Fig. 1: Clamping voltage versus peak pulse current
(Tjinitial = 25°C) Rectangularwaveformtp = 2.5µs.
Ipp(A)
10.0
tp = 2.5µs
1.0
0.1
0 102030405060
Vcl(V)
Fig. 3: Relative variation of leakage current versus
junction temperature (typical values).
IR[Tj] / IR[Tj=25°C]
1000
100
Fig. 2: Capacitance versus reverse applied voltage
(typical values).
C(pF)
14
12
10
8
6
4
2
0
02468101214
VR(V)
F=1MHz
Vosc=30mV
Tj=25°C
RMS
10
Tj(°C)
1
255075100125
APPLICATION EXAMPLE
A1
Connector
A3
C1
B2
C3
IC
to be
protected
3/9
ESDA14V2-4BF1
TECHNICAL INFORMATION
1. ESD protection by ESDA14V2- 4BF1
With the focus of lowering the operation levels, the problem of malfunction caused by the environment is
critical. Electrostatic discharge (ESD) is a major cause of failure in electronic systems.
As a transient voltage suppressor, ESDA14V2-4BF1is an ideal choice for ESD protectionby suppressing
ESDevents. It iscapable of clampingthe incoming transient to a low enough level such that anydamage is
prevented on the device protected by ESDA14V2-4BF1.
ESDA14V2-4BF1serves as a parallel protection elements, connectedbetween the signal line andground.
As the transient rises above the operating voltage of the device, the ESDA14V2-4BF1 becomes a low
impedance path diverting the transient current to ground.
The clamping voltage is given by the following formula:
VVRI
=+.
CLBRd pp
As shown in figure A1, the ESD strikes are clamped by the transient voltage suppressor.
Fig. A1: ESD clamping behavior
Rg
Ip
Rd
Vg
V
V(i/o)
BR
R load
Device
to be
ESD Surge
ESDA14V2-4BF1
Tohave a good approximationof the remaining voltagesat both Vi/o side,we provide the typicaldynamical
resistance value Rd. By taking into account the following hypothesis :
This confirms the very low remaining voltage across the device to be protected. It is also important to note
that in this approximation the parasitic inductance effect was not taken into account. This could be a few
tenths of volts during a few ns at the Vi/o side.
4/9
V(i/o)
ESDA14V2-4BF1
Fig. A2: ESD test board
TEST BOARD
V(i/o)
®
EB14
15
Fig. A3: ESD test configuration
A1, C1, A3 or C3
± 15kV
ESD Air discharge
B2
V(i/o)
The measurements done here after show very clearly (Fig. A4) the high efficiency of the ESD protection:
theclamping voltage V(i/o) becomes veryclose to +V
(positiveway, Fig. A4a) and -VBR(negativeway,
BR
Fig. A4b).
Fig. A4: Remaining voltage during ESD surge
V(i/o)
a: Response in the positive way
V(i/o)
b: Response in the negative way
5/9
ESDA14V2-4BF1
CROSSTALK BEHAVIOR
Fig. A5: Crosstalk phenomenon
R
G1
Line 1
V
G1
R
G2
R
L1
αβ1G112G2V+ V
Line 2
V
G2
DRIVERS
R
L2
RECEIVERS
αβ
2G221G1V+ V
Thecrosstalk phenomena aredue to the coupling between2 lines. Couplingfactors ( β12or β21 ) increase
when the gap across lines decreases, particularly in silicon dice. In the example above, the expected
signal on load R
the V
signal represents the effect of the crosstalk phenomenon of the line 1 on the line 2. This
G1
is α2VG2, in fact the real voltage at this point has got an extra value β21VG2. This part of
L2
phenomenon has to be taken into account when the drivers impose fast digital data or high frequency
analog signals. The perturbed line will be more affected if it works with low voltage signal or high load
Fig. A6: Analog crosstalk measurements
Connected to the port1
of the Network Analyser
6/9
TEST BOARD
A1
EB14
15
C3
Connected to the port2
of the Network Analyser
ESDA14V2-4BF1
Fig. A7: Typical analog crosstalk measurements
Typical crosstalk response of ESDA14V2-4BF1 (A1/A3 line)
0.00
-10.00
-20.00
-30.00
-40.00
-50.00
-60.00
-70.00
-80.00
-90.00
-100.0
100.0k1.0M10.0M100.0M1.0G
FigureA6 gives the measurement circuit for theanalog crosstalk application. In figureA7, the curve shows
theeffect of theline A1 on theline A3. Inusual frequency rangeof analog signals (upto 100MHz) theeffect
on disturbed line is less than -30dB.
f/Hz
Fig. A8: Digital crosstalk measurements configu-
Fig. A9: Digital crosstalk results
ration.
0 - 3V
Pulse generator
f = 5MHz
risetime = 3ns
A1
G1
V
C3
unloaded
B2 = GND
β
21 G1V
unloaded
VG1
β21 G1V
rise time: t= 3ns
crosstalk
10-90%
Figure A8 shows the measurement circuit used to quantify the crosstalk effect in a classical digital
application.
Figure A9 shows that in sucha condition, the impact on the disturbed line is less than 50 mV peak to peak.
No data disturbance was noted on the concerned line. The measurements performed with falling edges
give an impact within the same range.
Note: More packing informations are available in the application note AN1235: "Flip-Chip: Package description and recommandations for use"
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