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A High-Efficiency, Small-Size GaN Doherty Amplifier for LTE Micro ...

A High-Efficiency, Small-Size GaN Doherty Amplifier for LTE Micro ...

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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.

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