Infineon BFP620F Low noise sige:c bipolar rf transistor Datasheet

BFP620F
Low Noise SiGe:C Bipolar RF Transistor
• High gain low noise RF transistor
3
• Based on Infineon's reliable high volume
2
4
1
Silicon Germanium technology
• Outstanding noise figure NFmin = 0.7 dB at 1.8 GHz
Outstanding noise figure NF min = 1.3 dB at 6 GHz
• Maximum stable gain
Gms = 21 dB at 1.8 GHz
Top View
4
Gma = 10 dB at 6 GHz
3
XYs
• Pb-free (RoHS compliant) and halogen-free thin small
1
flat package (1.4 x 0.8 x 0.59 mm) with visible leads
2
Direction of Unreeling
• Qualification report according to AEC-Q101 available
ESD (Electrostatic discharge) sensitive device, observe handling precaution!
Type
BFP620F
Marking
R2s
1=B
Pin Configuration
2=E
3=C
4=E
-
Package
-
TSFP-4
Maximum Ratings at TA = 25 °C, unless otherwise specified
Parameter
Symbol
Collector-emitter voltage
VCEO
Value
Unit
V
TA = 25 °C
2.3
TA = -55 °C
2.1
Collector-emitter voltage
VCES
7.5
Collector-base voltage
VCBO
7.5
Emitter-base voltage
VEBO
1.2
Collector current
IC
80
Base current
IB
3
Total power dissipation1)
Ptot
185
mW
Junction temperature
TJ
150
°C
Storage temperature
TStg
mA
TS ≤ 96°C
1T
S is
-55 ... 150
measured on the emitter lead at the soldering point to the pcb
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BFP620F
Thermal Resistance
Parameter
Symbol
Junction - soldering point1)
RthJS
Value
Unit
290
K/W
Values
Unit
Electrical Characteristics at T A = 25 °C, unless otherwise specified
Parameter
Symbol
min.
typ.
max.
2.3
2.8
-
V
ICES
-
-
10
µA
ICBO
-
-
100
nA
IEBO
-
-
3
µA
hFE
110
180
270
DC Characteristics
Collector-emitter breakdown voltage
V(BR)CEO
IC = 1 mA, I B = 0
Collector-emitter cutoff current
VCE = 7.5 V, VBE = 0
Collector-base cutoff current
VCB = 5 V, IE = 0
Emitter-base cutoff current
VEB = 0.5 V, IC = 0
DC current gain
-
IC = 50 mA, VCE = 1.5 V, pulse measured
1For
the definition of RthJS please refer to Application Note AN077 (Thermal Resistance Calculation)
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BFP620F
Electrical Characteristics at TA = 25 °C, unless otherwise specified
Parameter
Symbol
Values
Unit
min.
typ.
max.
fT
-
65
-
Ccb
-
0.12
0.2
Cce
-
0.2
-
Ceb
-
0.45
-
AC Characteristics (verified by random sampling)
Transition frequency
GHz
IC = 50 mA, VCE = 1.5 V, f = 1 GHz
Collector-base capacitance
pF
VCB = 2 V, f = 1 MHz, VBE = 0 ,
emitter grounded
Collector emitter capacitance
VCE = 2 V, f = 1 MHz, VBE = 0 ,
base grounded
Emitter-base capacitance
VEB = 0.5 V, f = 1 MHz, VCB = 0 ,
collector grounded
Minimum noise figure
dB
NFmin
IC = 5 mA, VCE = 1.5 V, f = 1.8 GHz, ZS = ZSopt
-
0.7
-
IC = 5 mA, VCE = 1.5 V, f = 6 GHz, ZS = ZSopt
-
1.3
-
Gms
-
21
-
dB
Gma
-
10
-
dB
Power gain, maximum stable1)
IC = 50 mA, VCE = 1.5 V, ZS = ZSopt,
ZL = ZLopt , f = 1.8 GHz
Power gain, maximum available1)
IC = 50 mA, VCE = 1.5 V, ZS = ZSopt,
ZL = ZLopt, f = 6 GHz
|S21e|2
Transducer gain
dB
IC = 50 mA, VCE = 1.5 V, ZS = ZL = 50 Ω,
f = 1.8 GHz
-
19.5
-
f = 6 GHz
-
9.5
-
IP3
-
25
-
P-1dB
-
14
-
Third order intercept point at output2)
dBm
VCE = 2 V, IC = 50 mA, ZS =ZL =50 Ω, f = 1.8 GHz
1dB compression point at output
IC = 50 mA, VCE = 2 V, ZS =ZL =50 Ω, f = 1.8 GHz
1G
1/2
ma = |S21e / S12e| (k-(k²-1) ), Gms
2IP3 value depends on termination of
= |S21e / S12e|
all intermodulation frequency components.
Termination used for this measurement is 50Ω from 0.1 MHz to 6 GHz
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BFP620F
Total power dissipation P tot = ƒ(TS)
Permissible Pulse Load RthJS = ƒ(tp)
10 3
200
mW
160
K/W
RthJS
Ptot
140
120
0.5
0.2
0.1
0.05
0.02
0.01
0.005
D=0
10 2
100
80
60
40
20
0
0
15
30
45
60
75
90 105 120 °C
10 1 -7
10
150
10
-6
10
-5
10
-4
10
-3
10
-2
TS
s
10
tp
Permissible Pulse Load
Collector-base capacitance Ccb = ƒ(VCB )
Ptotmax/PtotDC = ƒ(tp )
f = 1MHz
10 1
0.4
P totmax/ PtotDC
pF
CCB
0.3
D=0
0.005
0.01
0.02
0.05
0.1
0.2
0.5
0.25
0.2
0.15
0.1
0.05
10 0 -7
10
10
-6
10
-5
10
-4
10
-3
10
-2
s
10
0
0
0
tp
1
2
3
4
5
6
V
8
VCB
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0
BFP620F
Third order Intercept Point IP3=ƒ(IC)
Transition frequency fT= ƒ(IC)
(Output, ZS=ZL=50Ω)
f = 1GHz
VCE = parameter, f =1.8GHz
VCE = Parameter in V
30
70
GHz
2.3V
dBm
60
1.7V
1 to 2.3
55
20
50
fT
IP3
1.4V
15
45
0.8
40
0.8V
10
35
1.1V
30
25
5
20
15
0
10
0.3
0.5
5
-5
0
10
20
30
40
50
60
70 mA
0
0
90
10
20
30
40
50
60
70
80 mA
IC
100
IC
Power gain Gma, Gms = ƒ(IC )
Power Gain Gma, Gms = ƒ(f),
VCE = 1.5V
|S21|² = f (f)
f = Parameter in GHz
VCE = 1.5V, IC = 50mA
50
30
dB
dB
0.9
26
40
24
35
1.8
G
G
22
20
30
18
2.4
16
3
14
4
12
5
10
6
25
20
|S21|²
Gma
15
10
8
6
0
Gms
10
20
30
40
50
60
70 mA
5
0
90
IC
1
2
3
4
GHz
6
f
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BFP620F
Power gain Gma, Gms = ƒ (VCE )
Noise figure F = ƒ(IC )
IC = 50mA
VCE = 1.5V, ZS = ZSopt
f = Parameter in GHz
30
dB
3
0.9
24
2.5
1.8
G
20
2.4
2
3
16
4
F [dB]
5
12
1.5
6
8
1
4
f = 6GHz
f = 5GHz
f = 4GHz
f = 3GHz
f = 2.4GHz
f = 1.8GHz
f = 0.9GHz
0.5
0
-4
0.2
0.6
1
1.4
V
1.8
2.6
0
0
VCE
Noise figure F = ƒ(IC )
VCE = 1.5V, f = 1.8 GHz
10
20
30
40
50
60
70
80
I [mA]
c
Noise figure F = ƒ(f)
VCE = 1.5V, ZS = ZSopt
3
2.5
2.5
2
2
IC = 50mA
F [dB]
F [dB]
1.5
1.5
IC = 5.0mA
1
1
Z = 50Ω
S
Z =Z
S
Sopt
0.5
0.5
0
0
0
10
20
30
40
50
60
70
80
1
Ic [mA]
2
3
4
5
6
7
f [GHz]
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BFP620F
Source impedance for min.
noise figure vs. frequency
VCE = 1.5V, IC = 5.0mA/50.0mA
1
1.5
2
0.5
0.4
3
0.3
4
0.2
2.4GHz
5
1.8GHz
3GHz
10
0.1
0.1
0
0.2 0.3 0.4 0.5
1
1.5
4GHz
−0.1
2
3
4 5
5GHz
−10
6GHz
−0.2
Ic = 5.0mA
−0.3
−5
−4
−3
I = 50mA
−0.4
c
−2
−0.5
−1.5
−1
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Package TSFP-4
8
BFP620F
2013-09-09
BFP620F
Edition 2009-11-16
Published by
Infineon Technologies AG
81726 Munich, Germany
 2009 Infineon Technologies AG
All Rights Reserved.
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of conditions or characteristics. With respect to any examples or hints given herein,
any typical values stated herein and/or any information regarding the application of
the device, Infineon Technologies hereby disclaims any and all warranties and
liabilities of any kind, including without limitation, warranties of non-infringement of
intellectual property rights of any third party.
Information
For further information on technology, delivery terms and conditions and prices,
please contact the nearest Infineon Technologies Office (<www.infineon.com>).
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Due to technical requirements, components may contain dangerous substances.
For information on the types in question, please contact the nearest Infineon
Technologies Office.
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components can reasonably be expected to cause the failure of that life-support
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endangered.
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2013-09-09
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