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A <strong>High</strong>-<strong>Efficiency</strong>, <strong>Small</strong>-<strong>Size</strong> <strong>GaN</strong> <strong>Doherty</strong> <strong>Amplifier</strong><br />

<strong>for</strong> <strong>LTE</strong> <strong>Micro</strong>-Cell and Active Antenna System Applications<br />

Peter Xia, Milos Jankovic<br />

TriQuint Semiconductor, 500 W Renner Road, Richardson, TX , 75080, USA<br />

E-mail address: peter.xia@tqs.com<br />

Abstract — In this paper a high-efficiency, small-size <strong>GaN</strong><br />

<strong>Doherty</strong> amplifier <strong>for</strong> <strong>LTE</strong> micro-cell base station and active<br />

antenna systems base station application is presented. It is<br />

implemented with a TriQuint Semiconductor wideband discrete<br />

<strong>GaN</strong> RF power transistor, theT1G6001528-Q3. <strong>Doherty</strong><br />

amplifier per<strong>for</strong>mance is in the <strong>LTE</strong> standard frequency range<br />

2.62 GHz ~2.69 GHz; average output power=38.5dBm; the peak<br />

saturated output power is >46dBm; drain efficiency is >55%;<br />

gain is >15dB; 2 carrier 2x10 MHz; 8dB PAR <strong>LTE</strong> signal<br />

wave<strong>for</strong>m with Netlogic standard DPD; ACPR is better than -<br />

50dBc; <strong>Doherty</strong> amplifier size 30mm x 70mm.<br />

Index Terms — <strong>GaN</strong>, <strong>Doherty</strong> <strong>Amplifier</strong>, <strong>LTE</strong>, <strong>Micro</strong>-Cell,<br />

Active Antenna System, Base Station.<br />

I. INTRODUCTION<br />

In today’s communications networks, achieving higher data<br />

rates and spectrum efficiency are always motivations <strong>for</strong><br />

developing new technology. In order to meet the increasingly<br />

more stringent requirements of high data rate and high<br />

spectrum efficiency demanded by wireless<br />

telecommunications subscribers, the 4G wireless system<br />

including Long Term Evolution (<strong>LTE</strong>) have been developed to<br />

take advantage of some new technology. For example:<br />

Orthogonal Frequency Division Multiplexing ( OFDM ) and<br />

Multiple Input Multiple Output ( MIMO ) , which have<br />

properties of higher data rates and higher spectral efficiency in<br />

20 MHz signal bandwidth; downlink data rates of 100<br />

megabits per second ( Mbps ) and an uplink data rate of 50<br />

Mbps can be achieved. <strong>LTE</strong> modulation signal bandwidth is<br />

10 MHz <strong>for</strong> one carrier and 20MHz <strong>for</strong> two carriers. In order<br />

to provide a high data rate while consuming less power, small<br />

size base stations such as a micro-cell base stations or an<br />

active antenna system base station will be utilized more<br />

frequently in <strong>LTE</strong>-based networks than in W-CDMA (3G)<br />

networks. In this type of small-size wireless base station, highefficiency<br />

and small-sized RF power amplifiers are necessary<br />

to provide the per<strong>for</strong>mance required as cost-effectively as<br />

possible.<br />

Due to higher efficiency at a 6~10dB back-off range and<br />

better linearity with a digital pre-distortion ( DPD ) system,<br />

<strong>Doherty</strong> amplifier configurations are popularly used in<br />

wireless base station RF power amplifiers [1]~[2]. Although<br />

there are now some new advanced technology being<br />

developed <strong>for</strong> wireless base-station RF power amplifiers<br />

[3]~[4], high power and high efficiency RF amplifier<br />

configuration utilizing a <strong>Doherty</strong> amplifier configuration still<br />

is the most common wireless base station technology in mass<br />

production.<br />

A gallium nitride (<strong>GaN</strong>) RF power transistor, due to its high<br />

efficiency and high power density, has characteristics<br />

supporting the needs of next-generation RF power device<br />

applications [5]~[7] and was there<strong>for</strong>e the technology of<br />

choice <strong>for</strong> implementing this amplifier design.<br />

II. RF GAN POWER DEVICE<br />

The active device employed in the reported <strong>Doherty</strong> Power<br />

<strong>Amplifier</strong> is TriQuint Semiconductor T1G6001528-Q3<br />

packaged high electron mobility transistor (HEMT). It is a<br />

wideband discrete <strong>GaN</strong> on SiC HEMT, which operates at 28V<br />

and be able to support DC to 6 GHz frequency requirements.<br />

The device is built with TriQuint’s production 0.25μm <strong>GaN</strong><br />

on SiC process, which features advances field plate techniques<br />

to maximize power and efficiency at high drain bias operating<br />

conditions. This optimization can potentially lower systems<br />

costs in terms of simple amplifier line-ups and lower thermal<br />

management costs.<br />

The T1G6001528-Q3 uses a discrete die with 5 mm of total<br />

gate periphery. It is constructed based on four, 1.25mm unit<br />

HEMT cells, as shown in Fig. 1. The die placement and bond<br />

wire profiles are optimized <strong>for</strong> broadband per<strong>for</strong>mance.<br />

Fig. 1. T1G6001528-Q3 <strong>GaN</strong> transistor 1.25mm unit cell<br />

The packaged device utilized in this amplifier typically<br />

provides 18W of output power (P3dB) and linear gain higher<br />

than 10dB at 6 GHz. Maximum PAE is greater than 50%<br />

across the whole band. At 2.6 GHz frequency, its saturated


power is about 25W; gain is approximately 16dB; the<br />

maximum saturated efficiency is approximately 75%.<br />

Fig. 2 T1G6001528-Q3 package<br />

T1G6001528-Q3 package is show as Fig.2, the device<br />

dimension except input / output lead is 5mm x 6mm. The<br />

per<strong>for</strong>mance of this small device comes from its high power<br />

density. The small <strong>for</strong>m factor of the transistor is a key factor<br />

that enables development of a smaller-scale <strong>Doherty</strong> amplifier.<br />

The T1G6001528-Q3 provided this per<strong>for</strong>mance: Vd=28V,<br />

Idq=100mA, at pulse wave<strong>for</strong>m PW=50uS, duty=10%, its<br />

load-pull data at 2.65GHz is measured as following in Fig. 3.<br />

The reported <strong>Doherty</strong> amplifier is designed based on this loadpull<br />

data.<br />

Fig. 3 T1G6001528-Q3 load-pull data<br />

III. DOHERTY AMPLIFIER CONFIGURATION<br />

A symmetric <strong>Doherty</strong> amplifier is a very popular RF high<br />

power, high efficiency amplifier configuration <strong>for</strong><br />

contemporary wireless base stations. The amplifier<br />

demonstrated in this paper is designed using two<br />

T1G6001528-Q3 discrete packaged HEMTs, and the whole<br />

<strong>Doherty</strong> amplifier size is 30mm x 70mm as shown as Fig. 4.<br />

The small size is very necessary <strong>for</strong> micro-cell base stations or<br />

active antenna systems base stations where space is at a<br />

minimum.<br />

RF in<br />

Bias Vgs≈-­‐3.7V<br />

Idq=100mA<br />

Bias Vgs=-­‐5V<br />

Carrier amplifier<br />

T1G6001528-­‐Q3<br />

Peakingamplifier<br />

T1G6001528-­‐Q3<br />

28V Vds<br />

28V Vds<br />

Fig. 4 30mm x 70mm <strong>Doherty</strong> <strong>Amplifier</strong> Board<br />

RF out<br />

The amplifier PCB material is Taconic RF35B, with a<br />

thickness (H) of 16.6mm, and a dielectric constant (εr) of<br />

3.66.<br />

There is a 3dB hybrid at the input area, which is used to<br />

split the input signal into a carrier amplifier (the up path) and a<br />

peaking amplifier (the down path). The carrier amplifier is<br />

biased in class AB at Idq=100mA; the peaking amplifier is<br />

biased in class C mode. Since the carrier amplifier and<br />

peaking amplifier operate in different modes, their output<br />

impedances are not identical, so their output matching<br />

circuitry is slightly different.<br />

When designing a <strong>Doherty</strong> amplifier, the ideal situation is<br />

to design load impedance at Zopt equal to the maximum Psat<br />

point, and design load impedance at 2*Zopt equal to the<br />

maximum efficiency point. But because the T1G6001528-Q3<br />

is a wideband general purpose device, it is not specifically<br />

designed <strong>for</strong> 2.65 GHz <strong>Doherty</strong> purposes; its maximum<br />

efficiency is not at a 2:1 VSWR circle of the maximum<br />

saturated power. When we designed this <strong>Doherty</strong> amplifier,<br />

we had to compromise the load impedance at Zopt and 2 *<br />

Zopt. This means the load impedance at Zopt is not at the<br />

maximum saturated power point and the load impedance at 2 *<br />

Zopt is not at the maximum efficiency point.<br />

IV. DOHERTY AMPLIFIER PERFORMANCE<br />

The <strong>Doherty</strong> amplifier utilizing the T1G6001528-Q3 (as<br />

documented in Fig 3) has been measured with several kinds of<br />

signal wave<strong>for</strong>ms to characterize its per<strong>for</strong>mance <strong>for</strong> base<br />

station applications.<br />

Fig.5 shows its AM/AM and AM/PM curve, which is a<br />

critical parameter <strong>for</strong> DPD correction per<strong>for</strong>mance. In a<br />

typical normal LDMOS device <strong>Doherty</strong> amplifier, phase<br />

always drops when input power increases, which will reduce<br />

DPD correction per<strong>for</strong>mance. But in this amplifier utilizing<br />

the T1G6001528-Q3, phase variation of input power is totally<br />

different, which will be a benefit <strong>for</strong> DPD correction.


Fig.6 shows its PAR and efficiency variation with output<br />

power, which is measured at 2.65GHz, the WCDMA signal<br />

wave<strong>for</strong>m with PAR @ 0. 01% CCDF = 10.2dB.<br />

Fig. 7 shows its high power per<strong>for</strong>mance over the standard<br />

<strong>LTE</strong> frequency range of approximately 2.62GHz to 2.69GHz,<br />

which is measured with a WCDMA signal wave<strong>for</strong>m, the<br />

data is tested at 38dBm average output power, the saturated<br />

power is calculated using an average output power plus PAR.<br />

It can be seen from Fig.7 that in a standard <strong>LTE</strong> frequency<br />

range (2620 MHz~2690 MHz), when average output power at<br />

38dBm, its efficiency is higher than 55%.<br />

In contemporary base station designs, the RF power<br />

amplifier output need varies when the number of phones<br />

calling users within a given geographic area varies. This<br />

requirement is called “traffic control”. In order to let base<br />

stations always operate at high efficiency, generally the<br />

variation of output power is implemented through adjusting<br />

RF power amplifier working voltages. So that the base station<br />

Gain(dB)<br />

17<br />

16<br />

15<br />

14<br />

13<br />

12<br />

11<br />

10<br />

Output_PAR(dB)<br />

15<br />

13<br />

11<br />

9<br />

7<br />

5<br />

2.65GHz AM/AM & AM/PM<br />

Gain<br />

Phase<br />

13 15 17 19 21 23 25 27 29 31 33<br />

Pin( dBm)<br />

Fig. 5 AM/AM and AM/PM<br />

T1G6001528 <strong>Doherty</strong> Output PAR and <strong>Efficiency</strong> vs. Pout<br />

1C-­‐WCDMA , 10.2dB PAR at 0.01%CCDF<br />

30 31 32 33 34 35 36 37 38 39<br />

Pout (dBm )<br />

130<br />

128<br />

126<br />

124<br />

122<br />

120<br />

118<br />

116<br />

Phase(° )<br />

AM/AM<br />

AM/PM<br />

Fig. 6 PAR and efficiency variation with output power<br />

60<br />

56<br />

52<br />

48<br />

44<br />

40<br />

36<br />

32<br />

28<br />

24<br />

20<br />

<strong>Efficiency</strong> ( % )<br />

Psat ( dBm) & Eff ( % )<br />

Pout (dBm)<br />

60<br />

58<br />

56<br />

54<br />

52<br />

50<br />

48<br />

46<br />

44<br />

42<br />

40<br />

39.5<br />

39<br />

38.5<br />

38<br />

37.5<br />

37<br />

36.5<br />

36<br />

35.5<br />

35<br />

WCDMA Per<strong>for</strong>mance<br />

1C WCDMA , 10.2dB PAR at 0.01%CCDF<br />

Eff<br />

Psat<br />

Psat<br />

Eff<br />

Gain<br />

40<br />

10<br />

2620 2630 2640 2650 2660 2670 2680 2690<br />

Frequency ( MHz )<br />

Gain<br />

Fig. 7 Psat , Eff, Gain variation over frequency range<br />

T1G6001528 <strong>Doherty</strong> Eff and Pout @7.5dB OBO vs Drain Voltage<br />

1C-­‐WCDMA , 10.2dB PAR at 0.01%CCDF<br />

24 26 28<br />

Drain Voltage (V)<br />

30 32<br />

Fig. 8 Eff and Pout variation with drain voltage<br />

Always operates at the highest efficiency, base station RF<br />

power amplifiers are required to provide stable efficiency<br />

when working voltages change. Fig. 8 shows the drain<br />

voltage range of 24V ~ 32V, with the same WCDMA<br />

wave<strong>for</strong>m, and the same PAR (7.5dB), the efficiency and<br />

average output power varies with the voltage.<br />

To satisfy the requirements of high-efficiency base station<br />

operations, most RF power amplifiers need to operate with<br />

digital pre-distortion (DPD) to obtain linear per<strong>for</strong>mance,<br />

which is represent with ACPR in RF power amplifiers. So <strong>for</strong><br />

today’s base station RF power amplifiers, the per<strong>for</strong>mance of<br />

DPD correction is very important. In order to verify this<br />

<strong>Doherty</strong> amplifier’s DPD correction effect , the system<br />

utilized in this paper was tested with a Netlogic standard DPD<br />

system, in a two carrier <strong>LTE</strong> (20 MHz signal bandwidth)<br />

environment, with PAR @ 0.01% CCDF = 8dB. The<br />

measured ACPR per<strong>for</strong>mance at 2.65GHz is shown Fig 9, at<br />

20<br />

19<br />

18<br />

17<br />

16<br />

15<br />

14<br />

13<br />

12<br />

11<br />

60<br />

59<br />

58<br />

57<br />

56<br />

55<br />

54<br />

53<br />

52<br />

51<br />

50<br />

Gain ( dB )<br />

<strong>Efficiency</strong> (%)


38.5dBm Pout. After DPD is applied, the ACPR is better than<br />

-50dBc.<br />

ACPR (dBc)<br />

-­‐20<br />

-­‐25<br />

-­‐30<br />

-­‐35<br />

-­‐40<br />

-­‐45<br />

-­‐50<br />

-­‐55<br />

-­‐60<br />

T1G6001528 <strong>Doherty</strong> Linearity<br />

2C 0110 10MHz <strong>LTE</strong>, 8dB PAR at 0.01%CCDF, 2650MHz<br />

Be<strong>for</strong>e DPD<br />

After DPD<br />

33 34 35 36 37 38 39<br />

Pout (dBm)<br />

Eff<br />

Fig. 9 ACPR per<strong>for</strong>mance with DPD<br />

V. CONCLUSION<br />

A 2.6 GHz <strong>GaN</strong> <strong>Doherty</strong> amplifier has been demonstrated.<br />

At 38.5dBm average output power, in a standard <strong>LTE</strong><br />

frequency range of 2.62 GHz ~ 2.69 GHz, drain efficiency is<br />

greater than 55%; gain is greater than 15dB. For a two carrier<br />

20 MHz bandwidth 8dB PAR <strong>LTE</strong> signal, ACPR after DPD is<br />

better than -50dBc. The <strong>Doherty</strong> amplifier dimension is 30mm<br />

x 70mm. The combination of high efficiency and small size<br />

made possible utilizing gallium nitride transistors in a base<br />

station amplifier is very useful <strong>for</strong> <strong>LTE</strong> micro-cell base<br />

stations as well as active antenna array system designs.<br />

65<br />

60<br />

55<br />

50<br />

45<br />

40<br />

35<br />

30<br />

25<br />

Eff ( % )<br />

ACKNOWLEDGEMENT<br />

The authors would like to express their appreciation <strong>for</strong> the<br />

assistance and support of TriQuint Semiconductor’s Defense<br />

Products and Foundry Services business unit, which provided<br />

load pull fixtures, gallium nitride transistors and additional<br />

resources <strong>for</strong> the initial assessment of this project, as well as<br />

Mr. Jeff Gengler who provided DPD testing.<br />

REFERENCES<br />

[1] Steve C Cripps, “RF Power <strong>Amplifier</strong> <strong>for</strong> Wireless<br />

Communication”, Norwood, MA, Artech House, 1999.<br />

[2] Frederick H. Raab, et al., “Power <strong>Amplifier</strong> and Transmitter <strong>for</strong><br />

RF and <strong>Micro</strong>wave”, IEEE Trans. <strong>Micro</strong>wave Theory Tech.,<br />

Vol. 50 pp. 814-826, March 2002<br />

[3] D. Kimball, et al., “<strong>High</strong> <strong>Efficiency</strong> WCDMA Envelope<br />

Tracking Base-Station <strong>Amplifier</strong> Implemented with GaAs<br />

HVHBTs”, 2008 IEEE MTT-S Int. <strong>Micro</strong>wave Symposium<br />

Digest.<br />

[4] I, Kim, et al., “Envelope Injection Consideration of <strong>High</strong> Power<br />

Hybrid EER Transmitter <strong>for</strong> IEEE 802.16 Mobile WiMAX<br />

Application”, 2008 IEEE MTT-S Int. <strong>Micro</strong>wave Symposium<br />

Digest .<br />

[5] H. Deguchi, et al., “A 33W <strong>GaN</strong> HEMT <strong>Doherty</strong> <strong>Amplifier</strong> with<br />

55% Drain <strong>Efficiency</strong> <strong>for</strong> 2.6GHz Base Stations”, 2010 IEEE<br />

MTT-S Int. <strong>Micro</strong>wave Symposium Digest.<br />

[6] H. Sano, et al., “A 40W <strong>GaN</strong> HEMT <strong>Doherty</strong> Power <strong>Amplifier</strong><br />

with 48% <strong>Efficiency</strong> <strong>for</strong> WiMAX Application”, 2007 IEEE<br />

Compound Semiconductor Integrated Circuit Symposium<br />

Digest.<br />

[7] N. Yoshimura, et al., “A 2.5-2.7GHz Broadband 40W <strong>GaN</strong><br />

HEMT <strong>Doherty</strong> amplifier with higher than 45% drain efficiency<br />

<strong>for</strong> multi-band applications”, 2012 IEEE Topical Conference on<br />

Power <strong>Amplifier</strong>s <strong>for</strong> Wireless and Radio Applications.<br />

.

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