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HSMS-285L-BLKG Datasheet(PDF) 7 Page - Agilent(Hewlett-Packard)

Part # HSMS-285L-BLKG
Description  Surface Mount Zero Bias Schottky Detector Diodes
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Manufacturer  HP [Agilent(Hewlett-Packard)]
Direct Link  http://www.home.agilent.com
Logo HP - Agilent(Hewlett-Packard)

HSMS-285L-BLKG Datasheet(HTML) 7 Page - Agilent(Hewlett-Packard)

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7
Since no external bias is used
with the HSMS-285x series, a
single transfer curve at any given
frequency is obtained, as shown in
Figure 2.
The most difficult part of the
design of a detector circuit is the
input impedance matching
network. For very broadband
detectors, a shunt 60
Ω resistor
will give good input match, but at
the expense of detection
sensitivity.
When maximum sensitivity is
required over a narrow band of
frequencies, a reactive matching
network is optimum. Such net-
works can be realized in either
lumped or distributed elements,
depending upon frequency, size
constraints and cost limitations,
but certain general design
principals exist for all types.[3]
Design work begins with the RF
impedance of the HSMS-285x
series, which is given in Figure 9.
1 GHz
2
3
4
5
6
0.2
0.6
1
2
5
Figure 9. RF Impedance of the
HSMS-285x Series at -40 dBm.
915 MHz Detector Circuit
Figure 10 illustrates a simple
impedance matching network for
a 915 MHz detector.
65nH
100 pF
VIDEO
OUT
RF
INPUT
WIDTH = 0.050"
LENGTH = 0.065"
WIDTH = 0.015"
LENGTH = 0.600"
TRANSMISSION LINE
DIMENSIONS ARE FOR
MICROSTRIP ON
0.032" THICK FR-4.
Figure 10. 915 MHz Matching
Network for the HSMS-285x Series
at Zero Bias.
A 65 nH inductor rotates the
impedance of the diode to a point
on the Smith Chart where a shunt
inductor can pull it up to the
center. The short length of 0.065"
wide microstrip line is used to
mount the lead of the diode’s
SOT-323 package. A shorted shunt
stub of length <
λ/4 provides the
necessary shunt inductance and
simultaneously provides the
return circuit for the current gen-
erated in the diode. The imped-
ance of this circuit is given in
Figure 11.
FREQUENCY (GHz): 0.9-0.93
Figure 11. Input Impedance.
The input match, expressed in
terms of return loss, is given in
Figure 12.
0.9
-20
FREQUENCY (GHz)
0.915
0
-10
-15
0.93
-5
Figure 12. Input Return Loss.
As can be seen, the band over
which a good match is achieved is
more than adequate for 915 MHz
RFID applications.
Voltage Doublers
To this point, we have restricted
our discussion to single diode
detectors. A glance at Figure 8,
however, will lead to the sugges-
tion that the two types of single
diode detectors be combined into
a two diode voltage doubler[4]
(known also as a full wave recti-
fier). Such a detector is shown in
Figure 13.
VIDEO OUT
Z-MATCH
NETWORK
RF IN
Figure 13. Voltage Doubler Circuit.
Such a circuit offers several
advantages. First the voltage
outputs of two diodes are added
in series, increasing the overall
value of voltage sensitivity for the
network (compared to a single
diode detector). Second, the RF
impedances of the two diodes are
added in parallel, making the job
of reactive matching a bit easier.
[3] Agilent Application Note 963, Impedance Matching Techniques for Mixers and Detectors.
[4] Agilent Application Note 956-4, Schottky Diode Voltage Doubler.
[5] Agilent Application Note 965-3, Flicker Noise in Schottky Diodes.


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