The Scientific World Journal

The Scientific World Journal / 2014 / Article

Research Article | Open Access

Volume 2014 |Article ID 136340 | 6 pages | https://doi.org/10.1155/2014/136340

100 nm AlSb/InAs HEMT for Ultra-Low-Power Consumption, Low-Noise Applications

Academic Editor: J. F. Paris
Received30 Aug 2013
Accepted05 Jan 2014
Published23 Feb 2014

Abstract

We report on high frequency (HF) and noise performances of AlSb/InAs high electron mobility transistor (HEMT) with 100 nm gate length at room temperature in low-power regime. Extrinsic cut-off frequencies of 100/125 GHz together with minimum noise figure  dB and associated gain  dB at 12 GHz have been obtained at drain bias of only 80 mV, corresponding to 4 mW/mm DC power dissipation. This demonstrates the great ability of AlSb/InAs HEMT for high-frequency operation combined with low-noise performances in ultra-low-power regime.

1. Introduction

Though the best high frequency performances are obtained for InAlAs/InGaAs HEMT technology which is more mature [1], AlSb/InAs HEMTs are potentially excellent candidates for low-voltage, low-power consumption operation in the case of high-speed analog and digital applications [2]. AlSb/InAs heterostructures are grown since the 1980s [3, 4], but AlSb/InAs HEMT with noticeable RF figures-of-merit and amplifiers with interesting low-noise performances have only been obtained since the last ten years [5, 6].

The best extrinsic of 303 GHz has been reached for a transistor with 120 nm gate length at drain bias of 0.44 V [7]. The main modifications regarding our previous work [7, 8] lie in an optimization of heterostructure growth conditions [9], no ohmic cap layer [10], and the use of alternative metallic gate stack [11]. With this technology, the highest combination of cut-off frequencies obtained simultaneously for AlSb/InAs HEMTs has recently been shown at  mV [10], beyond previous record of 260/280 GHz reported for 100 nm HEMT at  mV [12]. Cut-off frequencies of 290/335 GHz were obtained for a 120 nm HEMT. We presently focus on HEMT operation in mobility regime ( mV) in which we will demonstrate that no impact ionization occurs. In these low drain bias conditions, corresponding to ultra-low-power dissipation, previous works report of 112/107 GHz for ( V;  mW/mm) [5] and of 143/115 GHz at ( V;  mW/mm) [7]. In this study, we present a full set of characteristics at  mV regarding DC, HF, and noise performances, extracting RF figures-of-merit, extrinsic and intrinsic parameters, and noise parameters obtained from small-signal equivalent circuit with noise sources.

2. Heterostructure and Device Fabrication

2.1. Heterostructure

The AlSb/InAs heterostructure was grown by molecular beam epitaxy on 3-inche semi-insulating GaAs substrate. A thick AlSb buffer is used to accommodate the large lattice mismatched between 6.1 Å materials and GaAs substrate. Then, the structure consists of a 120 Å InAs channel, a 65 Å AlSb spacer, a Te δ-doping plane, and a composite Schottky barrier with a 25 Å Al0.8Ga0.2Sb layer and a 50 Å Al0.5In0.5As layer (Figure 1). The Al0.5In0.5As layer in the composite Schottky barrier avoids oxidation of Al0.8Ga0.2Sb with air exposure and acts as a hole barrier [13]. Hall measurements at room temperature exhibit a sheet carrier density of 1.5 × 1012 cm−2 and electron mobility of 26000 cm²/(Vs), giving sheet resistance of 160 Ω/□.

2.2. Device Fabrication

HEMTs fabrication starts with ohmic contact evaporation of Pd/Pt/Au after e-beam lithography, followed by rapid thermal annealing at 275°C. Despite the absence of highly doped cap layer in the heterostructure, contact resistance, obtained by transmission-line model measurements, is still below 0.05 Ω·mm. Schottky T-gate is realized using bilayer resist e-beam lithography process and Mo/Pt/Au metallization. Then, Ti/Au bonding pads are evaporated. Finally, the active area is defined by chemical deep mesa isolation using HF/H2O2 solution to completely remove the AlSb buffer, leading to air-bridge gate. Device features are a two-finger 100 nm long gate with 2 × 25 μm transistor width (Figure 2). Source-drain spacing is 1.2 μm.

3. Static and Dynamic Measurements

Drain current-voltage characteristics are plotted in Figure 3. Pinch-off voltage is −1.0 V. Maximum drain currents are 220 mA/mm and 620 mA/mm for drain bias of 80 mV and 240 mV, respectively. These are similar to our previous results [7, 8] despite the higher sheet resistance of the heterostructure and the higher source-drain spacing in the present device.

HF measurement setup consists in a 67 GHz Agilent PNA for -parameters on-wafer measurements and an Agilent HP4142 generator for DC biasing. Extrinsic current gain and unilateral power gain for  mV and  mV at peak are presented in Figure 4. Cut-off frequencies (, ) obtained simultaneously at  mV are (108 GHz, 129 GHz) for power dissipation  mW/mm and (232 GHz, 250 GHz) at  mV for  mW/mm. is calculated as , with power consumption in the gate being negligible.

In Figure 5, the evolution of extrinsic cut-off frequencies is plotted as a function of for   mV and   mV. This evidences the ability of AlSb/InAs HEMT for RF performances in low drain bias regime. In fact, (, ) are (100 GHz, 125 GHz) for  mW/mm at  mV. The DC power consumption at  mV for reaching the same cut-off frequencies is, respectively, 30 mW/mm and 22 mW/mm. Consequently, to get the same RF performances in more standard drain bias conditions, power consumption must be at least 5 times higher.

Finally, intrinsic and extrinsic parameters have been extracted from the small-signal equivalent circuit (SSEC) presented in Figure 6.

Resistance parallel to and current source parallel to output conductance to account, respectively, for gate leakage current and impact ionization have been added to the classical model. Indeed, there is impact ionization in AlSb/InAs HEMT at high drain bias with an increase of gate current and a typical bell-shape of the - characteristic [14], which is a signature of impact ionization in DC measurements. With RF characterization, impact ionization results in parameter evolving from inductive to capacitive behaviour with increasing frequency as can be seen for  mV in Figure 7. In the literature, this phenomenon in HEMTs has been modelised with a low-pass filter [15]. We prefer to introduce an additional current source controlled by gate-drain voltage as realized by Isler [16] to account for impact ionization effects. This model allows to perfectly fit scattering parameters at  mV and  mV as shown in Figure 7.

Parameters extracted from the SSEC at peak are presented in Table 1. is much higher at  mV compared to  mV, which is relevant of much lower gate leakage current, and is negligible at  mV, which stresses that there is no impact ionization at this drain voltage.


(mV)   (Ω/mm)   (Ω·mm) (Ω·mm) (S/mm) (S/mm) (fF/mm) (fF/mm) (S/mm) (k Ω)

80740.110.110.750.734683270.00780
240740.110.111.360.725842591.4712

4. Noise Measurements

Regarding low impact ionization occurring at  mV as shown above with RF wideband measurements, SSEC with noise sources as presented in Figure 8 is used. For the sake of simplicity, there is no current source accounting for impact ionization since extracted value of at  mV is negligible. As a consequence, no additional noise source, which should probably be correlated with output noise current or even input noise voltage, is required for extraction of accurate parameters values. We extracted the following noise parameters using method [17]: minimum noise figure , associated gain , noise equivalent resistance , and output noise temperature at 12 GHz (Figures 9 and 10). is 0.5 dB and is 12 dB for 4 mW/mm power dissipation. As a comparison, we should quote results obtained by Ma et al. [5] for 2 × 20 μm HEMT with above 0.5 dB at 12 GHz in the “best bias conditions for minimum noise figure.” The present results should also be compared with similar and reported in literature for AlSb/InAs HEMTs but with 50% higher DC power consumption of 6 mW/mm at  mV [6, 18]. In the present case, at  mV, , and are optima for  mW/mm and it is important to underline that it would be impossible to reach these noise performances at  mV with such low-power consumption. Despite an accurate extraction of noise parameters under high drain bias is not done here, the element values would obviously be degraded due to the higher gate voltage required to operate in low-power regime, which would increase shot noise. Then, drain polarization of transistor at  mV allows an excellent compromise between noise performances and power dissipation.

5. Conclusion

In this study, we reported on microwave and noise performances in low-power regime of AlSb/InAs HEMTs with optimized heterostructure. Combined (, ) of (100 GHz, 125 GHz) have been obtained at  mV and DC power consumption of 4 mW/mm, performances that cannot be reached at  mV for such a low power dissipation. A small-signal equivalent circuit was established and demonstrated that impact ionization effects at  mV are negligible, which is not the case for  mV. This allowed an accurate extraction of noise parameters thanks to SSEC with noise sources fully reliable in mobility regime.  dB and  dB have been obtained at 12 GHz for ( mV;  mW/mm). These results exhibit the high suitability of AlSb/InAs HEMTs for combined RF and low-noise performances in ultra-low-power dissipation regime.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

This work is supported by the National Research Agency under Projects Low IQ (no. ANR-08-NANO-022) and SMIC (no. ANR-11-ASTR-031-03).

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Copyright © 2014 Cyrille Gardès et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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