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5/28/2018 Switchless Bi-Directional Amplifier
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Proceedings of Asia-Pacific Microwave Conference 2006
Copyright 2006 IEICE
Switchless Bi-directional Amplifier
Chi Sun YU, Ka Tsun MOK, Wing Shing CHAN and Sai Wing LEUNG
Department of Electronic Engineering, City University of Hong Kong, Kowloon,Hong Kong, SAR PRC
Tel: +852-27844304, Fax: +852-27844712, E-mail: [email protected],
Abstract Traditional radio frequency bi-directional amplifiers rely on switches with theirassociated increase in cost, size and loss to achievetime division duplexing. A switchless bi-directionalamplifier is proposed whereby the power amplifier(PA) and Low noise amplifier (LNA) are connecteddirectly in an anti-parallel configuration.Experimental results show that there is no gaindegradation when compared with the individualpower amplifier and low noise amplifier.
Index Terms Bi-directional, Low NoiseAmplifier, Power Amplifier, Switchless, TimeDivision Duplexing
I. INTRODUCTION
Radio transceiver chips designed for standard
wireless communication applications are
becoming more integrated. In some applications
[1], the whole of the RF front end, including the
RF filter and T/R switch, is integrated into the
transceiver chip which only leaves a single RF I/O
pin for the antenna connection. This pin is used
for both transmission and reception under time
division duplex, TDD. In this case, if we want to
add an external power amplifier to increase the
transmitter output power or add an external low
noise amplifier to enhance receiver sensitivity, a
bi-directional transmit/receive module is typically
used [2, 3]. This configuration normally uses two
single pole double throw (SPDT) RF switches to
toggle between the transmitting and receiving
paths; two SPDT switches make the configuration
more expensive and also lowers the performanceby increasing the insertion loss. If these RF
switches can be eliminated and yet still provide bi-
directional amplification, it will be an ideal low
cost and simple solution for portable wireless
communication applications.
II. PROPOSED IDEA
In this paper, a switchless bi-directional
amplifier is proposed for a highly integrated radio
transceiver front-end whereby the power amplifier
(PA) and Low noise amplifier (LNA) isconnecting directly in anti-parallel as shown in
Fig. 1. The direct connection has been proven to
work well [4] but had limitations in the required
ON/OFF impedance, which the work here will
address.
In this configuration, one end of the bi-
directional amplifier module is connected to the
antenna and another end is connected to the RF
I/O of the radio transceiver chip. When
transmitting, the control signal TX_EN is used to
enable the power amplifier for operation while the
RX_EN is used to disable the low noise amplifier.
The transmission signal from the RF I/O will be
amplified by the power amplifier and then fed to
the antenna for radiation. When receiving, control
signals TX_EN and RX_EN will be toggled to
disable the power amplifier and to enable the low
noise amplifier. Received signal from the antenna
will be amplified by the low noise amplifier and
then fed to the RF I/O.
Fig. 1. Proposed bi-directional amplifier concept
For this concept to work the OFF state
impedance for both the power amplifier and the
low noise amplifier must be high (ideally an open
circuit). Since the OFF state input and output
impedance of the power amplifier and low noise
amplifier is not an ideal open circuit, the poweramplifier and low noise amplifier will load each
other during transmission and reception
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respectively. The power amplifier maximum
output power, power-amplifier/low-noise-
amplifier gain and low noise amplifier noise figure
will correspondingly be affected. In order to
minimize this effect, four transmission line lengths
(TL1, TL2, TL3 and TL4) were carefully selected
at both the input and output of the power amplifierand low noise amplifier as shown in Fig. 2.
Fig. 2. Proposed bi-directional amplifier with optimized
transmission lines
Four transmission lines are used to transform
the input and output impedance of the power
amplifier and low noise amplifier to a higher
impedance value during its OFF state, and remains
matched during its ON state. This is because the
input and output impedance of the low noise
amplifier and power amplifier are designed to be
close to the transmission line characteristic
impedance Z0, the four transmission lines will not
have much effect on the input and output
matching conditions during the ON state.
Therefore, whilst Z1 and Z2 are transformed to
high impedances, Z3 and Z4 remain close to Z0
when transmitting; Z1 and Z2 remain close to Zo
while Z3 and Z4 are transformed to high
impedances when receiving.
III. EXPERIMENTAL VERIFICATION
A circuit was designed for the 2.4GHz ISM
band to verify this idea and is shown in Fig. 3. An
Infineon BFP650 NPN RF transistor was used for
the transmit power amplifier while the Infineon
BFP620 NPN RF transistor was used for the
receive low noise amplifier. The BFP620transistor is in the common emitter configuration
and biased with a supply voltage, VCC1, of 1.5V
and a collector current of 5mA. R1 is used to set
the bias current, L1 is the choke, C1 and C2 are
the DC blocking capacitors and L2 is for output
matching. RX_EN was 1.5V to enable the low
noise amplifier while TX_EN was 0V to disable
the power amplifier during reception. The BFP650
transistor is also in the common emitterconfiguration but biased with a supply voltage
VCC2 of 2.0V and a collector current of 50mA.
R2 is used to set the bias current, L3 is the choke,
C3 and C5 are the DC blocking capacitors and
capacitor C4 is used for input matching, TX_EN
is 2.0V to enable the power amplifier while
RX_EN is 1.0V to disable the low noise
amplifier during transmission. The negative
control voltage was used here is to avoid the low
noise amplifier being turned ON by the power
amplifier at the higher output power level.
Fig. 3. Circuit diagram of proposed bi-directional
amplifier
The BFP650 power amplifier and BFP620 low
noise amplifier stages were designed separately at
2.442GHz with the input and output impedance of
both power amplifier and low noise amplifier
matched close to 50 using lumped components
in its ON state. The input impedance, output
impedance and transducer power gain GT of the
individual BFP650 power amplifier and BFP620
low noise amplifier were measured in its ON and
OFF states and are recorded below in TABLE I,
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TABLE III
INPUT IMPEDANCE,OUTPUT IMPEDANCE AND
TRANSDUCER POWER GAIN
OF BI-DIRECTIONAL AMPLIFIER
Bi-directional amplifierTransmission
Bi-directionalamplifier Reception
Z6 = 62.6+j32.2 Z6 = 118.6+j21.9 GT= 14.0dB GT= 14.4dB
Z5 = 49.1+j52.4 Z5 = 87.5+j7.0
where the notation of the input and output
impedance refers to figure 2. The input power ofthe BFP650 power amplifier was set to 0dBm
while for BFP620 low noise amplifier it was set
to 20dBm. The noise figure of the BFP620 low
noise amplifier was measured to be 1.43dB during
its ON state using a noise figure meter.
The four transmission line lengths (TL1, TL2,
TL3 and TL4) were calculated to provide phase
shifts to transform the OFF impedances to a
higher value. Transmission lines were
implemented using semi-rigid cables with outer
diameter of 2.2mm and inner conductor diameterof 0.65mm. The length of these four transmission
lines were calculated to be TL1=12mm,
TL2=26.4mm, TL3=16.8mm and TL4=43mm
respectively, and the measured input impedance,
output impedance and transducer power gain GT
of the power amplifier and low noise amplifier
after insertion of these transmission lines are
shown in TABLE II.
After insertion of these transmission lines, the
impedance of both the power amplifier and low
noise amplifier increased significantly in the OFF
state. Subsequently, a bi-directional amplifier was
constructed using these transmission line lengths
as shown in figure 3. Since the bi-directional
amplifier is targeted for portable wireless
applications, the gain and power level of the
power amplifier were adjusted to the proper levels
suited for typical 2.4GHz portable wireless
applications. The input power to the power
amplifier was set to 0dBm and the input power
level to the low noise amplifier was set to -20dBm.
Control signals TX_EN and RX_EN were used to
control the power amplifier and low noise
amplifier operation respectively. Then, the inputimpedance, output impedance and transducer
power gain GT of the bi-directional amplifier
were measured under its transmission andreception state respectively as shown in TABLE
III.
From the measurement results, the gain of the
bi-directional amplifier was 14.0dB during
transmission and 14.4dB during reception. Since
the input power during transmission was 0dBm
and the gain measured was 14.0dB, the output
power level of this bi-directional amplifier was
14.0dBm, which fulfills the typical Bluetooth
Class 1 output power requirement. The noise
figure was measured to be 2.3dB and giving a
0.87dB degradation, which is better than those
achieved using low cost PIN diode switches [5, 6]
when compared to at 2.442GHz.
In particular, there is no gain degradation during
the transmit state when comparing with the
individual power amplifier; in fact, the gain
increased by 0.3dB during the receive state when
compared with the individual low noise amplifier.
IV. CONCLUSION
In this paper, a switchless bi-directional
amplifier is proposed and examined at 2.442GHz.
14.0dB gain was achieved under transmission
with 14.0dBm output power while 14.4dB gainwas achieved under reception, which is suitable
TABLE II
INPUT IMPEDANCE,OUTPUT IMPEDANCE AND TRANSDUCER POWER GAIN OF
POWER AMPLIFIER AND LOW NOISE AMPLIFIER WITH THE FOUR TRANSMISSION LINES
PA ON state PA OFF state LNA ON state LNA OFF state
Z4= 46.5-j22.2 Z4
= 778.6-j7.5 Z1
= 47.2-j19.2 Z1
= 425.3+j405.3
GT = 13.9dB GT = -15.8dB GT = 14.4dB GT = -14.5dB
Z3= 55.9-j5.3 Z3
= 525.7-j252.2 Z2
= 63.3-j26.0 Z2
= 476.8+j189.4
TABLE I
INPUT IMPEDANCE,OUTPUT IMPEDANCE AND TRANSDUCER POWER GAIN OF
INDIVIDUAL POWER AMPLIFIER AND LOW NOISE AMPLIFIER
PA ON state PA OFF state LNA ON state LNA OFF state
Z4 = 53.5 j13.6 Z4 = 113.8+j282.6 Z1 = 83.6 j0.2 Z1 = 10.2+j55.9
GT = 14.0dB GT = -15.8dB GT = 14.1dB GT = -14.5dBZ3 = 45.9 + j11.4 Z3 = 6.9+j32.9 Z2 = 33.3 + j10.8 Z2 = 6.4-j10.4
5/28/2018 Switchless Bi-Directional Amplifier
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for Bluetooth Class 1 applications. There is no
gain degradation during both transmit and receive
states. Although the noise figure was degraded by
0.87dB in the receive state, it is similar to that
obtained with a switch and is acceptable for
Bluetooth applications. The concept behind the
switchless bidirectional amplifier has been provento work and the elimination of two SPDT RF
switches is ideally suitable for low cost
applications.
ACKNOWLEDGEMENT
The authors would like to acknowledge the City
University of Hong Kong [research grant number
7001780] for the financial support of the work
presented here. We would like to acknowledge
Agilent Technologies for the use of ADS software.
REFERENCES
[1] Zeevo ZV4002 Product Brief, Single ChipBluetoothTM Solution for Embedded Applications.
[2] W.R. Wissenman, L.C. Witkowski, G..E. Brehm,R.P. Coats, D.D. Heston, R.D. Hudgens, R.E.Lehmann, H.M. Macksey and Q.Q. Tserng, X-
Band GaAs Single-Chip T/R Radar Module,Microwave Journal, September 1987, pp.167-172.[3] Zeevo ZV4301/4002 Class-1 Design Guide APP-
1035, version 3.0 23Sep2004.[4] T.K. Lee, W.S. Chan and T.Y.M. Siu, Power
amplifier/low noise amplifier RF switch, IEEElectronics Letters, Vol. 36, No. 24, 23rdNovember 2000, pp.1983-1984.
[5] An SPDT PIN Diode T/R Switch for PCNApplications, Agilent Technologies ApplicationNote 1067.
[6] DECT(1.9GHz) Transmit-Receive PIN-DiodeSwitch, Infineon Application Note No. 007.