AVAGO HBAT-540B-BLKG High performance schottky diode for transient suppression Datasheet

HBAT-5400, 5402, 540B, 540C
High Performance Schottky Diode
for Transient Suppression
Data Sheet
Description
Features
The HBAT-540x series of Schottky diodes, commonly
referred to as clipping /clamping diodes, are optimal for
circuit and waveshape preservation applications with
high speed switching. Low series resistance, R S, makes
them ideal for protecting sensitive circuit elements
against high current transients carried on data lines.
With picosecond switching, the HBAT-540x can respond
to noise spikes with rise times as fast as 1 ns. Low capacitance minimizes waveshape loss that causes signal degradation.
• Ultra-low Series Resistance for Higher Current
Handling
Package Lead Code ­Identification (Top View)
SINGLE
3
1
0, B
SERIES
3
2
COMMON
ANODE
3
1
E
2
1
2, C
2
COMMON
CATHODE
3
1
F
2
• Low Capacitance
• Low Series Resistance
• Lead-free Option Available
Applications
RF and computer designs that require circuit protection,
high-speed switching, and voltage clamping.
Absolute Maximum Ratings, TA= 25ºC
Symbol
Unit
DC Forward Current
mA
220
430
A
1.0
1.0
IF
IF- peak
PT
Absolute Maximum [1]
HBAT-5400/-5402
HBAT-540B/-540C
Parameter
Peak Surge Current (1µs pulse)
mW
250
825
PINV
Peak Inverse Voltage
Total Power Dissipation
V
30
30
TJ
Junction Temperature
°C
150
150
TSTG
Storage Temperature
°C
-65 to 150
-65 to 150
θ JC
Thermal Resistance, junction to lead
°C/W
500
150
Note:
1. Operation in excess of any one of these conditions may result in permanent damage to the device.
Linear and Non-linear SPICE Model[2]
SPICE Parameters
0.08 pF
2 nH
Parameter
RS
SPICE model
Unit
BV
V
40
CJO
pF
3.0
EG
eV
0.55
IBV
A
10E-4
IS
A
1.0E-7
N
Note:
2. To effectively model the packaged HBAT-540x product, please refer to
Application Note AN1124.
Value
1.0
RS
Ω
2.4
PB
V
0.6
PT
2
M
0.5
HBAT-540x DC Electrical Specifications, TA = +25°C[1]
Part
Package
Number
Marking
Lead
HBAT-Code [2]
Code Configuration Package
VF (mV)
-5400
V0
-540B
-5402
0
Single
B
V2
2
Series
-540C
C
Maximum
Forward
Voltage
VBR (V)
Minimum
Breakdown
Typical
Voltage
Capacitance
C T (pF)
R S (Ω)
Typical
Series
Resistance
t (ps)
Maximum
Eff. Carrier
Lifetime
2.4
100[6]
SOT-23
SOT-323
(3-lead SC-70)
800 [3]
30[4]
3.0[5]
SOT-23
SOT-323
(3-lead SC-70)
Notes:
1. T = +25°C, where T is defined to be the temperature at the package pins where contact is made to the circuit board.
2. Package marking code is laser marked.
3. IF = 100 mA; 100% tested
4. IR = 100 µA; 100% tested
5. VF = 0; f =1 MHz
6. Measured with Karkauer method at 20 mA guaranteed by design.
A
A
Typical Performance
10
1
0.1
0.01
TA = +75C
TA = +25C
TA = –25C
0
0.1
0.2
0.3
0.4
0.5
100
10
1
0.1
0.01
0.6
TJ – JUNCTION TEMPERATURE (C)
500
100
IF – FORWARD CURRENT (mA)
IF – FORWARD CURRENT (mA)
300
TA = +75C
TA = +25C
TA = –25C
0
VF – FORWARD VOLTAGE (V)
0.2
0.4
0.6
0.8
1.0
1.2
160 Max. safe junction temp.
140
120
100
80
60
40
0
1.4
IF – FORWARD CURRENT (mA)
Figure 1. Forward Current vs. Forward Voltage at
Temperature for HBAT-5400 and HBAT-5402.
TA = +75C
TA = +25C
TA = –25C
20
0
50
100
150
200
Figure 2. Forward Current vs. Forward Voltage at
Temperature for HBAT-540B and HBAT-540C.
Figure 3. Junction Temperature vs. Current as a
Function of Heat Sink Temperature for HBAT-5400
and HBAT-5402.
3.0
CT – TOTAL CAPACITANCE (pF)
Tj – JUNCTION TEMPERATURE (C)
Note: Data is calculated from SPICE parameters.
160 Max. safe junction temp.
140
120
100
80
60
40
TA = +75C
TA = +25C
TA = –25C
20
0
0
100
200
300
400
500
2.5
2.0
1.5
1.0
600
IF – FORWARD CURRENT (mA)
0
5
10
15
20
VR – REVERSE VOLTAGE (V)
Figure 4. Junction Temperature vs. Current as a
Function of Heat Sink Temperature for HBAT-540B
and HBAT-540C.
Figure 5. Total Capacitance vs. Reverse Voltage.
Note: Data is calculated from SPICE parameters.
Device Orientation For Outlines SOT-23/323
4 mm
CARRIER
TAPE
USER
FEED
DIRECTION
COVER TAPE
END VIEW
TOP VIEW
REEL
8 mm
ABC
ABC
ABC
250
IF – FORWARD CURRENT (mA)
ABC
Note: "AB" represents package marking code.
"C" represents date code.
Recommended PCB Pad Layout for Avago’s
Package Dimensions
SOT‑23 Products
Outline SOT-23
e2
XXX
E
E1
0.079
2.0
e
L
B
0.035
0.9
C
DIMENSIONS (mm)
D
SYMBOL
A
A1
B
C
D
E1
e
e1
e2
E
L
A
A1
Notes:
XXX-package marking
Drawings are not to scale
MIN.
0.79
0.000
0.37
0.086
2.73
1.15
0.89
1.78
0.45
2.10
0.45
0.031
0.8
MAX.
1.20
0.100
0.54
0.152
3.13
1.50
1.02
2.04
0.60
2.70
0.69
Dimensions in
Tape Dimensions and Product Orientation For Outline SOT-23
P
P2
D
E
P0
F
W
D1
t1
Ko
9° MAX
DESCRIPTION
13.5° MAX
8° MAX
B0
A0
SYMBOL
SIZE (mm)
SIZE (INCHES)
CAVITY
LENGTH
WIDTH
DEPTH
PITCH
BOTTOM HOLE DIAMETER
A0
B0
K0
P
D1
3.15 ± 0.10
2.77 ± 0.10
1.22 ± 0.10
4.00 ± 0.10
1.00 + 0.05
0.124 ± 0.004
0.109 ± 0.004
0.048 ± 0.004
0.157 ± 0.004
0.039 ± 0.002
PERFORATION
DIAMETER
PITCH
POSITION
D
P0
E
1.50 + 0.10
4.00 ± 0.10
1.75 ± 0.10
0.059 + 0.004
0.157 ± 0.004
0.069 ± 0.004
CARRIER TAPE
WIDTH
THICKNESS
W
t1
8.00 +0.30 –0.10
0.229 ± 0.013
0.315 +0.012 –0.004
0.009 ± 0.0005
DISTANCE
BETWEEN
CENTERLINE
CAVITY TO PERFORATION
(WIDTH DIRECTION)
F
3.50 ± 0.05
0.138 ± 0.002
CAVITY TO PERFORATION
(LENGTH DIRECTION)
P2
2.00 ± 0.05
0.079 ± 0.002
0.039
1
0.039
1
e1
inches
mm
Package Dimensions
Recommended PCB Pad Layout for Avago’s
Outline SOT-323 (SC-70 3 Lead)
SC70 3L/SOT-323 Products
e1
0.026
XXX
E
E1
e
0.079
L
B
C
D
0.039
DIMENSIONS (mm)
A
A1
Notes:
XXX-package marking
Drawings are not to scale
SYMBOL
A
A1
B
C
D
E1
e
e1
E
L
MIN.
MAX.
0.80
1.00
0.00
0.10
0.15
0.40
0.10
0.20
1.80
2.25
1.10
1.40
0.65 typical
1.30 typical
1.80
2.40
0.425 typical
0.022
Dimensions in inches
Tape Dimensions and Product Orientation For Outline SOT-323 (SC-70 3 Lead)
P
P2
D
P0
E
F
W
C
D1
t1 (CARRIER TAPE THICKNESS)
K0
8° MAX.
A0
DESCRIPTION
8° MAX.
B0
SYMBOL
SIZE (mm)
SIZE (INCHES)
CAVITY
LENGTH
WIDTH
DEPTH
PITCH
BOTTOM HOLE DIAMETER
A0
B0
K0
P
D1
2.40 ± 0.10
2.40 ± 0.10
1.20 ± 0.10
4.00 ± 0.10
1.00 + 0.25
0.094 ± 0.004
0.094 ± 0.004
0.047 ± 0.004
0.157 ± 0.004
0.039 + 0.010
PERFORATION
DIAMETER
PITCH
POSITION
D
P0
E
1.55 ± 0.05
4.00 ± 0.10
1.75 ± 0.10
0.061 ± 0.002
0.157 ± 0.004
0.069 ± 0.004
CARRIER TAPE
WIDTH
THICKNESS
W
t1
8.00 ± 0.30
0.254 ± 0.02
0.315 ± 0.012
0.0100 ± 0.0008
COVER TAPE
WIDTH
TAPE THICKNESS
C
Tt
5.4 ± 0.10
0.062 ± 0.001
0.205 ± 0.004
0.0025 ± 0.00004
DISTANCE
CAVITY TO PERFORATION
(WIDTH DIRECTION)
F
3.50 ± 0.05
0.138 ± 0.002
CAVITY TO PERFORATION
(LENGTH DIRECTION)
P2
2.00 ± 0.05
0.079 ± 0.002
Tt (COVER TAPE THICKNESS)
Applications Information
P
Schottky Diode Fundamentals
The HBAT-540x series of clipping/clamping diodes
are Schottky devices. A Schottky device is a rectifying,
metal-semiconductor contact formed between a metal
and an n‑doped or a p-doped semiconductor. When a
metal-semiconductor junction is formed, free electrons
flow across the junction from the semiconductor and fill
the free-energy states in the metal. This flow of electrons
creates a depletion or potential across the junction. The
difference in energy levels between semiconductor and
metal is called a Schottky barrier.
P-doped, Schottky-barrier diodes excel at applications
requiring ultra low turn-on voltage (such as zero-biased
RF detectors). But their very low, breakdown-voltage
and high series-resistance make them unsuitable for
the clipping and clamping applications involving high
forward currents and high reverse voltages. Therefore,
this discussion will focus entirely on n‑doped Schottky
diodes.
Under a forward bias (metal connected to positive in an
n‑doped Schottky), or forward voltage, VF, there are many
electrons with enough thermal energy to cross the barrier
potential into the metal. Once the applied bias exceeds
the built-in potential of the junction, the forward current,
IF, will increase rapidly as VF increases.
When the Schottky diode is reverse biased, the potential
barrier for electrons becomes large; hence, there is
a small probability that an electron will have sufficient thermal energy to cross the junction. The reverse
leakage current will be in the nanoampere to microampere range, depending upon the diode type, the reverse
voltage, and the temperature.
In contrast to a conventional p-n junction, current in
the Schottky diode is carried only by majority carriers.
Because no minority carrier charge storage effects are
present, Schottky diodes have carrier lifetimes of less
than 100 ps and are extremely fast switching semiconductors. Schottky diodes are used as rectifiers at
­frequencies of 50 GHz and higher.
Another significant difference between Schottky and
p-n diodes is the forward voltage drop. Schottky diodes
have a threshold of typically 0.3 V in comparison to that
of 0.6 V in p-n junction diodes. See Figure 6.
N
METAL N
CAPACITANCE
CURRENT
CAPACITANCE
CURRENT
0.6 V
–
0.3 V
+
–
+
BIAS VOLTAGE
BIAS VOLTAGE
PN JUNCTION
SCHOTTKY JUNCTION
Figure 6.
Through the careful manipulation of the diameter of the
Schottky contact and the choice of metal deposited on
the n-doped silicon, the important characteristics of the
diode (junction capacitance, C J; parasitic series resistance, RS; breakdown voltage, VBR; and forward voltage,
VF,) can be optimized for specific applications. The HSMS270x series and HBAT‑540x series of diodes are a case in
point.
Both diodes have similar barrier heights; and this
is indicated by corresponding values of saturation
current, IS. Yet, different contact diameters and ­epitaxiallayer thickness result in very different values of junction
capacitance, C J and RS. This is portrayed by their SPICE
parameters in Table 1.
Table 1. HBAT-540x and HSMS‑270x SPICE Parameters.
Parameter
BV
HBAT-540x
HSMS-270x
40 V
25 V
CJ0
3.0 pF
6.7 pF
EG
0.55 eV
0.55 eV
IBV
10E-4 A
10E-4 A
IS
1.0E-7 A
1.4E-7 A
N
1.0
1.04
RS
2.4 Ω
0.65 Ω
PB
0.6 V
0.6 V
PT
2
2
M
0.5
0.5
At low values of IF ≤ 1 mA, the forward voltages of the
two diodes are nearly identical. However, as current rises
above 10 mA, the lower series resistance of the HSMS270x allows for a much lower forward voltage. This gives
the HSMS-270x a much higher current ­handling capability. The trade-off is a higher value of junction capacitance.
The forward voltage and current plots illustrate the differences in these two Schottky diodes, as shown in Figure
7.
300
HBAT-540x
10
1
.1
.01
11600 (V F – I F R S )
0
0.1
0.2
0.3
0.4
0.5
0.6
VF – FORWARD VOLTAGE (V)
Figure 7. Forward Current vs.
Forward
Voltage
Figure
7. Forward
Currentatvs.25°C.
Forward Voltage at 25°C.
Because the automatic, pick-and-place equipment used
to assemble these products selects dice from adjacent
sites on the wafer, the two diodes which go into the HBAT5402 or HBAT-540C (series pair) are closely matched —
without the added expense of testing and binning.
Current Handling in Clipping/Clamping Circuits
The purpose of a clipping/clamping diode is to handle
high currents, protecting delicate circuits downstream
of the diode. Current handling capacity is determined
by two sets of characteristics, those of the chip or device
itself and those of the package into which it is mounted.
noisy data-spikes
current
limiting
Vs
long cross-site cable
pull-down
(or pull-up)
0V
voltage limited to
Vs + Vd
0V – Vd
Figure 8. Two Schottky Diodes Are Used for Clipping/Clamping in a Circuit.
Consider the circuit shown in Figure 8, in which two
Schottky diodes are used to protect a circuit from noise
spikes on a stream of digital data. The ability of the diodes
to limit the voltage spikes is related to their ability to sink
the associated current spikes. The ­importance of current
­handling capacity is shown in Figure 9, where the forward
voltage generated by a forward current is compared in
two diodes. The first is a conventional Schottky diode of
the type generally used in RF circuits, with an RS of 7.7Ω.
The second is a Schottky diode of identical characteristics, save the R S of 1.0 Ω. For the conventional diode, the
relatively high value of RS causes the voltage across the
diode’s terminals to rise as current increases. The power
dissipated in the diode heats the junction, causing RS to
climb, giving rise to a runaway thermal condition. In the
second diode with low RS , such heating does not take
place and the voltage across the diode terminals is maintained at a low limit even at high values of current.
nT J
IF = IS e
–1
2
1
1
T J n –4060 T J – 298
IS = I0
e
298
(1)
(2)
(3)
TJ = V F I F θ JC + TA
where:
I F = forward current
IS = saturation current
VF = forward voltage
RS = series resistance
TJ = junction temperature
IO = saturation current at 25°C
n = diode ideality factor
θ JC = thermal resistance from junction to case
(diode lead)
= θpackage + θchip
T A = ambient (diode lead) ­temperature
Equation (1) describes the forward V-I curve of a Schottky
diode. Equation (2) provides the value for the diode’s saturation current, which value is plugged into (1). Equation
(3) gives the value of junction temperature as a function
of power dissipated in the diode and ambient (lead)
temperature.
6
VF – FORWARD VOLTAGE (V)
I F – FORWARD CURRENT (mA)
Maximum reliability is obtained in a Schottky diode
when the steady state junction temperature is maintained at or below 150°C, although brief excursions to
higher junction temperatures can be tolerated with no
significant impact upon mean-time-to-failure, MTTF. In
order to compute the junction temperature, Equations
(1) and (3) below must be simultaneously solved.
HSMS-270x
100
5
4
Rs = 7.7 Ω
3
2
Rs = 1.0 Ω
1
0
0
0.1
0.2
0.3
0.4
0.5
IF – FORWARD CURRENT (mA)
Figure 9. Comparison of Two Diodes.
Figure 9. Comparison of Two Diodes.
The key factors in these equations are: RS, the series resistance of the diode where heat is generated under high
current conditions; θ chip, the chip thermal resistance of
the Schottky die; and θ package, or the package thermal
­resistance.
RS for the HBAT-540x family of diodes is typically 2.4Ω,
other than the HSMS-270x family, this is the lowest of
any Schottky diode available. Chip thermal resistance is
typically 40°C/W; the thermal resistance of the iron-alloyleadframe, SOT-23 package is typically 460°C/W; and the
thermal resistance of the copper-leadframe, SOT-323
package is typically 110°C/W. The impact of package
thermal resistance on the current handling capability
of these diodes can be seen in Figures 3 and 4. Here the
computed values of junction temperature vs. forward
current are shown for three values of ambient temperature. The SOT-323 products, with their copper leadframes,
can safely handle almost twice the current of the larger
SOT-23 diodes. Note that the term “ambient temperature”
refers to the temperature of the diode’s leads, not the air
around the circuit board. It can be seen that the HBAT540B and HBAT‑540C products in the SOT‑323 package
will safely withstand a steady-state forward current of 330
mA when the diode’s terminals are maintained at 75°C.
Part Number Ordering Information
Part Number
No. of Devices
Container
HBAT-5400-BLKG
HBAT-5400-TR1G
HBAT-5400-TR2G
100
3,000
10,000
Antistatic Bag
7" Reel
13" Reel
HBAT-5402-BLKG
HBAT-5402-TR1G
HBAT-5402-TR2G
100
3,000
10,000
Antistatic Bag
7" Reel
13" Reel
HBAT-540B-BLKG
HBAT-540B-TR1G
HBAT-540B-TR2G
100
3,000
10,000
Antistatic Bag
7" Reel
13" Reel
HBAT-540C-BLKG
HBAT-540C-TR1G
100
3,000
Antistatic Bag
7" Reel
HBAT-540C-TR2G
10,000
13" Reel
For pulsed currents and transient current spikes of less
than one microsecond in duration, the junction does
not have time to reach thermal steady state. Moreover,
the diode junction may be taken to temperatures higher
than 150°C for short timeperiods without impacting
device MTTF. Because of these factors, higher currents
can be safely handled. The HBAT-540x family has the
second highest current handling capability of any Avago
diode, next to the HSMS-270x series.
For product information and a complete list of distributors, please go to our web site: www.avagotech.com
Avago, Avago Technologies, and the A logo are trademarks of Avago Technologies in the United States and other countries.
Data subject to change. Copyright © 2005-2008 Avago Technologies. All rights reserved. Obsoletes 5989-4779EN
AV02-1394EN - July 4, 2008
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