpoint
interface and the VSET pin. In measurement mode, VRMS is
directly connected to VSET (see the Measurement Mode Basic
Connections section for more information). In controller mode,
a control voltage is applied to VSET, and the VRMS pin typically
drives the control input of an amplification or attenuation system.
In this case, the voltage at the VSET pin forces a signal amplitude
at the RF inputs of the ADL5906 that balances the system through
feedback.
RF INPUT INTERFACE
Figure 42 shows the RF input connections within the ADL5906.
Two internal 2.5 kΩ resistors connected between RFIN+ and RFIN−
primarily set the input impedance. A dc level of approximately
half the supply voltage on each pin is established internally at
the center point of the bias resistors. Either the RFIN+ or the
RFINpin can be used as the single-ended RF input pin. Connect
signal coupling capacitors from the input signal to the RFIN+
and RFINpins. A single external 60.4 Ω resistor to ground
from the desired input creates an equivalent 50 impedance
over a broad section of the operating frequency range. RF ac-couple
the other input pin to common (ground). The input signal high-
pass corner formed by the internal and external resistances of
the input coupling capacitor is
fHIGHPASS = 1/(2 × π × 50 × C) (8)
where C is the capacitance in farads, and fHIGHPASS is in hertz.
The input coupling capacitors must be large enough in value to
pass the input signal frequency of interest and determine the low
end of the frequency response. RFIN+ and RFINcan also be
driven differentially using a balun.
ESD
ESD ESD ESD ESD ESD
ESD
ESD ESD ESD ESD ESD
ESD
RFIN–RFIN+
VPOS
VBIAS
GND
LOAD
2.5kΩ 2.5kΩ
11287-141
Figure 42. RF Inputs
Extensive ESD protection is employed on the RF inputs, and this
protection limits the maximum possible input to the ADL5906.
TEMPERATURE SENSOR INTERFACE
The ADL5906 provides a temperature sensor output with a scaling
factor of the output voltage of approximately 4.8 mV/°C. The
output is capable of sourcing 4 mA and sinking 50 µA maximum
at 25°C. An external resistor can be connected from VTEMP to
GND to provide additional current sink capability. The typical
output voltage at 25°C is approximately 1.4 V.
VTEMP
VPOS
GND
INTERNAL
VPAT
12kΩ
4kΩ
11287-042
Figure 43. TEMP Interface Simplified Schematic
VREF INTERFACE
The VREF pin provides an internally generated voltage reference
for the user. The VREF voltage is a temperature stable 2.3 V
reference that is capable of sourcing 4 mA and sinking 50 µA
maximum. An external resistor can be connected from VREF
to GND to provide additional current sink capability. The
voltage on this pin can be used to drive the TADJ/PWDN and
VTGT pins.
INTERNAL
VOLTAGE
16kΩ
VREF
VPOS
GND
11287-143
Figure 44. VREF Interface Simplified Schematic
ADL5906 Data Sheet
Rev. A | Page 18 of 32
TEMPERATURE COMPENSATION INTERFACE
The ADL5906 has a TADJ pin that provides the ability to optimize
temperature performance using proprietary techniques as in
the ADL5902. Just like the ADL5902, the ADL5906 has dual
functionality on Pin 1, TADJ/PWDN; however, the PWDN
function was redesigned to be driven by CMOS logic as low
as 1.8 V. For more detail on the power-down interface, see the
Power-Down Interface section.
For optimal performance, the output temperature drift must
be compensated using the TADJ pin. The absolute value of
compensation varies with frequency and VTGT. For recommended
VTADJ values at popular frequencies, see the Setting VTADJ section.
One difference in the temperature compensation of the ADL5906
compared to the ADL5902 is that VTADJ adjusts the slope of the
detector, and with the ADL5902, the intercept was adjusted.
Adjusting the slope was found beneficial to locking in temperature
drift and thereby producing parallel error curves over most
frequencies. Any remaining intercept temperature drift can
then be reduced in the digital domain after sampling VRMS
because the intercept drift is quite repeatable at frequencies
up to approximately 5.8 GHz (see the Using VTEMP to
Improve Intercept Temperature Drift section).
There is a trade-off in setting values, and optimizing for one
area of the dynamic range may mean less than optimal drift
performance at other input amplitudes. In addition, different
voltages applied to the VTGT pin impact drift; all TADJ voltages
shown in the performance curves were determined with a
VTGT of 0.8 V. For VTGT values that do not deviate too far
from the nominal 0.8 V, and for frequencies up to approximately
5 GHz, it is expected that the TADJ voltages are a good starting
point for the best temperature drift compensation.
Compensating the device for temperature drift using VTADJ allows
for great flexibility. If the user requires minimum temperature drift
at a given input power, a subset of the dynamic range, or even
over a different temperature range than shown in this data
sheet, the VTADJ can be swept while monitoring VRMS over the
temperature at the frequency and amplitude of interest. The
optimal VTADJ to achieve minimum temperature drift at a given
power and frequency is the value of VTADJ where the output has
minimum movement.
3.20
3.25
3.30
3.35
3.40
3.45
3.50
3.55
3.60
3.65
3.70
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
OU TPUT VOLTAGE (V)
V
TADJ
VOLTAGE (V)
11287-043
Figure 45. Effect of VTADJ at Various Temperatures, 2.14 GHz, 0 dBm
Var y ing V TADJ has only a very slight effect on VRMS at device
temperatures near 25°C; however, the compensation circuit has
increasing effect as the temperature departs farther from 25°C.
It is important to note that the slope is adjusted vs. temperature.
The pivot point of this is at low input power levels and thereby
moves the VRMS output more at larger input signal levels; that
is, near maximum input power, the temperature drift can be
minimized the most. This is advantageous in most power
measurement cases because errors at larger powers tend to have
more of a negative effect.
The TADJ/PWDN pin has a nominal input resistance of 70 kΩ and
can be conveniently driven from an external source or from an
attenuated value of VREF using a resistor divider. The resistors are
shown in the evaluation board schematic (see Figure 63). The
voltage range for VTADJ is from 0 V to approximately 1.0 V because
approximately 1.3 V is the logic threshold for power down of
the device.
Data Sheet ADL5906
Rev. A | Page 19 of 32
POWER-DOWN INTERFACE
Figure 46 shows a simplified schematic representation of the
TADJ/PWDN interface.
The quiescent and power-down currents for the ADL5906 at
25°C are approximately 68 mA and 250 µA, respectively. The
dual function TADJ/PWDN pin is connected to the temperature
compensation circuit as well as the power-down circuit. The
temperature compensation circuit responds only to voltages
between 0 V and 1 V. When the voltage on this pin is greater than
~1.4 V, the device is fully powered down. Figure 38 shows this
characteristic as a function of VPWDN. The TADJ/PWDN pin with
an internal 70 kresistor to ground sinks approximately 26 µA
at 1.8 V, 47 µA at 3.3 V, and 72 µA at 5 V. The source used to disable
the ADL5906 must have a sufficiently high current capability for
this reason. Figure 31 shows the typical response times for various
RF input levels. The output reaches within 1 dB of its steady state
value in approximately 12 µs for CRMS = 1 nF; however, the reference
voltage is available to full accuracy in a much shorter time. This
wake-up response varies depending on the input coupling and
the value of CRMS.
TEMPERATURE
COMPENSATION
CIRCUIT
ESD
ESD
TADJ/
PWDN
VPOS
GND
TADJ
MAXIMUM
OPERATING
VOLTAGE = 1V
ESD
50k
PW D = P WDN ×
LOGIC
THRESHOLD
~1V ± 0.1V
LOGIC
THRESHOLD
~1.3V ± 0.1V
5
7
20k
1k
1k
70k
SHUTDOWN
CIRCUIT
11287-044
Figure 46. TADJ/PWDN Interface Simplified Schematic
VSET INTERFACE
The VSET interface has a high input impedance of 72 kΩ. The
voltage at VSET is converted to an internal current used to set the
internal VGA gain. The VGA attenuation control is approximately
18 d B / V.
GND
1kΩ
9kΩ
VSET 63k
GAIN ADJUST
11287-045
Figure 47. VSET Interface Simplified Schematic
OUTPUT INTERFACE
The ADL5906 incorporates rail-to-rail output drivers with pull-up
and pull-down capabilities. The level shift circuitry and the output
amplifier are very fast compared to the typical rms response
required by a complex waveform. In essence, the output stage from
the CRMS pin to the VRMS output is only a dc signal because
by definition VRMS is supposed to be a single rms value. The
VRMS pin can source and sink up to 10 mA.
LEVEL
SHIFT
CIRCUITRY
ESD
CRMS
VRMS
ESD
VPOS
GND
ESD
CRMS
EXTERNAL26pF
~2.1V DC BIAS
ITGT
ISQR
2k
500
11287-046
Figure 48. VRMS Interface Simplified Schematic
VTGT INTERFACE
The target voltage can be set with an external source or by
connecting the VREF pin (nominally 2.3 V) to the VTGT pin
through a resistive voltage divider. With 0.8 V on the VTGT pin,
the rms voltage that must be provided by the VGA to balance
the AGC feedback loop is 0.8 V × 0.05 = 40 mV rms. Most of
the characterization information in this data sheet was collected
at VTGT = 0.8 V. Voltages higher and lower than this can be used;
however, doing so increases or decreases the gain at the internal
squaring cell, which results in a corresponding increase or decrease
in intercept. This, in turn, affects the sensitivity and the usable
measurement range, in addition to the sensitivity to different
carrier modulation schemes. As VTGT decreases, the squaring
circuits produce more noise; this becomes noticeable in the output
response at low input signal amplitudes. As VTGT increases,
measurement error due to modulation increases, and temperature
drift tends to decrease. The chosen VTGT value of 0.8 V represents a
compromise between these characteristics.
VTGT 50kΩ
50kΩ
20kΩ
ESD
ESD
ESD
VPOS
GND
ITGT
g × X2
11287-047
Figure 49. VTGT Interface
ADL5906 Data Sheet
Rev. A | Page 20 of 32
BASIS FOR ERROR CALCULATIONS
The slope and intercept used in the error plots are calculated using
the coefficients of a linear regression performed on data collected
in its central operating range. The error plots in the Typical
Performance Characteristics section are shown in two formats:
error from the ideal line and error with respect to the 25°C output
voltage. The error from the ideal line is the decibel difference in
VRMS from the ideal straight-line fit of VRMS calculated by the linear
regression fit over the linear range of the detector, typically at
25°C. The error in decibels is calculated by
Error (dB) = (VRMS Slope × (PIN PZ))/Slope (9)
where PZ is the x-axis intercept expressed in decibels relative to
1 mW (the input amplitude that produces a 0 V output if such an
output were possible).
The error from the ideal line is not a measure of absolute accuracy
because it is calculated using the slope and intercept of each device.
However, it verifies the linearity and the effect of temperature
and modulation on the response of the device. An example of
this type of plot is Figure 9. The slope and intercept that form
the ideal line are those at 25°C with CW modulation. Figure 4,
Figure 5, Figure 7, and Figure 8 show the error with various
popular forms of modulation with respect to the ideal CW
line. This method for calculating error is accurate, assuming
that each device is calibrated at room temperature.
In the second plot format, the VRMS voltage at a given input
amplitude and temperature is subtracted from the corresponding
VRMS at 25°C and then divided by the 25°C slope to obtain an error
in decibels. This type of plot does not provide any information
on the linear-in-dB performance of the device; it merely shows
the decibel equivalent of the deviation of VRMS over temperature,
given a calibration at 25°C. When calculating error from any
one particular calibration point, this error format is accurate. It
is accurate over the full range shown on the plot assuming that
enough calibration points are used. Figure 12 shows this plot type.
The error calculations for Figure 34 are similar to those for the
VRMS plots. The slope and intercept of the VTEMP function vs.
temperature are determined and applied as follows:
Error (°C) = (VTEMP Slope × (Temp TZ))/Slope (10)
where:
VTEMP is the voltage at the TEMP pin at that temperature.
Slope is, typically, 4.8 mV/°C.
Temp is the ambient temperature of the ADL5906 in degrees
Celsius.
TZ is the x-axis intercept expressed in degrees Celsius (the
temperature that would result in a VTEMP of 0 V if this were
possible).
MEASUREMENT MODE BASIC CONNECTIONS
The basic connections circuit for ADL5906 is shown in Figure 51.
The ADL5906 requires a single supply of nominally 5 V. The
supply is connected to the VPOS1 and VPOS2 supply pins.
Decouple each of these pins using two capacitors with values equal
or similar to those shown in Figure 51. Place these capacitors as
close as possible to the VPOS pins. The three no connect pins
(NIC) are not internally connected. Leave these pins unconnected.
An external 60.4 Ω resistor combines with the relatively high RF
input impedance of the ADL5906 to provide a broadband 50 Ω
match. Place an ac coupling capacitor between this resistor and
RFIN+. AC-couple the RFINinput to ground using the same
value capacitor. To operate down to 10 MHz, the coupling
capacitors must be at least 100 pF.
The ADL5906 is placed in measurement mode by connecting
the VRMS pin to the VSET pin. In measurement mode, the output
voltage is proportional to the log of the rms input signal level.
SETTING VTADJ
As described in the Theory of Operation section, the output
temperature drift can be compensated by applying a voltage to
the TADJ pin. The compensating voltage varies with frequency.
The voltage for the TADJ pin can be easily derived from a resistor
divider connected to the VREF pin. Table 4 shows the recommended
VTADJ voltages for operation from −55°C to +125°C, along with
resistor divider values. Resistor values are chosen so that they
neither pull too much current from the VREF pin (IOUTMAX = 4 mA)
nor are so large that the maximum bias current at a VTADJ = 1 V
(14 µA) affects the resulting voltage.
The VTADJ function provides temperature compensation of
theoutput slope of the ADL5906. The Using VTEMP to Improve
Intercept Temperature Drift section describes how the temperature
stability of the ADL5906 can be further improved.
Table 4. Recommended VTADJ Voltages
Frequency VTADJ (V) R9 (Ω) R12 (Ω)
10 MHz to 2.14 GHz 0.35 1500 270
2.6 GHz 0.4 1500 316
3.5 GHz 0.45 1500 365
5.8 GHz 1.0 1540 1200
8 GHz 1.0 1540 1200
10 GHz 1.0 1540 1200
Data Sheet ADL5906
Rev. A | Page 21 of 32
SETTING VTGT
As described in the Theory of Operation section, setting the
voltage on VTGT to 0.8 V represents a compromise between
achieving excellent rms accuracy and maximizing dynamic range.
The voltage on VTGT can be derived from the VREF pin using
a resistor divider, as shown Figure 51. Like the resistors chosen
to set the VTADJ voltage, the resistors setting VTGT must have
reasonable values that do not pull too much current from VREF
or cause bias current errors. In addition, note the combined current
that VREF must deliver to generate the VTADJ and VTGT voltages.
The values shown in Figure 51 and Table 4 result in a maximum
VREF current of 1.7 mA. This current is well below the maximum
specified VREF current of 4 mA.
CHOOSING A VALUE FOR CRMS
CRMS provides the averaging function for the internal rms
computation. Using the minimum value for CRMS allows the
quickest response time to a pulsed waveform but leaves significant
output noise on the output voltage signal. By the same token, a
large filter capacitor reduces output noise but at the expense of
response time.
In applications where response time is not critical, a relatively large
capacitor can be placed on the CRMS pin. In Figure 51, a value
of 0.1 µF is used. For most signal modulation schemes, this value
ensures excellent rms measurement compliance and low residual
output noise. There is no maximum capacitance limit for CRMS.
Figure 50 shows how output noise varies with CRMS when the
ADL5906 is driven by a single-carrier W-CDMA signal (Test
Model TM1-64, peak envelope power = 10.56 dB, bandwidth =
3.84 MHz).
0.1
1
10
100
1000
10000
100000
1000000
0
50
100
150
200
250
300
350
110 100 1000 10000
RISE TIME/FALL TI ME (µs)
OUTPUT NOISE (mV p-p)
C
RMS
(nF)
OUTPUT NOISE (V p-p)
RISE TIME (µs)
FALL TIME (µs)
11287-049
Figure 50. Output Noise, Rise and Fall Times vs. CRMS Capacitance,
Single-Carrier W-CDMA (TM1-64) at 2.14 GHz with PIN = 0 dBm
Figure 50 also shows how the response time is affected by the
value of CRMS. To measure this, an RF burst at 2.14 GHz at 0 dBm
was applied to the ADL5906. The 10% to 90% rise time and
90% to 10% fall time were then measured.
C9
0.1µF
(SEE TEXT)
(AND TABLE)
R9
(SEE TEXT)
(AND TABLE)
X
2
BIAS AND P OWE R
DOWN CONTROL
1
NIC
ITGT
LINEAR-IN-dB VGA
(NEGATIVE SL O PE)
ISQR
26pF
2
VPOS1 VPOS2
3
GND1
VREF VTGT
GND2
4
11
10
9
5
CRMS
6
VRMS
VRMS
7
VSET
8
16
15
14
13
VTEMP
NIC
RFIN–
RFIN+
NIC
EPAD
ADL5906
12
X2
VREF
2.3V
TEMPERATURE
SENSOR
G = 5
R3
60.4Ω
C10
10nF
RFIN
C12
10nF
R12 R11
2kΩ
R10
3.74kΩ
+5V
C3
0.1µF
C4
100pF
C7
0.1µF
C5
100pF
+5V
11287-148
TADJ/
PWDN
Figure 51. Basic Connections for Operation in Measurement Mode
ADL5906 Data Sheet
Rev. A | Page 22 of 32
Table 5. Recommended Minimum CRMS Values for Various Modulation Schemes
Modulation/Standard
Peak Envelope
Power Ratio (dB)
Carrier
Bandwidth (MHz) CRMSMIN (nF)
Output Noise
(mV p-p)
Rise/Fall
Time (µs)
QPSK, 5 MSPS (SQR COS Filter, α = 0.35) 3.8 5 1 84 0.2/10
QPSK ,15 MSPS (SQR COS Filter,
α
= 0.35)
3.8
15
1
42
0.2/10
64 QAM, 1 MSPS (SQR COS Filter, α = 0.35) 7.4 1 10 265 3/85
64 QAM, 5 MSPS (SQR COS Filter, α = 0.35) 7.4 5 1 380 0.2/10
64 QAM, 13 MSPS (SQR COS Filter, α = 0.35) 7.4 13 1 205 0.2/10
W-CDMA, One-Carrier, TM1-64 10.56 3.84 1 820 0.2/10
W-CDMA Four-Carrier, TM1-64, TM1-32, TM1-16, TM1-8 12.08 18.84 1 640 0.2/10
LTE, TM1, One-Carrier, 20 MHz (2048 QPSK Subcarriers) 11.58 20 1 140 0.2/10
Table 5 shows the recommended minimum values of CRMS for
popular modulation schemes. Using lower capacitor values results
in rms measurement errors. Output response time is also shown.
If the output noise shown in Table 5 is unacceptably high, it can
be reduced by
Increasing CRMS
Implementing an averaging algorithm after the output voltage
of the ADL5906 has been sampled by an analog-to-digital
converter (ADC)
The values in Table 5 were experimentally determined to be the
minimum capacitance that ensures good rms accuracy for that
particular signal type. This test was carried out by starting out
with a large capacitance value on the CRMS pin (for example,
10 µF). The value of VRMS was noted for a fixed input power level
(for example, 10 dBm). The value of CRMS was then progressively
reduced (this can be done with press-down capacitors) until
the value of VRMS started to deviate from its original value (this
indicates that the accuracy of the rms computation is degrading
and that CRMS is becoming too small).
In general, the minimum required rms averaging capacitance
increases as the peak-to-average ratio of the carrier increases. The
minimum required CRMS also tends to increase as the bandwidth
of the carrier decreases. With narrow-band carriers, the noise
spectrum of the VRMS output tends to have a correspondingly
narrow profile. The relatively narrow spectral profile demands
a larger value of CRMS that reduces the low-pass corner frequency
of the averaging function and ensures a valid rms computation.
OUTPUT VOLTAGE SCALING
The linear output voltage range of the ADL5906 is nominally
0.3 V to 3.7 V. VRMS is clamped to a maximum voltage of ~3.9 V;
this helps improve falling edge settling speeds because the VRMS
output stays closer to the nominal linear-in-dB output range of
0.3 V to 3.7 V. Within the 0 V to 3.9 V maximum output range,
the slope can be adjusted as needed via extra resistors, as shown
in Figure 52.
If only a part of the RF input power range of the ADL5906 is
being used (for example,10 dBm to 60 dBm), increase the
scaling so that this reduced input range fits into the available
output swing (0 V to 3.9 V) of the ADL5906.
The output swing is reduced by simply adding a voltage divider on
the output pin, as shown in the A side of Figure 52. Reducing the
output scaling can be used when interfacing the ADL5906 to an
ADC with a 0 V to 2.5 V input range.
6
7
VSET
R6
R2
VRMS
6
7
VSET
A B
R1
R15
VRMS
11287-149
Figure 52. Decreasing and Increasing Slope
The output voltage swing can be increased using a technique that is
analogous to setting the gain of an op amp in noninverting mode
(see the B side of Figure 52) with the VSET pin being the equivalent
of the inverting input of the op amp.
With VRMS connected to VSET, the nominal transfer function
of the ADL5906 is given by
VRMS = Slope × (PIN Intercept)
For example at 3.5 GHz, with PIN equal to 0 dBm, the nominal
output voltage is equal to 0.052 V/dB × (0 dBm (−64 dBm) =
3.328 V.
To scale this voltage downward using a resistor divider, choose a
value for R15 and calculate R1 using the following equation:
×= 1
'
RMS
RMS
V
V
R15R1 (11)
Data Sheet ADL5906
Rev. A | Page 23 of 32
To scale this voltage upward, choose a value for R2 and calculate
R6 using the following equation:
= 1)
||
(
RMS
'
RMS
IN V
V
R
R2R6
(12)
where:
RIN is the input resistance of VSET (72 kΩ).
V'RMS is the desired maximum output voltage.
VRMS is the nominal maximum output voltage before scaling
(see Figure 9 through Figure 26).
When choosing R1, R2, R6, and R15, notice the current drive
capability of the VRMS pin and the input resistance of the VSET
pin. The choice of resistors must not be too small because this
results in excessive current drawn out of the VRMS pin (the VRMS
pin can source a maximum current of 10 mA). However, choosing
an R2 that is too large is also problematic. If the value of R2 chosen
is compatible with the input resistance of the VSET pin (72 kΩ),
this input resistance, which varies slightly from part to part,
contributes to the resulting slope and output voltage. In general,
ensure that the value of R2 is at least 10 times smaller than the
input resistance of VSET. Therefore, the values for R6 and R2
must be in the 1 kΩ to 5range. Similar values must be used
for R1 and R15.
It is also important to take into account part-to-part and frequency
variation in output swing along with the maximum output voltage
(3.9 V) of the output stage of the ADL5906. The VRMS part-to-
part distribution is well characterized at major frequency bands
in the Typical Performance Characteristics section (see Figure 12
through Figure 14, Figure 18 through Figure 20, Figure 24, and
Figure 25). The resistor values in Table 6, which were calculated
based on 3.5 GHz operation, have been conservatively chosen so
that there is no chance that the desired output voltage swings
exceed the output swing of the ADL5906 (when scaling upward)
or the input range of a 0 V to 2.5 V ADC (when scaling down-
ward). In each case, the nominal maximum voltage that results is
100 mV below the desired maximum to account for part-to-part
variation and resistor tolerances.
Table 6. Output Voltage Range Scaling Examples at 3.5 GHz
Desired Input Range (dBm)
Slope Increase Slope Decrease
New Slope (mV/dB) Nominal Maximum Output Voltage (V) R6 (Ω) R2 (Ω) R1 (Ω) R15(Ω)
0 to −60
274
2000
59
3.8
−10 to −50 681 2000 70 3.8
0 to −60 787 2000 37 2.4
−10 to −50 348 2000 44 2.4
ADL5906 Data Sheet
Rev. A | Page 24 of 32
SYSTEM CALIBRATION AND ERROR CALCULATION
The measured transfer function of the ADL5906 at 2.14 GHz is
shown in Figure 53, which contains plots of both output voltage
vs. input level and linearity error vs. input level. As the input level
varies from −65 dBm to +5 dBm, the output voltage varies from
~0.25 V to ~3.9 V.
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
OUTPUT VOLTAGE (V)
P
IN
(d Bm)
11287-051
OUTPUT VOLTAGE –4 0°C
OUTPUT VOLTAGE + 25°C
OUTPUT VOLTAGE + 85°C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
Figure 53. 2.14 GHz VRMS and Log Conformance Error at +25°C, −40°C, and
+85°C Using Two-Point Calibration at 0 dBm and 40 dBm
Because slope and intercept vary from device to device, board
level calibration must be performed to achieve high accuracy.
The equation for the idealized output voltage can be written as
VRMS(IDEAL) = Slope × (PIN Intercept) (13)
where:
Slope is the change in output voltage divided by the change in
input power (dB).
Intercept is the calculated input power level at which the output
voltage is equal to 0 V (note that Intercept is an extrapolated
theoretical value and not a measured value).
In general, calibration is performed during equipment manufacture
by applying two or more known signal levels to the input of the
ADL5906 and measuring the corresponding output voltages.
The calibration points must be within the linear operating range
of the device.
With a two-point calibration, the slope and intercept are calculated
as follows:
Slope = (VRMS1VRMS2)/(PIN1 PIN2) (14)
Intercept = PIN1 − (VRMS1/Slope) (15)
After the slope and intercept are calculated and stored in nonvolatile
memory during equipment calibration, an equation can be used
to calculate an unknown input power based on the output
voltage of the detector.
PIN (Unknown) = (VRMS(MEASURED)/Slope) + Intercept (16)
The log conformance error is the difference between this straight
line and the actual performance of the detector.
Error (dB) = (VRMS(MEASURED) VRMS(IDEAL))/Slope (17)
Figure 53 includes a plot of this error at +25°C, 40°C, and +85°C
when using a two-point calibration (calibration points are 0 dBm
and 40 dBm). The error at the calibration points at 25°C (in
this case, −40 dBm and 0 dBm) is equal to 0 dB by definition.
The residual nonlinearity of the transfer function that is apparent
in the two-point calibration error plot can be reduced by
increasing the number of calibration points. Figure 54 shows
the post-calibration error plots for a three-point calibration. With
a multipoint calibration, the transfer function is segmented, with
each segment having its own slope and intercept. Multiple known
power levels (three levels in this case) are applied, and multiple
voltages are measured. When the equipment is in operation, the
measured voltage from the detector is first used to determine
which of the stored slope and intercept calibration coefficients
are to be used. Then, the unknown power level is calculated
by inserting the appropriate slope and intercept values into
Equation 16.
When choosing calibration points, there is no requirement for,
or value in, equal spacing between the points. There is also no
limit to the number of calibration points used. However, when
more calibration points are used, calibration time increases.
OUTPUT VOLTAGE (V)
P
IN
(d Bm)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
OUTPUT VOLTAGE –40°C
OUTPUT VOLTAGE +25°C
OUTPUT VOLTAGE +85°C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
11287-152
V
TADJ
= 0.35V
Figure 54. 2.14 GHz VRMS and Log Conformance Error at +25°C, −40°C, and
+85°C Using Three-Point Calibration at 0 dBm, −40 dBm, and 55 dBm
The 40°C and +85°C error plots in Figure 54 are generated using
the +25°C slope and intercept values. This is consistent with
equipment calibration in a mass production environment where
calibration of multiple temperatures is not practical.
Data Sheet ADL5906
Rev. A | Page 25 of 32
USING VTEMP TO IMPROVE INTERCEPT
TEMPERATURE DRIFT
In applications where VTEMP and VRMS are both being digitized
by an ADC, the VTEMP voltage can be used to further improve
the temperature drift of the ADL5906.
As shown in Figure 54, whereas the slope is stable vs. the
temperature at 2140 MHz, the intercept of the ADL5906 does
vary slightly vs. temperature (approximately +0.3 dB at +85°C
and 0.8 dB at 40°C). This variation in intercept is constant vs.
input power level at most frequencies. Table 7 lists the average
temperature coefficient of VRMS in mV/°C at frequencies from
100 MHz to 5.8 GHz. This temperature coefficient is given by
the following equation:
TCVRMS = (DRIFTVRMS/ΔTEMP) × Slope (18)
where:
DRIFTVRMS is the specified drift of VRMS (scaled in dB) from
ambient to either 40°C or +85°C at an input power level of
0 dBm (see Table 1).
TEMP is equal to either +65°C for cold drift (that is, +25°C −
(−40°C)) or +60°C for hot drift (that is, +85°C − +25°C).
Slope is the specified slope of VRMS (see Table 1).
For example, at 2.14 GHz, TCVRMS for hot drift can be calculated as
TCVRMS = (0.3 dB/60°C) × 56 mV/dB = 0.28 mV/°C
The value for slope that is used can also be the slope that is
calculated during device calibration. This gives results that are
slightly more accurate because there is slight variation in slope
from device to device.
Table 7 also lists the typical temperature coefficient of the VTEMP
temperature sensor output. To calculate the appropriate amount of
compensation required at a particular frequency, a VTEMP weighting
factor is calculated. This is simply the ratio of the temperature
coefficients of VTEMP and VRMS. These weighting factors are
also shown in Table 7.
Using the data shown in Table 7, an adjusted value for VRMS (VRMS)
can be calculated using the following equation:
= FactorWeighting
VV
V'V
TEMP25TEMP
RMSRMS
(19)
where:
VTEMP25 is equal to the voltage measured on VTEMP during system
calibration at ambient temperature.
VTEMP is equal to the voltage on VTEMP during normal operation.
Figure 55 to Figure 62 show typical plots of VRMS vs. input level
and temperature at frequencies from 100 MHz to 5.8 GHz when
this temperature compensation algorithm is applied.
From a system calibration and operation perspective, the only
additional measurements that are required to implement this
algorithm are measurement and storage of VTEMP during calibration
(that is, at ambient temperature) and measurement of VTEMP
during operation. All other information required to implement
this algorithm (that is, nominal temperature drift of VRMS and
temperature coefficient of VTEMP) is based on typical data sheet
specifications.
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
V
RMS
' (V)
P
IN
(d Bm)
V
RMS
' –40°C
V
RMS
' +25°C
V
RMS
' +85°C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
11287-153
V
TADJ
= 0.35V
Figure 55. VRMS’ and Log Conformance Error vs. Input Level and Temperature
at 100 MHz Using VTEMP Intercept Compensation
–65 –55 –45 –35 –25 –15 –5 5
PIN (dBm)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
ERRO R ( dB)
VRMS' (V)
VRMS' –40°C
VRMS' + 25°C
VRMS' + 85°C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
11287-054
VTADJ = 0.35V
Figure 56. VRMS’ and Log Conformance Error vs. Input Level and Temperature
at 700 MHz Using VTEMP Intercept Compensation
ADL5906 Data Sheet
Rev. A | Page 26 of 32
–65–55–45–35–25–15 –5 5
P
IN
(dBm)
–6
–5
–4
3
2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
ERROR (dB)
V
RMS
' (V)
11287-155
V
RMS
'–40°C
V
RMS
' +25°C
V
RMS
'
+85°C
ERROR –40°C
ERROR +25°C
ERROR +85°C
VTADJ = 0.35V
Figure 57. VRMS’ and Log Conformance Error vs. Input Level and Temperature
at 900 MHz Using VTEMP Intercept Compensation
PIN (dBm)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
VRMS' (V)
VRMS' –40°C
VRMS' + 25°C
VRMS' + 85°C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
11287-156
VTADJ = 0.35V
Figure 58. VRMS’ and Log Conformance Error vs. Input Level and Temperature
at 1900 MHz Using VTEMP Intercept Compensation
PIN (dBm)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
VRMS' (V)
11287-057
VRMS' –40°C
VRMS' +25° C
VRMS' +85° C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
VTADJ = 0.35V
Figure 59. VRMS’ and Log Conformance Error vs. Input Level and Temperature
at 2140 MHz using VTEMP Intercept Compensation
PIN (dBm)
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65
–55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
V
RMS
' (V)
V
RMS
' –40°C
V
RMS
' +25°C
V
RMS
' +85°C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
11287-058
V
TADJ
= 0.4V
Figure 60. VRMS’ and Log Conformance Error vs. Input Level and Temperature
at 2600 MHz Using VTEMP Intercept Compensation
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
V
RMS
' (V)
P
IN
(d Bm)
11287-059
V
RMS
' –40°C
V
RMS
'+25°C
V
RMS
' +85° C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
V
TADJ
= 0.45V
Figure 61. VRMS’ and Log Conformance Error vs. Input Level and Temperature
at 3500 MHz Using VTEMP Intercept Compensation
–6
–5
–4
–3
–2
–1
0
1
2
3
4
5
6
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
–65 –55 –45 –35 –25 –15 –5 5
ERRO R ( dB)
V
RMS
' (V)
P
IN
(d Bm)
11287-060
V
RMS
' –40°C
V
RMS
' +25° C
V
RMS
' +85° C
ERRO R –40°C
ERRO R +25°C
ERRO R +85°C
V
TADJ
= 1V
Figure 62. VRMS’ and Log Conformance Error vs. Input Level and Temperature
at 5800 MHz Using VTEMP Intercept Compensation
Data Sheet ADL5906
Rev. A | Page 27 of 32
Table 7. Scaling Factors for Intercept Temperature Drift Compensation Using VTEMP
Frequency
(MHz)
TCVRMS, −40°C to +25°C,
PIN = 0 dBm (mV/°C)
TCVRMS, 25°C to 85°C,
PIN = 0 dBm (mV/°C)
TCVTEMP
(mV/°C)
VTEMP Weighting Factor,
40°C to +25°C
(TCVTEMP/TCVRMS)
VTEMP Weighting Factor,
+25°C to +85°C
(TCVTEMP/TCVRMS)
100 0.72615 0.19667 4.8 6.61017 24.40678
700 0.81692 0.295 4.8 5.87571 16.27119
900 0.72615 0.295 4.8 6.61017 16.27119
1900
0.70154
0.19
4.8
6.84211
25.26316
2140 0.68923 0.28 4.8 6.96429 17.14286
2600 0.76154 0.275 4.8 6.30303 17.45455
3500 1.2 0 4.8 4
5800 1.23931 0.08041 4.8 5.99417 85.287
1TCVRMS based on temperature drift at PIN = −10 dBm.
DESCRIPTION OF CHARACTERIZATION
For a description on how characterization was completed, see the ADL5902 data sheet.
ADL5906 Data Sheet
Rev. A | Page 28 of 32
EVALUATION BOARD
The ADL5906-EVALZ is a fully populated, 4-layer, FR4-
based evaluation board. For normal operation, it requires a
5 V/100 mA power supply. The 5 V power supply must be
connected to the VPOS and GND test loops. The RF input
signal is applied to the SMA connector (RFIN). The output
voltage is available on the SMA connector (VOUT1) or on the
test loop (VOUT). Configuration options for the evaluation
board are listed in Table 8.
X
2
BIAS AND POWER
DOWN CONTROL
1
NIC
I
TGT
LINEAR-IN-dB VGA
(NEGATIVE SLOPE)
I
DET
26pF
2
VPOS1 VPOS2
3
GND1VREF VTGT GND2
4
11
10
9
5
CRMS
C9
0.1µF
6
VRMS
7
VSET
8
16
15
14
13
VTEMP
NIC
RFIN–
RFIN+
NIC
EPAD
ADL5906
12
X
2
V
REF
2.3V
TEMPERATURE
SENSOR
G = 5
R3
60.4
C10
10nF
RFIN
TC2
VOUT
V
OUT1
VREF VTGT
GND
C12
10nF
R12
270
R9
1.5k
R11
2k
R10
3.74k
R6
0
R1
0
R2
(OPEN)
R15
(OPEN)
VSET
V
POS
C3
0.1µF
C4
100pF
C7
0.1µF
C5
100pF
11287-150
TADJ/
PWDN
Figure 63. Evaluation Board Schematic
Table 8. Evaluation Board Configuration Options
Component Function/Notes Default Value
RFIN, R3, C10,
C12
RF input. The evaluation board is configured for single-ended drive on the RFIN+ pin (Pin 14).
Capacitors C10 and C12 have been set large enough so that the full frequency range of the
device is covered. If operation down to 10 MHz is not required, the value of these capacitors
can be reduced.
RFIN = SMA connector,
C10 = C12 = 10 nF,
R3 = 60.4 Ω
VTGT, R10,
R11
VTGT interface. R10 and R11 are set up to provide 0.8 V to VTGT derived from VREF. If R10 and
R11 are removed, an external voltage can be applied on the VTGT test point.
VTGT = black test loop,
R10 = 3.74 kΩ,
R11 = 2 kΩ,
VTGT = 0.8 V
VPOS, GND,
C3, C4, C5,C7
Power supply interface and decoupling. Apply the power supply for the evaluation board to
the VPOS and GND test loops. The nominal supply decoupling consists of a 100 pF capacitor and a
0.1 μF capacitor on each power supply pin, with the 100 pF capacitor placed closer to the pin.
VPOS = red test loop,
GND = black test loop,
C3 = C7 = 0.1 μF,
C4 = C5 = 100 pF
Data Sheet ADL5906
Rev. A | Page 29 of 32
Component Function/Notes Default Value
VOUT, VOUT1,
VSET, R1, R2,
R6, R15
Output interface. In measurement mode, a portion of the voltage at the VRMS pin is fed back
to the VSET pin via R6 (R6 is normally set to 0 Ω). Using the voltage divider created by R2 and
R6, the magnitude of the slope of VRMS is increased by reducing the portion of VRMS that is fed
back to VSET. Resistors R1 and R15 can be used to reduce the output slope.
VOUT = black test loop,
VOUT1 = SMA connector,
VSET = black test loop,
R1 = R6 = 0 Ω,
R15 = R2 = open
In controller mode, R6 must be open. In this mode, the ADL5906 can control the gain of a variable
gain amplifier (VGA) or voltage variable attenuator (VVA). A setpoint voltage is applied to the
VSET test loop, and the VRMS test loop or SMA connector drives the gain control input of the
VGA/VVA.
C9 RMS averaging capacitor. The value of the rms averaging capacitor should be set based on the
peak-to-average ratio of the input signal and based on the desired output response time and
residual output noise.
C9 = 0.1 µF
TC2, R9, R12 TADJ/PWDN interface. The TADJ/PWDN pin controls the slope temperature compensation
and/or shuts down the device. The evaluation board is configured with VTADJ connected to
VREF through a resistor divider (R9, R12). This voltage divider can be removed (or simply
overdriven) allowing for the external application of a voltage to the VTADJ pin by applying a
voltage to the TC2 test point.
TC2 = black test loop,
R9 = 1.5 kΩ, R12 = 270,
VTADJ = 0.35 V
EVALUATION BOARD ASSEMBLY DRAWINGS
11287-055
Figure 64. ADL5906 Evaluation Board Layout, Top Side
11287-056
Figure 65. ADL5906 Evaluation Board Layout, Bottom Side
ADL5906 Data Sheet
Rev. A | Page 30 of 32
OUTLINE DIMENSIONS
COMPLIANT
TO
JEDEC S TANDARDS MO-220- WGGC.
111908-A
1
0.65
BSC
BOTTOM VIEWTOP VI EW
16
5
8
9
1213
4
EXPOSED
PAD
PI N 1
INDICATOR
4.10
4.00 S Q
3.90
0.70
0.60
0.50
SEATING
PLANE
0.80
0.75
0.70 0.05 MAX
0.02 NOM
0.20 RE F
0.25 M IN
COPLANARITY
0.08
PI N 1
INDICATOR
0.35
0.30
0.25
2.25
2.10 S Q
1.95
FOR PRO P E R CONNECTION O F
THE EXPOSED PAD, REFER TO
THE P IN CONFI GURATIO N AND
FUNCTION DES CRIPT IO NS
SECTION OF THIS DATA SHEET.
Figure 66. 16-Lead Lead Frame Chip Scale Package [LFCSP_WQ]
4 mm × 4 mm Body, Very Very Thin Quad
(CP-16-23)
Dimensions shown in millimeters
ORDERING GUIDE
Model1 Temperature Range Package Description Package Option Ordering Quantity
ADL5906ACPZN-R2 −40°C to +105°C 16-Lead Lead Frame Chip Scale Package [LFCSP_WQ] CP-16-23 250
ADL5906ACPZN-R7 −40°C to +105°C 16-Lead Lead Frame Chip Scale Package [LFCSP_WQ] CP-16-23 1,500
ADL5906SCPZN-R7 −55°C to +125°C 16-Lead Lead Frame Chip Scale Package [LFCSP_WQ] CP-16-23 1,500
ADL5906-EVALZ Evaluation Board
1 Z = RoHS Compliant Part.
Data Sheet ADL5906
Rev. A | Page 31 of 32
NOTES
ADL5906 Data Sheet
Rev. A | Page 32 of 32
NOTES
©2013 Analog Devices, Inc. All rights reserved. Trademarks and
registered trademarks are the property of their respective owners.
D11287-0-10/13(A)
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