ATF-54143-TR1G Avago Technologies US Inc., ATF-54143-TR1G Datasheet - Page 10
![IC TRANS E-PHEMT 2GHZ SOT-343](/photos/5/63/56357/516-sot-343_sml.jpg)
ATF-54143-TR1G
Manufacturer Part Number
ATF-54143-TR1G
Description
IC TRANS E-PHEMT 2GHZ SOT-343
Manufacturer
Avago Technologies US Inc.
Datasheet
1.ATF-54143-TR1G.pdf
(17 pages)
Specifications of ATF-54143-TR1G
Package / Case
SC-70-4, SC-82-4, SOT-323-4, SOT-343
Transistor Type
pHEMT FET
Frequency
2GHz
Gain
16.6dB
Voltage - Rated
5V
Current Rating
120mA
Noise Figure
0.5dB
Current - Test
60mA
Voltage - Test
3V
Power - Output
20.4dBm
Configuration
Single Dual Source
Transistor Polarity
N-Channel
Power Dissipation
725 mW
Drain Source Voltage Vds
5 V
Gate-source Breakdown Voltage
- 5 V to 1 V
Continuous Drain Current
120 mA
Maximum Operating Temperature
+ 150 C
Maximum Drain Gate Voltage
- 5 V to 1 V
Minimum Operating Temperature
- 65 C
Mounting Style
SMD/SMT
Continuous Drain Current Id
120mA
Power Dissipation Pd
725mW
Noise Figure Typ
0.5dB
Rf Transistor Case
SOT-343
No. Of Pins
4
Termination Type
SMD
Rohs Compliant
Yes
Filter Terminals
SMD
Drain Current Idss Max
5µA
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Lead Free Status / RoHS Status
Lead free / RoHS Compliant, Lead free / RoHS Compliant
Other names
516-1572-2
Available stocks
Company
Part Number
Manufacturer
Quantity
Price
Company:
Part Number:
ATF-54143-TR1G
Manufacturer:
AVAGO
Quantity:
15 600
Company:
Part Number:
ATF-54143-TR1G
Manufacturer:
AVAGO
Quantity:
30 000
Part Number:
ATF-54143-TR1G
Manufacturer:
AVAGO/安华高
Quantity:
20 000
ATF-54143 Applications
Information
Introduction
Agilent Technologies’s ATF-54143
is a low noise enhancement mode
PHEMT designed for use in low
cost commercial applications in
the VHF through 6 GHz frequency
range. As opposed to a typical
depletion mode PHEMT where the
gate must be made negative with
respect to the source for proper
operation, an enhancement mode
PHEMT requires that the gate be
made more positive than the
source for normal operation.
Therefore a negative power
supply voltage is not required for
an enhancement mode device.
Biasing an enhancement mode
PHEMT is much like biasing the
typical bipolar junction transistor.
Instead of a 0.7 V base to emitter
voltage, the ATF-54143 enhance-
ment mode PHEMT requires
about a 0.6V potential between
the gate and source for a nominal
drain current of 60 mA.
Matching Networks
The techniques for impedance
matching an enhancement mode
device are very similar to those
for matching a depletion mode
device. The only difference is in
the method of supplying gate
bias. S and Noise Parameters for
various bias conditions are listed
in this data sheet. The circuit
shown in Figure 1 shows a typical
LNA circuit normally used for
900 and 1900 MHz applications
(Consult the Agilent Technologies
website for application notes
covering specific applications).
High pass impedance matching
networks consisting of L1/C1 and
L4/C4 provide the appropriate
match for noise figure, gain, S11
and S22. The high pass structure
also provides low frequency gain
reduction which can be beneficial
from the standpoint of improving
out-of-band rejection at lower
frequencies.
10
Figure 1. Typical ATF-54143 LNA with Passive
Biasing.
Capacitors C2 and C5 provide a
low impedance in-band RF
bypass for the matching net-
works. Resistors R3 and R4
provide a very important low
frequency termination for the
device. The resistive termination
improves low frequency stability.
Capacitors C3 and C6 provide
the low frequency RF bypass for
resistors R3 and R4. Their value
should be chosen carefully as C3
and C6 also provide a termina-
tion for low frequency mixing
products. These mixing products
are as a result of two or more in-
band signals mixing and produc-
ing third order in-band distortion
products. The low frequency or
difference mixing products are
bypassed by C3 and C6. For best
suppression of third order
distortion products based on the
CDMA 1.25 MHz signal spacing,
C3 and C6 should be 0.1 µF in
value. Smaller values of capaci-
tance will not suppress the
generation of the 1.25 MHz
difference signal and as a result
will show up as poorer two tone
IP3 results.
Bias Networks
One of the major advantages of
the enhancement mode technol-
ogy is that it allows the designer
to be able to dc ground the
source leads and then merely
apply a positive voltage on the
gate to set the desired amount of
quiescent drain current I
INPUT
Zo
R7
R5
R6
C1
L1
R1
C3
C2
Q1
L2
C7
Q2
L3
R2
L4
C5
R4
C6
C4
d
.
R3
Zo
OUTPUT
Vdd
Whereas a depletion mode
PHEMT pulls maximum drain
current when V
hancement mode PHEMT pulls
only a small amount of leakage
current when V
V
device threshold voltage, will
drain current start to flow. At a
V
0.6V, the drain current I
approximately 60 mA. The data
sheet suggests a minimum and
maximum V
desired amount of drain current
will be achieved. It is also impor-
tant to note that if the gate
terminal is left open circuited,
the device will pull some amount
of drain current due to leakage
current creating a voltage differ-
ential between the gate and
source terminals.
Passive Biasing
Passive biasing of the ATF-54143
is accomplished by the use of a
voltage divider consisting of R1
and R2. The voltage for the
divider is derived from the drain
voltage which provides a form of
voltage feedback through the use
of R3 to help keep drain current
constant. Resistor R5 (approxi-
mately 10kΩ) provides current
limiting for the gate of enhance-
ment mode devices such as the
ATF-54143. This is especially
important when the device is
driven to P
Resistor R3 is calculated based
on desired V
power supply voltage.
R3 =
V
V
voltage.
I
I
the R1/R2 resistor voltage
divider network.
ds
BB
gs
ds
DD
ds
is the desired drain current.
is the current flowing through
is increased above V
of 3V and a nominal V
is the device drain to source
is the power supply voltage.
V
I
DD
ds
+ I
– V
1dB
BB
gs
ds
ds
, I
or P
over which the
p
gs
gs
ds
= 0V, an en-
= 0V. Only when
(1)
SAT
and available
.
to
d
, the
gs
will be
of