HAL Id: hal-00553308
https://hal.archives-ouvertes.fr/hal-00553308
Submitted on 7 Jan 2011
HAL is a multi-disciplinary open access
archive for the deposit and dissemination of sci-
entific research documents, whether they are pub-
lished or not. The documents may come from
teaching and research institutions in France or
abroad, or from public or private research centers.
L’archive ouverte pluridisciplinaire HAL, est
destinée au dépôt et à la diffusion de documents
scientifiques de niveau recherche, publiés ou non,
émanant des établissements d’enseignement et de
recherche français ou étrangers, des laboratoires
publics ou privés.
A Methodology for multi-band class E RF PA design.
Antoine Diet, Martine Villegas, Geneviève Baudoin, Fabien Robert
To cite this version:
Antoine Diet, Martine Villegas, Geneviève Baudoin, Fabien Robert. A Methodology for multi-band
class E RF PA design.. IEEE International Microwaves Workshops Series on “RF front ends for
Software Defined and Cognitive Radio Solutions” IMWS 2010., Feb 2010, Aveiro, Portugal. p. n°7.
�hal-00553308�
A Methodology for multi-band class E RF PA design
A. Diet
1, M. Villegas
2, G. Baudoin
2, F. Robert
21
UMR 8506, L2S-DRÉ. Supélec, F-91192 Gif Sur Yvette, France. antoine.diet@lss.supelec.fr
2
Université Paris-Est, ESYCOM, EA 2552; Groupe ESIEE, Noisy-Le-Grand 93162, France.
Abstract — This paper presents a simple methodology for the design of a highly efficient PA in the context of multi- radio devices. This PA belongs to the radiofrequency reconfigurable part within a transmitter. Our goal is to improve the PA efficiency over the bandwidth. The method is based on the extraction of the transistor’s non-linear output parameters and the optimisation of a given class E topology to an ideal impedance load. Herein, the method is illustrated by an integrated design using between 2 and 4 GHz and the results of the simulations (in terms of efficiency) agree well with the transient simulation and the S-Parameters optimisation. Considerations are given for the complete development of this design and the interest for future multi- band front end designs.
Index Terms — RF architecture, multi-radio, class E PA.
I. THE MULTI-RADIO CONTEXT
Wireless communications are widely used for our daily needs. There are numerous examples which use between 2 and 4 GHz and standard names like BLUETOOTH, WiFi, WiMAX, UMTS and LTE are well-known. An important aspect of today’s applications is the increasing data rate need, especially in connectivity standards (WiFi, WiMAX), because of the user’s high Quality of Service (QoS) demands. To increase the data rate, we tend to use wideband or multi-standard architecture [1] [5]. The concept of software radio includes a self-reconfigurable radio link. While focusing on the radiofrequency (RF) part, the term multi-radio is preferred. A multi-radio RF device is supposed to use different RF flexible blocks, whose parameters are the centre/carrier frequency, bandwidth, modulation scheme and average power, see figure 1.
figure 1 : Multi-radio front-end challenges
Also, the signal dynamics (represented by the Peak to Average Power Ratio) should not decrease the transmitter’s performance. Due to the different PAPRs of the standard signals (OFDM for example), the transmitter has to be linearised, because the power amplifier (PA) introduces crippling non-linear effects (NL) [13] [4]. The
present challenge is to linearise the RF architecture while keeping high efficiency, because this is related to battery- life (especially in our context of nomadic transceiver design). Lots of linearization techniques were proposed [1] and recent works made EER/polar-based architecture very popular [6]. The envelope information can be coded by a Pulse Width Modulation or a Sigma Delta (ΣΔ) process in order to present a constant power property which is beneficial for the architecture efficiency. This coding enables its recombination by a multiplication with the carrier signal, which is modulated by the phase information. This multiplication can be achieved before the PA or by supply modulation, if the PA is in a switched (SW) class [4] such as class D, S, E or F [3].
As RF blocks are flexible, the size of the transmitter is optimized and the system efficiency is directly dependant on the different configurations. Moreover, a major design challenge is to keep a highly efficient PA for the different bands specified by the standards (carrier frequency and bandwidth). The idea of the front end design is an optimization (frequency sweeping) of a Class E PA. The Class E was chosen for its high efficiency performance and for the small number of reactive components needed, whatever the topology is [3] [7] [8] [9] [10] [11] [12] [13].
As was discussed in [2], PAs for multi-radio can be of three types: (i) broadband, (ii) reconfigurable (for example: [5]) or (iii) multi-band matching PAs. We present in this paper a simple methodology based on previous studies of Class E and optimisation processing. A slight increase in the number of reactive components can improve the bandwidth of such a PA and drive us to a dual band PA optimisation.
II. PROPOSED DESIGN METHOD
The proposed design method is summarized in figure 2.
Once the given transistor and frequency bands are chosen, the idea is to first extract the non-linear (NL) output of the transistor in switched mode of operation, in part one of the method. In that order, we performed a transient simulation where the transistor input voltage implies a hard switching behaviour (a FET is supposed here). This hypothesis is achieved by a closed loop on the gate-to- source voltage that maintains the saturation of device whatever the frequency is, see figure 2. Thanks to this simulation, we calculated the frequency-dependant gate-
to-source voltage, and the resulting input power Pin (un- matched case). A Large Signal S-Parameters (LSSP) frequency simulation, including the parametric input power Pin, computes the LSSP output matching coefficient (S22 NL) of the transistor. In part two of the method, we model the real transistor as an ideal switch with its S22 NL (impedance) in parallel: a transistor and a
capacitor, as is drawn in figure 2 and confirmed by the Smith chart. This supposes that we consider the unilaterality (S12 = 0).
At this point, we can compute the load facing the ideal switch, made up of the S22 NL, the output network (to be designed) and the antenna, as seen in Figure 2.
OPTIMISATION, with the definition of Zopt
Simulation of the transistor in switched mode over the bandwidth and computation of the corresponding input power (transient simulation)
Characteristics Vgs, Ids, Vds of the transistor Definition of the gate voltage for switched mode at each frequency
Pin
Simulation in LSSP (Pin) Large Signal S-Parameter (frequency simulation)
S22
Extraction of S22, and definition of a LC topology, loaded by the antenna.
(S-Parameter frequency simulation)
Simulation of the optimum LC network with the transistor in switched mode (transient simulation). Computation of the efficiency.
Feedback loop
Input Power
VgsFREQ (2000000000.000 to 4000000000.000)
S(2,2)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
S22 = Zout Zload S22 + Zload
EqnZ_OPT=(31.155+j*23.265) (0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
VDC Idrain
Zload Lpola Output
Network
RF08265 load j 34
opt f . R e
Z fRF
Real transistor Output Network with DC feed Antenna
Ideal transistor
NL output impedance
Vdrain OPTIMISATION, with
the definition of Zopt
Simulation of the transistor in switched mode over the bandwidth and computation of the corresponding input power (transient simulation)
Characteristics Vgs, Ids, Vds of the transistor Definition of the gate voltage for switched mode at each frequency
Pin
Simulation in LSSP (Pin) Large Signal S-Parameter (frequency simulation)
S22
Extraction of S22, and definition of a LC topology, loaded by the antenna.
(S-Parameter frequency simulation)
Simulation of the optimum LC network with the transistor in switched mode (transient simulation). Computation of the efficiency.
OPTIMISATION, with the definition of Zopt
Simulation of the transistor in switched mode over the bandwidth and computation of the corresponding input power (transient simulation)
Characteristics Vgs, Ids, Vds of the transistor Definition of the gate voltage for switched mode at each frequency
Pin
Simulation in LSSP (Pin) Large Signal S-Parameter (frequency simulation)
S22
Extraction of S22, and definition of a LC topology, loaded by the antenna.
(S-Parameter frequency simulation)
Simulation of the optimum LC network with the transistor in switched mode (transient simulation). Computation of the efficiency.
Feedback loop Feedback loop
Input Power
VgsFREQ (2000000000.000 to 4000000000.000)
S(2,2)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
VgsFREQ (2000000000.000 to 4000000000.000)
S(2,2)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
S22 = Zout Zload S22 + Zload
EqnZ_OPT=(31.155+j*23.265) (0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
EqnZ_OPT=(31.155+j*23.265) (0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
VDC Idrain
Zload Lpola Output
Network
RF08265 load j 34
opt f . R e
Z fRF
Real transistor Output Network with DC feed Antenna
Ideal transistor
NL output impedance
Vdrain
VDC Idrain
Zload Lpola Output
Network
RF08265 load j 34
opt f . R e
Z fRF
Real transistor Output Network with DC feed Antenna
Ideal transistor
NL output impedance
Vdrain
Figure 2: Proposed design method Based on numerous theoretical developments
concerning class E topologies, [13] [12] [7] [8] [9] [10]
and [11], we focused on parallel-based topologies with finite DC feed inductor. The ideal load that must face the ideal transistor (the “perfect switch” part) of this type of topology [5] [11] is Zopt(ωRF) = 0.8265 Rload ej34°, where Rload is the reactive part of the antenna (radiating part) and ωRF the centre/carrier frequency. The optimisation process goals are to match the impedance of the circuit
(S22 NL + output network + antenna) to the optimal class E load Zopt. We compute the matching coefficient ГclassE according to this criteria (50 Ohms is replaced by Z0
= Zopt = 0.8265 Rload e j34°). Once the optimisation process meets the goals, the network is incorporated into the final transient simulation in order to evaluate the resulting efficiency over the bandwidth.
We applied this method with the model of a MESFET Avago ATF50189 and a designed antenna (Vivaldi type).
Results of the S22 NL (Zout) extraction are reported in Figure 2 (left) and the antenna impedance is drawn in the left, middle smith chart. Three networks are computed: for 2 to 2.5 GHz (LTE, UMTS band), 3.2 to 3.8 GHz (WiMAX) and for both frequency bands. Figure 3 shows the results of the optimisation for the three networks, by computing the matching coefficient ГclassE . We reported the result of the final transient simulation only with the network matching both frequency bands. This networks uses one DC feed inductor of 1 nH, two grounded shunt inductors of 1.62 and 2.36 nH, two series capacitors of 0.8 and 0.9 pF and two shunt capacitors of 0.4 and 1 pF. The
efficiency and output power are drawn in Figure 3. We notice high theoretical drain efficiency in the range of 90%, corresponding to the goal parameters of our optimisation process. In practice, this will be lowered by the practical loss of the circuit. Maximum efficiencies agree well with matched frequency bands predicted by the S-Parameters simulation.
Drain to source voltages and currents are drawn for 2.3 and 3.5 GHz, in order to demonstrate the class E operation of the amplifier. We notice the negative current due to the importance of the output transistor capacitance (intrinsic) at these frequencies of operation.
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-25 -20 -15 -10 -5
-30 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9
0.0 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-25 -20 -15 -10 -5
-30 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.6 0.7 0.8 0.9
0.5 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.6 0.7 0.8 0.9
0.5 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-40 -30 -20 -10
-50 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
-2 0 2 4
-4 6
freq_optim2bis..Vcharge3, V
-50 0 50
-100 100
freq_optim2bis..Icharge.i, mA
0 2 4 6 8
-2 10
freq_optim2bis..Vdrain3, V
1. 000 1. 003
-0. 10 -0. 05 0. 00 0. 05 0. 10 0. 15 0. 20
-0. 15 0. 25
time, us ec
-freq_optim2bis..I_Probe3.i
2.3 GHz
-4 -2 0 2 4
-6 6
freq_optim2bis..Vcharge3, V
-50 0 50 100
-100 150
freq_optim2bis..Icharge.i, mA
0 2 4 6 8
-2 10
freq_optim2bis..Vdrain3, V
800 801
-0.2 -0.1 0.0 0.1 0.2 0.3
-0.3 0.4
time, nsec
-freq_optim2bis..I_Probe3.i
3.5 GHz
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-25 -20 -15 -10 -5
-30 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9
0.0 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-25 -20 -15 -10 -5
-30 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9
0.0 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-25 -20 -15 -10 -5
-30 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.6 0.7 0.8 0.9
0.5 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-25 -20 -15 -10 -5
-30 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.6 0.7 0.8 0.9
0.5 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.6 0.7 0.8 0.9
0.5 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-40 -30 -20 -10
-50 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9
2.0E9 4.0E9
13 16 19 22 25 28
10 30
0.6 0.7 0.8 0.9
0.5 1.0
VgsFREQ
10*log10(P*1000) ETA
2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 3.8
2.0 4.0
-40 -30 -20 -10
-50 0
freq, GHz
dB(G_ADAPT)dB(S(1,1))
-2 0 2 4
-4 6
freq_optim2bis..Vcharge3, V
-50 0 50
-100 100
freq_optim2bis..Icharge.i, mA
0 2 4 6 8
-2 10
freq_optim2bis..Vdrain3, V
1. 000 1. 003
-0. 10 -0. 05 0. 00 0. 05 0. 10 0. 15 0. 20
-0. 15 0. 25
time, us ec
-freq_optim2bis..I_Probe3.i
2.3 GHz
-4 -2 0 2 4
-6 6
freq_optim2bis..Vcharge3, V
-50 0 50 100
-100 150
freq_optim2bis..Icharge.i, mA
0 2 4 6 8
-2 10
freq_optim2bis..Vdrain3, V
800 801
-0.2 -0.1 0.0 0.1 0.2 0.3
-0.3 0.4
time, nsec
-freq_optim2bis..I_Probe3.i
3.5 GHz
-2 0 2 4
-4 6
freq_optim2bis..Vcharge3, V
-50 0 50
-100 100
freq_optim2bis..Icharge.i, mA
0 2 4 6 8
-2 10
freq_optim2bis..Vdrain3, V
1. 000 1. 003
-0. 10 -0. 05 0. 00 0. 05 0. 10 0. 15 0. 20
-0. 15 0. 25
time, us ec
-freq_optim2bis..I_Probe3.i
2.3 GHz
-4 -2 0 2 4
-6 6
freq_optim2bis..Vcharge3, V
-50 0 50 100
-100 150
freq_optim2bis..Icharge.i, mA
0 2 4 6 8
-2 10
freq_optim2bis..Vdrain3, V
800 801
-0.2 -0.1 0.0 0.1 0.2 0.3
-0.3 0.4
time, nsec
-freq_optim2bis..I_Probe3.i
3.5 GHz
Figure 3 : Switched mode simulation of the transistor (transient) for three types of NT : (i) single band WiFi, (ii) single band WiMAX a nd (iii) dual band WiFi/WiMAX with transient drain to source voltage and current at 2.3 and 3.5 GHz. Efficiency (ETA in purple) and Output power (red) are reported on the same figure. Matching coefficient for 50 Ohms (blue) and Zopt (red) are draw with frequency alignment.
The drain-to-source voltage is varied from 1 to 3 V and shows the independence of the efficiency and the quasi- linear variation of the output power, characterizing the saturation of the transistor. These results are shown in figure 4. It is important to evaluate this efficiency of the dual band PA over the voltage and the frequency because
the multi-radio idea implies a power control whatever the signal parameters are.
34
34
826 0
826 0
j load
-j load with R
class E
e R . Z
e R . Z Γ Z
load 2.0E9 2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9 4.0E9
13 16 19 22 25 28
10 30
0.6 0.7 0.8 0.9
0.5 1.0
VgsFREQ
10*log10(P*1000) ETA ETA1 ETA2
10*log10(P1*1000)10*log10(P2*1000)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
ГclassEin dB
S11in dB
Poutin dBm Efficiency(normalised)Vds = 1 V
Vds = 3 V
Vds = 2 V
34
34
826 0
826 0
j load
-j load with R
class E
e R . Z
e R . Z Γ Z
load 2.0E9 2.2E9 2.4E9 2.6E9 2.8E9 3.0E9 3.2E9 3.4E9 3.6E9 3.8E9 4.0E9
13 16 19 22 25 28
10 30
0.6 0.7 0.8 0.9
0.5 1.0
VgsFREQ
10*log10(P*1000) ETA ETA1 ETA2
10*log10(P1*1000)10*log10(P2*1000)
(0.000 to 0.000)
G_OPT
freq (2.000GHz to 4.000GHz)
S(1,1)
ГclassEin dB
S11in dB
Poutin dBm Efficiency(normalised)Vds = 1 V
Vds = 3 V
Vds = 2 V
Figure 4 : Results of transient simulation with the transistor and the optimized dual-band network: efficiency and output power in
function of the frequency and for Vds = 1, 2 and 3 V
III. CONCLUSION
We presented a simple methodology for class E efficiency optimisation over frequency. This method helps drive the study of broadband or multi-band PA for multi- radio. Results based on a real transistor model reach almost a one octave class E PA with reactive element values in an acceptable range for integrated design. The small number of reactive component is attractive for the design of a dual-band PA, as presented. The possibility of output power variations are simulated for slow (average power) or fast (envelope information) amplitude control.
We will extend the number of frequency bands according to multi-radio front end needs.
REFERENCES
[1] G. Baudoin et al. “Radiocommunications Numériques : Principes, Modélisation et Simulation” Dunod, EEA, 2ème édition, 2007.
[2] P. Colantino “Multi-band PA architectural solutions”
Proceedings of European Microwave Week 2009, Whorshop, Rome, 2009.
[3] S. Cripps “Advanced techniques in RF Pas design”
Norwood, MA, Artech house, 2002.
[4] A. Diet et al. “EER architecture specifications for OFDM transmitter using a class E PA” IEEE MWCL, V14 I8, 2004, pp 389-391.
[5] A. Diet et al. “Flexibility of Class E HPA for Cognitive Radio” IEEE PIMRC 2008, September, Cannes, France.
[6] A. Diet et al. “Radio Communications Architectures”
chapter of Radio Communications, ISBN 978-953-7619-X-X, IN-TECH, to appear.
[7] A. Grebennikov “Class E high efficiency PA: Historical aspects and prospects” Applied Microwave and Wireless, 2002, pp 64-71.
[8] A. Grebennikov, NO Sokal “Switch-mode RF PAs”
Burlington MA, Elsevier, 2007.
[9] M. Kazimierczuk “Class E tuned PA with shunt inductor”
IEEE journal of Solid State Circuits, vol 16, February 1981, pp 2-7.
[10] T. Mader et al. “Switched mode high efficiency microwave PAs in a free space power combiner array” IEEE trans. on MTT, Vol 46, October 2008, pp 1391-1398.
[11] T. Mury, V. Fusco. “Series-L/Parallel-Tuned Class-E Power Amplifier Analysis” Proceedings of 35th European Microwave Conference, October 2005.
[12] F. Raab “Idealised operation of the class E tuned PA” IEEE trans. on Circuits and Systems, vol. 24, December 1977, pp 725- 735.
[13] N. Sokal, A. Sokal. “Class E, A new Class of high efficiency Tuned switching PAs” IEEE JSSC, V10, N3, June 1975, pp 168-176.
[14] M. Villegas et al. “Radiocommunications Numériques:
Conception de circuits intégrés RF et micro-ondes” Dunod, EEA, 2ème édition, 2007.