13
ATF-55143 Typical Scattering Parameters, V
DS
= 3V, I
DS
= 30 mA
Freq. S
11
S
21
S
12
S
22
MSG/MAG
GHz Mag. Ang. dB Mag. Ang. Mag. Ang. Mag. Ang. dB
0.1 0.996 -7.9 24.3 16.407 173.9 0.005 85.6 0.729 -4.5 35.16
0.5 0.937 -38.1 23.64 15.205 150.4 0.021 68.8 0.683 -21.2 28.60
0.9 0.840 -64.1 22.44 13.246 130.9 0.034 56.1 0.620 -34.3 25.91
1.0 0.819 -70.1 22.11 12.753 126.6 0.036 53.5 0.601 -36.8 25.49
1.5 0.712 -95.7 20.43 10.507 108.4 0.046 43.4 0.531 -46.5 23.59
1.9 0.646 -112.8 19.2 9.117 96.4 0.051 37.7 0.488 -51.8 22.52
2.0 0.631 -116.8 18.91 8.823 93.7 0.052 36.6 0.479 -52.9 22.30
2.5 0.571 -135.8 17.59 7.578 80.9 0.057 31.3 0.437 -57.7 21.24
3.0 0.531 -153.9 16.42 6.625 69.4 0.062 26.6 0.398 -61.8 20.29
4.0 0.499 171.8 14.49 5.303 48.1 0.071 18.1 0.328 -71.6 18.73
5.0 0.512 140.9 12.84 4.386 28.1 0.078 9.2 0.273 -84.7 16.32
6.0 0.529 116 11.35 3.693 9.4 0.085 0.7 0.242 -98.5 14.36
7.0 0.552 94.7 10.07 3.188 -8.3 0.092 -9 0.214 -112.9 12.98
8.0 0.573 73.9 8.91 2.79 -25.6 0.096 -18.6 0.179 -120.5 11.65
9.0 0.609 55.1 7.94 2.496 -42.7 0.107 -25.8 0.134 -128.4 10.92
10.0 0.684 37.3 7.05 2.251 -61.3 0.118 -39.2 0.064 -173.3 10.93
11.0 0.744 21.6 5.91 1.975 -79.5 0.123 -51.9 0.075 87.5 10.53
12.0 0.786 7.9 4.83 1.744 -96.4 0.128 -64.3 0.141 49.7 10.16
13.0 0.816 -7.2 3.86 1.56 -113.9 0.131 -77.5 0.187 26.4 9.84
14.0 0.842 -22.8 2.93 1.401 -132.6 0.133 -91.7 0.250 5.1 9.51
15.0 0.870 -37.1 1.56 1.197 -151.1 0.128 -106 0.367 -12.6 8.39
16.0 0.866 -50.3 -0.01 0.998 -168.2 0.122 -119.1 0.467 -24.8 6.39
17.0 0.882 -59.7 -1.4 0.851 177 0.12 -130.8 0.543 -38.2 5.77
18.0 0.927 -69.9 -2.55 0.746 161.2 0.115 -144.8 0.602 -52.8 8.12
Freq F
min
Γ
opt
Γ
opt
R
n/50
G
a
GHz dB Mag. Ang.
dB
0.5 0.19 0.59 18.4 0.09 26.27
0.9 0.25 0.5 25.5 0.09 24.41
1.0 0.26 0.52 30.7 0.09 23.98
1.9 0.41 0.44 50.6 0.08 20.51
2.0 0.42 0.43 54.5 0.08 20.18
2.4 0.49 0.34 65.1 0.08 18.92
3.0 0.59 0.27 84.7 0.07 17.28
3.9 0.72 0.17 132.6 0.06 15.33
5.0 0.88 0.19 -156.2 0.06 13.61
5.8 1.02 0.24 -125.3 0.09 12.71
6.0 1.06 0.25 -118.8 0.1 12.52
7.0 1.2 0.32 -88.8 0.17 11.73
8.0 1.37 0.39 -62.7 0.28 11.08
9.0 1.53 0.47 -43.1 0.43 10.41
10.0 1.66 0.57 -27 0.65 9.58
Notes:
1. F
min
values at 2 GHz and higher are based on measurements while the F
mins
below 2 GHz have been extrapolated. The F
min
values are based on
a set of 16 noise  gure measurements made at 16 di erent impedances using an ATN NP5 test system. From these measurements a true F
min
is
calculated. Refer to the noise parameter application section for more information.
2. S and noise parameters are measured on a microstrip line made on 0.025 inch thick alumina carrier. The input reference plane is at the end of
the gate lead. The output reference plane is at the end of the drain lead. The parameters include the e ect of four plated through via holes con-
necting source landing pads on top of the test carrier to the microstrip ground plane on the bottom side of the carrier. Two 0.020 inch diameter
via holes are placed within 0.010 inch from each source lead contact point, one via on each side of that point.
Typical Noise Parameters, V
DS
= 3V, I
DS
= 30 mA
14
ATF-55143 Applications Information
Introduction
Avago Technologies’ ATF-55143 is a low noise
enhancement mode PHEMT designed for use in low cost
commercial applications in the VHF through 6 GHz fre-
quency 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 enhance-
ment 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 volt-
age, the ATF-55143 enhancement mode PHEMT requires
about a 0.47V potential between the gate and source for
a nominal drain current of 10 mA.
Matching Networks
The techniques for impedance matching an enhance-
ment mode device are very similar to those for matching
a depletion mode device. The only di erence 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 33 shows a typical LNA cir-
cuit normally used for 900 and 1900 MHz applications
(Consult the Avago Technologies website for application
notes covering speci c applications). High pass imped-
ance matching networks consisting of L1/C1 and L4/C4
provide the appropriate match for noise  gure, gain, S11
and S22. The high pass structure also provides low fre-
quency gain reduction which can be bene cial from the
standpoint of improving out-of-band rejection.
INPUT
C1
C2
C3
L1
R4
R1 R2
Vdd
R3
L2 L3
L4
Q1
Zo
Zo
C4
C5
C6
OUTPUT
R5
Figure 33. Typical ATF-55143 LNA with Passive Biasing.
Capacitors C2 and C5 provide a low impedance in-band
RF bypass for the matching networks. 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 pro-
vide a termination for low frequency mixing products.
These mixing products are as a result of two or more in-
band signals mixing and producing third order in-band
distortion products. The low frequency or difference
mixing products are terminated 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 capacitance will
not suppress the generation of the 1.25 MHz di erence
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 technology 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
d
.
Whereas a depletion mode PHEMT pulls maximum
drain current when V
gs
= 0V, an enhancement mode
PHEMT pulls only a small amount of leakage current
when V
gs
= 0V. Only when V
gs
is increased above V
th
, the
device threshold voltage, will drain current start to  ow.
At a V
ds
of 2.7V and a nominal V
gs
of 0.47V, the drain
current I
d
will be approximately 10 mA. The data sheet
suggests a minimum and maximum V
gs
over which the
desired amount of drain current will be achieved. It is
also important 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
di erential between the gate and source terminals.
Passive Biasing
Passive biasing of the ATF-55143 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. Resis-
tor R5 (approximately 10kΩ) is added to limit the gate
current of enhancement mode devices such as the
ATF-55143. This is especially important when the device
is driven to P
1dB
or P
SAT
.
Resistor R3 is calculated based on desired V
ds
, I
ds
and
available power supply voltage.
R3 =
V
DD
V
ds
(1)
p
I
ds
+ I
BB
V
DD
is the power supply voltage.
V
ds
is the device drain to source voltage.
I
ds
is the desired drain current.
I
BB
is the current  owing through the R1/R2 resistor volt-
age divider network.
15
The values of resistors R1 and R2 are calculated with the
following formulas
R1 =
V
gs
(2)
p
I
BB
R2 =
(V
ds
V
gs
) R1
(3)
p
V
gs
Example Circuit
V
DD
= 3V
V
ds
= 2.7V
I
ds
= 10 mA
V
gs
= 0.47 V
Choose I
BB
to be at least 10X the normal expected gate
leakage current. I
BB
was conservatively chosen to be
0.5 mA for this example. Using equations (1), (2), and (3)
the resistors are calculated as follows
R1 = 940Ω
R2 = 4460Ω
R3 = 28.6Ω
Active Biasing
Active biasing provides a means of keeping the quies-
cent bias point constant over temperature and constant
over lot to lot variations in device dc performance. The
advantage of the active biasing of an enhancement
mode PHEMT versus a depletion mode PHEMT is that a
negative power source is not required. The techniques
of active biasing an enhancement mode device are very
similar to those used to bias a bipolar junction transis-
tor.
INPUT
C1
C2
C3
C7
L1
R5
R6
R7 R3
R2
R1
Q2
Vdd
R4
L2 L3
L4
Q1
Zo
Zo
C4
C5
C6
OUTPUT
Figure 34. Typical ATF-55143 LNA with Active Biasing.
An active bias scheme is shown in Figure 34. R1 and R2
provide a constant voltage source at the base of a PNP
transistor at Q2. The constant voltage at the base of Q2
is raised by 0.7 volts at the emitter. The constant emitter
voltage plus the regulated V
DD
supply are present across
resistor R3. Constant voltage across R3 provides a con-
stant current supply for the drain current. Resistors R1
and R2 are used to set the desired Vds. The combined
series value of these resistors also sets the amount of
extra current consumed by the bias network. The equa-
tions that describe the circuit’s operation are as follows.
V
E
= V
ds
+ (I
ds
R4) (1)
R3 =
V
DD
V
E
(2)
p
I
ds
V
B
= V
E
V
BE
(3)
V
B
=
R1
V
DD
(4)
p
R1 + R2
V
DD
= I
BB
(R1 + R2) (5)
Rearranging equation (4) provides the following for-
mula
R2 =
R
1
(V
DD
V
B
)
(4A)
V
B
and rearranging equation (5) provides the following
formula
R1 =
V
DD
(5A)
9
I
BB
(1 +
V
DD
V
B
)
p
V
B
Example Circuit
V
DD
= 3V I
BB
= 0.5 mA
V
ds
= 2.7V
I
ds
= 10 mA
R4 = 10Ω
V
BE
= 0.7V
Equation (1) calculates the required voltage at the emit-
ter of the PNP transistor based on desired V
ds
and I
ds
through resistor R4 to be 2.8V. Equation (2) calculates
the value of resistor R3 which determines the drain cur-
rent I
ds
. In the example R3 = 20Ω. Equation (3) calculates
the voltage required at the junction of resistors R1 and
R2. This voltage plus the step-up of the base emitter
junction determines the regulated V
ds
. Equations (4) and
(5) are solved simultaneously to determine the value
of resistors R1 and R2. In the example R1=4200Ω and
R2=1800Ω. R7 is chosen to be 1kΩ. This resistor keeps
a small amount of current  owing through Q2 to help
maintain bias stability. R6 is chosen to be 10kΩ. This
value of resistance is necessary to limit Q1 gate current
in the presence of high RF drive levels (especially when
Q1 is driven to the P
1dB
gain compression point). C7
provides a low frequency bypass to keep noise from Q2
e ecting the operation of Q1. C7 is typically 0.1 μF.

ATF-55143-TR2G

Mfr. #:
Manufacturer:
Broadcom / Avago
Description:
RF JFET Transistors Transistor GaAs Single Voltage
Lifecycle:
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