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HSMS-2855 Datasheet(PDF) 5 Page - Agilent(Hewlett-Packard)

Part # HSMS-2855
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-2855 Datasheet(HTML) 5 Page - Agilent(Hewlett-Packard)

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Applications Information
Introduction
Agilent’s HSMS-285x family of
Schottky detector diodes has been
developed specifically for low
cost, high volume designs in small
signal (Pin < -20 dBm) applica-
tions at frequencies below
1.5 GHz. At higher frequencies,
the DC biased HSMS-286x family
should be considered.
In large signal power or gain con-
trol applications (Pin > -20 dBm),
the HSMS-282x and HSMS-286x
products should be used. The
HSMS-285x zero bias diode is not
designed for large signal designs.
Schottky Barrier Diode
Characteristics
Stripped of its package, a
Schottky barrier diode chip
consists of a metal-semiconductor
barrier formed by deposition of a
metal layer on a semiconductor.
The most common of several
different types, the passivated
diode, is shown in Figure 5, along
with its equivalent circuit.
Figure 5. Schottky Diode Chip.
RS is the parasitic series
resistance of the diode, the sum of
the bondwire and leadframe
resistance, the resistance of the
bulk layer of silicon, etc. RF
energy coupled into RS is lost as
heat — it does not contribute to
the rectified output of the diode.
CJ is parasitic junction capaci-
tance of the diode, controlled by
the thickness of the epitaxial layer
and the diameter of the Schottky
contact. R j is the junction
resistance of the diode, a function
of the total current flowing
through it.
8.33 X 10-5 nT
Rj = –––––––––––– = RV – R s
IS + Ib
0.026
= ––––– at 25
°C
IS + Ib
where
n = ideality factor (see table of
SPICE parameters)
T = temperature in
°K
IS = saturation current (see
table of SPICE parameters)
Ib = externally applied bias
current in amps
IS is a function of diode barrier
height, and can range from
picoamps for high barrier diodes
to as much as 5
µA for very low
barrier diodes.
The Height of the Schottky
Barrier
The current-voltage characteristic
of a Schottky barrier diode at
room temperature is described by
the following equation:
V - IRS
I = IS (exp
(––––––) - 1)
0.026
On a semi-log plot (as shown in
the Agilent catalog) the current
graph will be a straight line with
inverse slope 2.3 X 0.026 = 0.060
volts per cycle (until the effect of
RS is seen in a curve that droops
at high current). All Schottky
diode curves have the same slope,
but not necessarily the same value
of current for a given voltage. This
is determined by the saturation
current, IS, and is related to the
barrier height of the diode.
Through the choice of p-type or
n-type silicon, and the selection of
metal, one can tailor the charac-
teristics of a Schottky diode.
Barrier height will be altered, and
at the same time CJ and RS will be
changed. In general, very low
barrier height diodes (with high
values of IS, suitable for zero bias
applications) are realized on
p-type silicon. Such diodes suffer
from higher values of RS than do
the n-type. Thus, p-type diodes are
generally reserved for small signal
detector applications (where very
high values of RV swamp out high
RS) and n-type diodes are used for
mixer applications (where high
L.O. drive levels keep RV low).
Measuring Diode Parameters
The measurement of the five
elements which make up the low
frequency equivalent circuit for a
packaged Schottky diode (see
Figure 6) is a complex task.
Various techniques are used for
each element. The task begins
with the elements of the diode
chip itself.
LP
RS
RV
Cj
CP
FOR THE HSMS-285x SERIES
CP = 0.08 pF
LP = 2 nH
Cj = 0.18 pF
RS = 25 Ω
RV = 9 KΩ
Figure 6. Equivalent Circuit of a
Schottky Diode.
RS
Rj
Cj
;;
METAL
SCHOTTKY JUNCTION
PASSIVATION
PASSIVATION
N-TYPE OR P-TYPE EPI
LAYER
N-TYPE OR P-TYPE SILICON SUBSTRATE
CROSS-SECTION OF SCHOTTKY
BARRIER DIODE CHIP
EQUIVALENT
CIRCUIT


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