This page contains a Flash digital edition of a book.
research  review Supressing leakage in


nitride diodes Leakage currents in Schottky barrier diodes plummet by seven orders of magnitude when the barrier composition is shifted from Al0.21


Ga0.79 N to Al0.11 Ga0.89 N.


ENGINEERS from Central Research Lab, Hitachi, have shown that reverse leakage currents in AlGaN/GaN Schottky barrier diodes can plummet through reductions in sheet carrier density.


High leakage currents are an Achilles heel for today’s GaN diodes, which hold much commercial promise thanks to their combination of high temperature, high frequency and high power.


It is widely believed that the dominant cause of leakage is structural defects, especially dislocations, which can result from strain in the AlGaN layer.


However, initial studies by the Hitachi researchers indicated that sheet carrier density also influences leakage current.


This finding motivated these engineers to carry out further work involving three AlGaN/GaN heterostructures that shared a 3.6 µm, highly-resistive GaN buffer layer and a 5 nm GaN cap.


In these samples, barrier compositions were Al0.11 Al0.21


Ga0.89 Ga0.79 N, Al0.16 Ga0.84 N and N, and corresponding room-


temperature two-dimensional electron gas densities determined by Hall measurements were 3.6 x 1012 6.6x1012


cm-2 respectively.


“We prepared those three samples with our own MOCVD [tool] under precisely controlled conditions,” says lead author Akihisa Terano. “We think that the material quality of our three samples is almost the same.”


All three epiwafers were processed into planar Schottky barrier diodes with contacts formed by electron beam evaporation (see Figure 1).


Measurements on the devices revealed that a three-fold fall in the density of the two-dimensional electron gas results in a reduction in leakage current by seven


and 1.0 x 1013 cm-2


cm-2 ,


, orders of magnitude (see Figure 2).


Unfortunately, slashing leakage current with this approach has its downsides.


“A reduction in the sheet density is thought to lead to some increase in the resistance of the drift layer, resulting in some decrease of the forward current,” explains Terano.


He and his co-workers are now planning to tackle this issue head-on, developing devices that combine a sufficiently high forward current with a low leakage.


A. Terano et al. Electron. Lett. 48 274 (2012)


Modelling of growth dynamics is a challenging computational task as it requires simulation of realistic QD sizes with atomistic resolution.


By performing a systematic set of multi- million atom atomistic simulations, the researchers in Ireland found a correlation between their calculations and the experimentally measured data.


The results quantitatively show the influence of indium-gallium intermixing and indium segregation effects on the polarisation properties of the QDs.


M. Usmanet et al. Nanotechnology 23 165202 (2012)


April / May 2012 www.compoundsemiconductor.net 51


Figure 2.Massive changes in leakage current result from relatively small changes in the density of the two- dimensional electron gas


Multi-million-atom QD metrology


Researchers have used a simulation of InAs quantum dots to accurately reproduce experimentally measured optical spectra


GROWTH DYNAMICS in real quantum dot devices has been modelled by an international team from Tyndall National Institute, Ireland, the National Nanotechnology Laboratory-CNR, Italy, and Purdue University, Indiana. The researchers used multi-million atom simulations that are claimed to deliver unprecedented precision.


Figure 1.Schottky diodes built by Hitachi feature 1000 µm by 200 µm cathodes and anodes,separated by 200 µm


The semiconductor device simulation tool, called NEMO 3D, was developed at NASA and Purdue. This tool can model structures containing up to 50 million atoms through parallelised computation on high performance supercomputing clusters.


By accurately mimicking indium-gallium intermixing and indium-segregation effects with an innovative two-layer composition model for quantum dots (QDs), the researchers can reproduce polarisation- dependent optical emission spectra of an MBE-grown InAs QD.


Tyndall has proposed an innovative two- composition model for the InAs QDs, comprised of an indium-rich central core surrounded by an indium-poor region close to the edges of the QD. This model allowed the researchers to reproduce the experimentally measured optical spectra.


Page 1  |  Page 2  |  Page 3  |  Page 4  |  Page 5  |  Page 6  |  Page 7  |  Page 8  |  Page 9  |  Page 10  |  Page 11  |  Page 12  |  Page 13  |  Page 14  |  Page 15  |  Page 16  |  Page 17  |  Page 18  |  Page 19  |  Page 20  |  Page 21  |  Page 22  |  Page 23  |  Page 24  |  Page 25  |  Page 26  |  Page 27  |  Page 28  |  Page 29  |  Page 30  |  Page 31  |  Page 32  |  Page 33  |  Page 34  |  Page 35  |  Page 36  |  Page 37  |  Page 38  |  Page 39  |  Page 40  |  Page 41  |  Page 42  |  Page 43  |  Page 44  |  Page 45  |  Page 46  |  Page 47  |  Page 48  |  Page 49  |  Page 50  |  Page 51  |  Page 52  |  Page 53  |  Page 54  |  Page 55  |  Page 56  |  Page 57  |  Page 58  |  Page 59  |  Page 60  |  Page 61  |  Page 62  |  Page 63  |  Page 64  |  Page 65  |  Page 66  |  Page 67  |  Page 68  |  Page 69  |  Page 70  |  Page 71  |  Page 72  |  Page 73  |  Page 74  |  Page 75  |  Page 76  |  Page 77  |  Page 78  |  Page 79  |  Page 80  |  Page 81  |  Page 82  |  Page 83  |  Page 84  |  Page 85  |  Page 86  |  Page 87  |  Page 88  |  Page 89  |  Page 90  |  Page 91  |  Page 92  |  Page 93  |  Page 94  |  Page 95  |  Page 96  |  Page 97  |  Page 98  |  Page 99  |  Page 100  |  Page 101  |  Page 102  |  Page 103  |  Page 104  |  Page 105  |  Page 106  |  Page 107  |  Page 108  |  Page 109  |  Page 110  |  Page 111  |  Page 112  |  Page 113  |  Page 114  |  Page 115  |  Page 116  |  Page 117  |  Page 118  |  Page 119  |  Page 120  |  Page 121  |  Page 122  |  Page 123  |  Page 124  |  Page 125  |  Page 126  |  Page 127  |  Page 128  |  Page 129  |  Page 130  |  Page 131  |  Page 132  |  Page 133  |  Page 134  |  Page 135  |  Page 136  |  Page 137  |  Page 138  |  Page 139  |  Page 140  |  Page 141  |  Page 142  |  Page 143  |  Page 144  |  Page 145  |  Page 146  |  Page 147  |  Page 148  |  Page 149  |  Page 150  |  Page 151  |  Page 152  |  Page 153  |  Page 154  |  Page 155  |  Page 156  |  Page 157  |  Page 158  |  Page 159  |  Page 160  |  Page 161  |  Page 162  |  Page 163  |  Page 164  |  Page 165  |  Page 166  |  Page 167  |  Page 168  |  Page 169  |  Page 170  |  Page 171  |  Page 172  |  Page 173  |  Page 174  |  Page 175