HSMS-2822-TR1G Avago Technologies US Inc., HSMS-2822-TR1G Datasheet - Page 5

• Manufacturer Part Number: HSMS-2822-TR1G
• Description: DIODE SCHOTTKY RF SER 15V SOT-23
• Manufacturer: Avago Technologies US Inc.

Specifications of HSMS-2822-TR1G

• Package / Case: SOT-23-3, TO-236-3, Micro3™, SSD3, SST3
• Diode Type: Schottky - 1 Pair Series Connection
• Voltage - Peak Reverse (max): 15V
• Current - Max: 1A
• Capacitance @ Vr, F: 1pF @ 0V, 1MHz
• Resistance @ If, F: 12 Ohm @ 5mA, 1MHz
• Product: Schottky Diodes
• Peak Reverse Voltage: 15 V
• Forward Continuous Current: 1 A
• Configuration: Dual Series
• Forward Voltage Drop: 0.5 V @ 0.01 A
• Maximum Reverse Leakage Current: 0.1 uA @ 1 V
• Operating Temperature Range: + 150 C
• Mounting Style: SMD/SMT
• Capacitance Ct: 1pF
• Diode Case Style: SOT-23
• No. Of Pins: 3
• Breakdown Voltage: 15V
• Forward Voltage: 340mV
• Leaded Process Compatible: Yes
• Rohs Compliant: Yes
• Forward Current If Max: 1A
• Forward Voltage Vf Max: 340mV
• Lead Free Status / RoHS Status: Lead free / RoHS Compliant
• Power Dissipation (max): -
• Lead Free Status / Rohs Status: Lead free / RoHS Compliant
• Other names: 516-1818-2; HSMS-2822-TR1G

5
Applications Information
Product Selection
Avago’s family of surface mount Schottky diodes provide
unique solutions to many design problems. Each is opti‑
mized for certain applications.
The first step in choosing the right product is to select
the diode type. All of the products in the HSMS‑282x fam‑
ily use the same diode chip–they differ only in package
configuration. The same is true of the HSMS‑280x, ‑281x,
285x, ‑286x and ‑270x families. Each family has a different
set of characteristics, which can be compared most easily
by consulting the SPICE parameters given on each data
sheet.
The HSMS‑282x family has been optimized for use in RF
applications, such as
• DC biased small signal detectors to 1.5 GHz.
• Biased or unbiased large signal detectors (AGC or
• Mixers and frequencymultipliers to 6 GHz.
The other feature of the HSMS‑282x family is its unit‑to‑unit
and lot‑to‑lot consistency. The silicon chip used in this
series has been designed to use the fewest possible pro‑
cessing steps to minimize variations in diode characteris‑
tics. Statistical data on the consistency of this product, in
terms of SPICE parameters, is available from Avago.
For those applications requiring very high breakdown
voltage, use the HSMS‑280x family of diodes. Turn to the
HSMS‑281x when you need very low flicker noise. The
HSMS‑285x is a family of zero bias detector diodes for small
signal applications. For high frequency detector or mixer
applications, use the HSMS‑286x family. The HSMS‑270x
is a series of specialty diodes for ultra high speed clipping
and clamping in digital circuits.
Schottky Barrier Diode Characteristics
Stripped of its package, a Schottky barrier diode chip
consists of a metal‑semiconductor barrier formed by de‑
position of a metal layer on a semiconductor. The most
common of several different types, the passivated diode,
is shown in Figure 10, along with its equivalent circuit.
R
of the bondwire and leadframe resistance, the resistance
of the bulk layer of silicon, etc. RF energy coupled into R
is lost as heat—it does not contribute to the rectified out‑
put of the diode. C
diode, controlled by the thick‑ness of the epitaxial layer
and the diameter of the Schottky contact. R
tion resistance of the diode, a function of the total current
flowing through it.
S
is the parasitic series resistance of the diode, the sum
power monitors) to 4 GHz.
J
is parasitic junction capacitance of the
j
is the junc‑
S
where
n = ideality factor (see table of SPICE parameters)
T = temperature in °K
I
I
R
I
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:
On a semi‑log plot (as shown in the Avago 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 R
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, I
height of the diode.
Through the choice of p‑type or n‑type silicon, and the
selection of metal, one can tailor the characteristics 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.
Figure 10. Schottky Diode Chip.
S
b
S
N-TYPE OR P-TYPE SILICON SUBSTRATE
v
= saturation current (see table of SPICE parameters)
is a function of diode barrier height, and can range from
= externally applied bias current in amps
N-TYPE OR P-TYPE EPI
PASSIVATION
= sum of junction and series resistance, the slope of the
R
R
V‑I curve
CROSS-SECTION OF SCHOTTKY
I = I
I = I
j
j
≈ ––––– at 25 °C
≈ ––––– at 25 °C
= –––––––––––– = R
= –––––––––––– = R
0.026
0.026
BARRIER DIODE CHIP
8.33 X 10
8.33 X 10
I
I
S
S
S
S
(e
(e
+ I
+ I
I
I
METAL
SCHOTTKY JUNCTION
–––––
–––––
0.026
0.026
V - IR
V - IR
S
b
S
b
+ I
+ I
HSMS-285A/6A fig 9
LAYER
-5
S
-5
S
b
b
PASSIVATION
– 1)
– 1)
nT
nT
S
, and is related to the barrier
V
V
– R
– R
EQUIVALENT
C
j
R
CIRCUIT
s
s
S
R
j
S
is seen