APN1014 - Skyworks Solutions, Inc.

APPLICATION NOTE
APN1014: A Level Detector Design for
Dual-Band GSM-PCS Handsets
Introduction
Schottky Detector Fundamentals
Schottky diode detectors are commonly used as amplitude
demodulators and level detectors in wireless and other RF and
microwave signal processors. Detector designs are simple
to realize using low-cost, plastic packaged, silicon Schottky
diodes. Figure 1 shows a simple conceptual design.
Schottky Equation
In this application note, we will review detector fundamentals
and show the performance of a broadband detector that
terminates a 50 W transmission line. Finally, a design for a
level detector is presented for use in a dual-band GSM-PCS
handset. This application uses the SMS7630 Zero-Bias Detector
(ZBD) Schottky diode.
Schottky diode detector operation is based on the equation that
characterizes the current-voltage relationship in a diode junction,
as shown:
I = ISAT( e
q (V - IRs )
nKt
-1)
Where: n = ideality factor (typically 1.0)
K = Boltsmann’s constant, 1.38044
X10-23 (joule/Kelvin)
q = electronic charge, 1.60206X10-19
(coulombs)
t = temperature (Kelvin)
RS = series resistance ()
ISAT = saturation current
RF Input
RF Choke
Video Output
Source
50 Ω
Load
>1M
Figure 1. Conceptual Video Detector Circuit
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APPLICATION NOTE • APN1014
This equation may be simplified for a Schottky diode operated as
a zero-biased detector at 300 K, where RS may be neglected and
n = 1.0 to:
I = ISAT ( e 38.6 V -1)
This equation is appropriate for all junction diodes (PN, PIN and
Schottky). However, only for the Schottky diode is this equation
valid at high microwave frequencies — even beyond 100 GHz.
The Schottky diode employs a metal to semiconductor junction
(palladium-silicide on P-type silicon for a ZBD). It is a majority
carrier diode with virtually zero minority carrier lifetime (stored
charge) to inhibit high-frequency performance. PN and PIN
junction diodes have finite minority carrier lifetime precluding
their use as a detector (or mixer) element at microwave
frequencies.
The dynamic resistance of a Schottky diode (the slope of the
I-V characteristic) is a function of forward current and may be
expressed as:
RV =
nKt x 1
q
I
This expression also gives the video resistance of the diode at
zero bias as:
Square Law and Linear Response
The response of a Schottky detector is generally presented as
a curve of detected output voltage vs. applied input power in
a circuit where the detector diode terminates a transmission
line as shown in Figure 1. At small signals, the output voltage
is closely proportional to the input power or the square of
the input voltage. This is called the square law region. In this
region, a 10 dB increase in input power results in a 10 times
increase in output voltage. At large input signals, the detector
voltage is more directly proportional to the input RF voltage.
This is the linear region, and it is where a 10 dB increase in
input power results in a 5 times increase in output voltage.
Figure 2 demonstrates this effect.
In a typical level detector, where the video load impedance is
much higher than the video resistance of the Schottky diode, the
square law region occurs when the output voltage is less than
10 mV. The linear region begins at about 100 mV output voltage.
It is more accurate to describe the borders of these regions
based on output voltage rather than input power. Output voltage
is independent of matching, coupling and source impedance.
The Zero Bias Detector (ZBD)
RV = 0.026n
ISAT
10000
The video resistance value may then be calculated directly from
saturation current.
As a detector, the Schottky diode’s performance has been
analyzed by simulating the application of a sinusoidal signal
at a DC operating point and deriving the generated nonsinusoidal response. Because of the nonlinear nature of the diode
equation, this response is not sinusoidal but is rich in harmonics.
Among the second order terms is a DC component, which is a
measure of the magnitude of the applied signal and becomes the
generated detector signal.
Output Voltage (V)
Linear
1000
100
10
1
Square Law
0.1
-40
-30
-20
-10
0
Incident Power (dBm)
Figure 2. Square Law and Linear Regions
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APPLICATION NOTE • APN1014
Silicon Schottky diodes are distinguished by their barrier height
and are determined by the different metals used in forming
the metal-semiconductor junction. Silicon Schottky diodes are
available in ZBD, low, medium, and high barrier designs. The
primary electrical differences, for the same junction area (capacitance), is the higher the barrier the higher the forward voltage.
For Schottky diodes used as mixers, the performance benefit of
the higher barrier diode is wider dynamic range (lower distortion).
Consequently, a higher barrier diode requires higher local oscillator power.
All Schottky diodes operating at zero external bias generate
virtually the same open circuit detector voltage at the same input
power. In this respect, all Schottky diodes may be considered
zero-bias detectors. However, the SMS7630 ZBD at zero bias has
a video resistance value of typically 3500 . At zero bias, the
video resistance for the SMS7621, a low barrier Schottky diode
with similar capacitance, is about 650 k. In many applications,
the video load resistance presented by an operational amplifier is
100 k or less. In this configuration, system sensitivity using the
SMS7630 ZBD is significantly better.
Detector Performance
The SMS7630-079 diode has been evaluated in the detector
circuit shown in Figure 3 with the Schottky diode terminating a
50  line. Data were taken from 100 MHz to 10 GHz at power
levels from -30 dBm to +15 dBm. The SC-79 packaged diode
was attached to the terminal of a 3.5 mm connector and the
output voltage was measured through a HP11612A bias TEE on a
voltmeter with 10 M input resistance.
The results in Figure 3 show that, with no attempt at matching,
this low-cost device gives a flat response generating approximately 30 mV at -20 dBm across this wide frequency band.
The voltage peak at 5 GHz is due to a resonance of the SC-79
package inductance with the diode junction capacitance. This
results in higher RF voltage across the diode junction.
Improved detector sensitivity may be achieved by maximizing
the RF voltage on the diode junction. This is accomplished by
increasing the source impedance. For the SMS7630 with 500 
source impedance at -20 dBm input power, the output voltage
will be about 130 mV, which is more than 4 times higher than
with a 50  source impedance. This type of matching is not the
same as the traditional conjugate power match and a consequence of high detector sensitivity is high SWR.
Video Output
HP11612A
RF Input
SMS7630
10
10
1
1
Output Voltage (V)
Output Voltage (V)
Source
50 Ω
0.1
5 GHz
0.01
PIN +10 dBm
PIN 0 dBm
0.1
PIN -10 dBm
PIN -20 dBm
0.01
10 GHz
1 GHz
0.001
0.001
-30
-20
-10
0
10
0.1
Input Power (dBm)
1.0
10.0
Frequency (GHz)
Figure 3. Unmatched Detector and Measurements
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APPLICATION NOTE • APN1014
.Schottky
Diode Model
The SPICE model is a reliable representation of the Schottky
diode. For the SMS7630, the SPICE model parameters are
presented in Table 1.
Parameter
Description
Unit
SMS7630
& Default
SMS1546
& Default
IS
Saturation current
A
5E-6
3E-7
RS
Series resistance

20
4
N
Emission coefficient (not used)
-
1.05
1.04
TT
Transit time (not used)
S
1E-11
1E-11
CJO
Zero-bias junction capacitance (not used)
F
1.4E-13
3.8E-13
VJ
Junction potential (not used)
V
0.34
0.51
M
Grading coefficient (not used)
-
0.4
0.36
EG
Energy gap (with XTI, helps define the dependence of IS on temperature)
EV
0.69
0.69
XTI
Saturation current temperature exponent
(with EG, helps define the dependence of IS on temperature)
-
2
2
KF
Flicker noise coefficient (not used)
-
0
0
AF
Flicker noise exponent (not used)
-
1
1
FC
Forward bias depletion capacitance coefficient (not used)
-
0.5
0.5
BV
Reverse breakdown voltage (not used)
V
2
2.5
IBV
Current at reverse breakdown voltage (not used)
A
1e-4
1e-5
ISR
Recombination current parameter (not used)
A
0
0
NR
Emission coefficient for ISR (not used)
-
2
2
IKF
High injection knee current (not used)
A
Infinity
Infinity
NBV
Reverse breakdown ideality factor (not used)
-
1
1
IBVL
Low-level reverse breakdown knee current (not used)
A
0
0
NBVL
Low-level reverse breakdown ideality factor (not used)
-
1
1
TNOM
Nominal ambient temperature at which these model parameters were derived
°C
27
27
FFE
Flicker noise frequency exponent (not used)
1
1
Table 1. Silicon PN Diode Values in Libra IV Assumed for SMS7630 and SMS1546 Models
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APPLICATION NOTE • APN1014
The power response at 1 GHz was modeled using these SPICE
parameters in a Libra IV platform and using the methodology
in Reference 1 showing good compliance of both methods to
measured values. This is shown in Figure 4.
Output Voltage (V)
10000
The consequence of this design is twice the video resistance, Rv,
in comparison to a single diode detector. This does not detract
from the performance because the RV value for a single ZBD
Schottky diode is about 5 k — much lower than the input
impedance of the typical operational amplifier following the
detector. Higher order voltage multipliers may be designed using
the same principle.
In the Libra IV model shown in Figure 6, the SMS7630-079
Schottky diodes DIOD1 and DIOD2 are used in a voltage doubler
configuration. Capacitors C4 and C5, and inductors L1 and L2
simulate the effect of the SC79 package. Capacitor C2 reflects
the mounting pad capacitance. The RF coupling is realized
through a high impedance resistive voltage divider, consisting of
two resistors.
1000
100
10
1
-30
-20
-10
0
RF Input
Incident Power (dBm)
VOUT (Ref. 1)
VOUT (SPICE)
D1–D2 SMS7630-079
10
VOUT (Meas.)
Figure 4. Detector Output Voltage
Dual-Band GSM-PCS Level Detector Design
A detector design was initiated to generate approximately 10 mV
at 10 dBm input power using a low-loss coupled structure for use
as a level detector. The frequency coverage would encompass
the GSM and PCS bands for typical usage in a dual-band
handset.
Figure 5 shows the design that uses two Schottky diodes in a
voltage doubler configuration. In the voltage doubler, the RF
voltage is applied to the parallel connection of two diodes, each
diode generating the same rectified voltage. The video output is
extracted from the series connection of the two diodes thus its
magnitude is twice that of a single diode.
RF Output
C1
10 p
R1
3 k
C2
100 p
D1
D2
V DET
R3
56 k
C3
100 p
R2
100
Figure 5. Level Detector Circuit Diagram
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APPLICATION NOTE • APN1014
20
Figure 6. Level Detector Circuit Model
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APPLICATION NOTE • APN1014
Figure 7. Detector PCB Layout
PRC1 = 3 k, and SRLC2 = 100 . The total impedance of the
divider is 3500 , causing about a 0.06 dB loss in the transmission path from Port 1 to Port 2. Capacitors SRLC1 and SRLC2
are used to prevent DC current leakage.
The PCB layout is shown in Figure 7, and the Bill of Materials is
shown in Table 2.
Designator
Value
Part Number
Footprint
C1
10 p
CM05CG100K10AB
0402
AVX
Manufacturer
C2
100 p
CM05CG5101K10AB
0402
AVX
C3
100 p
CM05CG5101K10AB
0402
AVX
R1
3 k
CR05-302J-T
0402
AVX/KYOCERA
R2
100 
CR05-101J-T
0402
AVX/KYOCERA
R3
56 k
CR05-563J-T
0402
AVX/KYOCERA
D1
SMS7630-079
SMS7630-079
SC-79
Skyworks Solutions
D2
SMS7630-079
SMS7630-079
SC-79
Skyworks Solutions
Table 2. Bill of Materials
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APPLICATION NOTE • APN1014
Dual-Band Detector Performance
In the 800 MHz to 1 GHz band the detector was flat within
0.10 dB; between 1.8 GHz and 2 GHz flatness was better than
0.15 dB.
In Figure 8, the measured detector DC output voltage is shown
vs. input power in the through line at 1 GHz simulating the GSM
band and at 2 GHz simulating the PCS band. Both measured
and simulated results agree. A useful dynamic range of 32 dB is
achieved based on an output voltage range from 10 mV to 2 V.
The through line insertion loss of the detector is less than 0.3
dB at frequencies below 1 GHz and less than 0.4 dB in the
band between 1.8 GHz and 2.0 GHz. Figure 9 shows that this
difference agrees well with the loss model used in the simulation.
The coupling ratio of this detector circuit is about 37 dB in a
50  environment. This circuit may be modified by changing
the through line resistors R1 and R2. This allows the designer to
achieve the same output voltage performance at different input
power levels. Table 3 demonstrates the flatness of the frequency
response at different signal levels.
10
0
-0.1
1
S21 (dB)
Detected Voltage (V)
Delta (Simu)
0.1
Delta
Without Coupling
-0.2
-0.3
With Coupling
0.01
-0.4
0.001
-0.5
0
5
15
10
20
25
30
35
40
0.5
Input Power (dBm)
1.0
1.5
2.0
2.5
3.0
Frequency (GHz)
VOUT @ 1 GHz (Simu)
VOUT @ 2 GHz (Simu)
VOUT @ 1 GHz (Meas)
VOUT @ 2 GHz (Meas)
Figure 9. Detector Loss vs. Frequency
Figure 8. Detector Output Voltage vs. Input Power
VOUT
mV
VOUT
mV
VOUT
mV
VOUT
mV
VOUT
mV
VOUT
mV
800 MHz
1 GHz
1.2 GHz
1.8 GHz
2 GHz
2.2 GHz
-10 dBm
0.131
0.129
0.128
0.122
0.118
0.112
0 dBm
1.24
1.23
1.22
1.21
1.18
1.13
5 dBm
4.15
4.13
4.11
3.88
3.84
3.12
10 dBm
12.23
12.21
11.99
11.91
11.53
11.39
15 dBm
34.81
34.62
34.33
33.77
33.65
33.53
20 dBm
91.38
91.36
91.35
88.86
86.51
83.91
30 dBm
422.65
422.61
422.15
421.38
419.38
405.31
Input Power
Table 3. Detector Frequency Response
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APPLICATION NOTE • APN1014
Conclusion
References
This application note demonstrates a detector design that may
be used for level setting in a dual-band handset. It operates
with frequency flatness better than 0.15 dB in any band. The
design utilizes two low-cost, plastic packaged SMS7630-079
ZBD Schottky diodes in a voltage doubler. Although intended for
GSM-PCS service, the design is appropriate for any dual-band
applications covering 800 MHz to 2.4 GHz.
R.G. Harrison, X. LePolozec, “Nonsquarelaw Behavior of Diode
Detectors Analyzed by the Ritz-Galerkin Method,” IEEE Trans.
Microwave Theory, May 1994.
List of Available Documents
The Level Detector Simulation Project Files for Libra I V.
The Level Detector PCB Gerber Photo-plot files.
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APPLICATION NOTE • APN1014
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