10
Figure 23. Typical ATF-54143 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 termina-
tion 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
ATF-54143 Applications Information
Introduction
Avago Technologies’ 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 0.7V base
to emitter voltage, the ATF-54143 enhancement 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 en-
hancement 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 23 shows a
typical LNA circuit normally used for 900 and 1900 MHz
applications (Consult the Avago Technologies website
for application notes covering speci c applications).
High pass impedance 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 frequency gain reduction which can
be bene cial from the standpoint of improving out-of-
band rejection at lower frequencies.
also provide 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
di erence 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 capacitance
will not suppress the generation of the 1.25 MHz di er-
ence 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
to
,
the device threshold voltage, will drain current start to
ow. At a V
ds
of 3V and a nominal V
gs
of 0.6V, the drain
current I
d
will be approximately 60 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-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 (approximately 10k) provides current limiting for
the gate of enhancement mode devices such as the
ATF-54143. 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.
V
dd
Z
o
L2 L3
C2
C3
L1
J1
R4
R5
C5
C6
L4
R3
R1 R2
C1
Z
o
C4
Q1
OUTPUT
INPUT
J2
11
I
BB
is the current  owing through the R1/R2 resistor
voltage divider network.
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)
V
gs
Example Circuit
V
DD
= 5V
V
ds
= 3V
I
ds
= 60 mA
V
gs
= 0.59V
Choose I
BB
to be at least 10X the normal expected gate
leakage current. I
BB
was chosen to be 2 mA for this
example. Using equations (1), (2), and (3) the resistors
are calculated as follows
R1 = 295
R2 = 1205
R3 = 32.3
Active Biasing
Active biasing provides a means of keeping the
quiescent bias point constant over temperature and
constant over lot to lot variations in device dc per-
formance. 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 transistor.
An active bias scheme is shown in Figure 24. 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 constant 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 equations 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
formula:
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
= 5V
V
ds
= 3V
I
ds
= 60 mA
R4 = 10
V
BE
= 0.7V
Equation (1) calculates the required voltage at the
emitter of the PNP transistor based on desired V
ds
and
I
ds
through resistor R4 to be 3.6V. Equation (2) calcu-
lates the value of resistor R3 which determines the
drain current I
ds
. In the example R3=23.3. 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=1450 and R2=1050. R7 is chosen to
be 1k. This resistor keeps a small amount of current
owing through Q2 to help maintain bias stability. R6 is
chosen to be 10k. This value of resistance is necessary
to limit Q1 gate current in the presence of high RF drive
level (especially when Q1 is driven to P
1dB
gain com-
pression point).
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 24. Typical ATF-54143 LNA with Active Biasing.
12
GATE
SOURCE
INSIDE Package
Port
G
Num=1
C
C1
C=0.13 pF
Port
S1
Num=2
SOURCE
DRAIN
Port
S2
Num=4
Port
D
Num=3
L
L6
L=0.175 nH
R=0.001
C
C2
C=0.159 pF
L
L7
L=0.746 nH
R=0.001
MSub
TLINP
TL4
Z=Z1 Ohm
L=15 mil
K=1
A=0.000
F=1 GHz
TanD=0.001
TLINP
TL10
Z=Z1 Ohm
L=15 mil
K=1
A=0.000
F=1 GHz
TanD=0.001
TLINP
TL3
Z=Z2 Ohm
L=25 mil
K=K
A=0.000
F=1 GHz
TanD=0.001
TLINP
TL9
Z=Z2 Ohm
L=10.0 mil
K=K
A=0.000
F=1 GHz
TanD=0.001
VAR
VAR1
K=5
Z2=85
Z1=30
Var
Egn
TLINP
TL1
Z=Z2/2 Ohm
L=20 0 mil
K=K
A=0.0000
F=1 GHz
TanD=0.001
TLINP
TL2
Z=Z2/2 Ohm
L=20 0 mil
K=K
A=0.0000
F=1 GHz
TanD=0.001
TLINP
TL8
Z=Z1 Ohm
L=15.0 mil
K=1
A=0.0000
F=1 GHz
TanD=0.001
TLINP
TL7
Z=Z2/2 Ohm
L=5.0 mil
K=K
A=0.0000
F=1 GHz
TanD=0.001
TLINP
TL5
Z=Z2 Ohm
L=26.0 mil
K=K
A=0.0000
F=1 GHz
TanD=0.001
TLINP
TL6
Z=Z1 Ohm
L=15.0 mil
K=1
A=0.0000
F=1 GHz
TanD=0.001
L
L1
L=0.477 nH
R=0.001
L
L4
L=0.4 nH
R=0.001
GaAsFET
FET1
Mode1=MESFETM1
Mode=Nonlinear
MSUB
MSub1
H=25.0 mil
Er=9.6
Mur=1
Cond=1.0E+50
Hu=3.9e+034 mil
T=0.15 mil
TanD=0
Rough=0 mil
NFET=yes
PFET=no
Vto=0.3
Beta=0.9
Lambda=82e-3
Alpha=13
Tau=
Tnom=16.85
Idstc=
Ucrit=-0.72
Vgexp=1.91
Gamds=1e-4
Vtotc=
Betatce=
Rgs=0.25 Ohm
Rf=
Gscap=2
Cgs=1.73 pF
Cgd=0.255 pF
Gdcap=2
Fc=0.65
Rgd=0.25 Ohm
Rd=1.0125 Ohm
Rg=1.0 Ohm
Rs=0.3375 Ohm
Ld=
Lg=0.18 nH
Ls=
Cds=0.27 pF
Rc=250 Ohm
Crf=0.1 F
Gsfwd=
Gsrev=
Gdfwd=
Gdrev=
R1=
R2=
Vbi=0.8
Vbr=
Vjr=
Is=
Ir=
Imax=
Xti=
Eg=
N=
Fnc=1 MHz
R=0.08
P=0.2
C=0.1
Taumdl=no
wVgfwd=
wBvgs=
wBvgd=
wBvds=
wldsmax=
wPmax=
AllParams=
Advanced_Curtice2_Model
MESFETM1
ATF-54143 Die Model
ATF-54143 curtice ADS Model

ATF-54143-BLKG

Mfr. #:
Manufacturer:
Broadcom / Avago
Description:
RF JFET Transistors Transistor GaAs Single Voltage
Lifecycle:
New from this manufacturer.
Delivery:
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