A. R. Long
University of Glasgow
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Publication
Featured researches published by A. R. Long.
Physical Review B | 2005
M. Pioro-Ladrière; John H. Davies; A. R. Long; A. S. Sachrajda; Louis Gaudreau; P. Zawadzki; J. Lapointe; J. A. Gupta; Z. R. Wasilewski; S. A. Studenikin
We have studied switching (telegraph) noise at low temperature in
IEEE Transactions on Nanotechnology | 2007
K. Kalna; James A. Wilson; David A. J. Moran; R.J.W. Hill; A. R. Long; R. Droopad; Matthias Passlack; I.G. Thayne; Asen Asenov
\mathrm{Ga}\mathrm{As}∕{\mathrm{Al}}_{x}{\mathrm{Ga}}_{1\ensuremath{-}x}\mathrm{As}
Physical Review B | 2000
David E. Grant; A. R. Long; John H. Davies
heterostructures with lateral gates and introduced a model for its origin, which explains why noise can be suppressed by cooling samples with a positive bias on the gates. The noise was measured by monitoring the conductance fluctuations around
Surface Science | 1994
R. Cuscó; M. Holland; J. H. Davies; Ivan A. Larkin; E. Skuras; A. R. Long; S.P. Beaumont
{e}^{2}∕h
Journal of Applied Physics | 2011
G. W. Paterson; M. Holland; S. Bentley; I.G. Thayne; A. R. Long
on the first step of a quantum point contact at around
Semiconductor Science and Technology | 1993
A. R. Long; J. H. Davies; M Kinsler; S Vallis; M. Holland
1.2\phantom{\rule{0.3em}{0ex}}\mathrm{K}
Journal of Vacuum Science & Technology B | 2007
M. Holland; C.R. Stanley; W Reid; I.G. Thayne; G. W. Paterson; A. R. Long; P. Longo; J. Scott; A.J. Craven; R. Gregory
. Cooling with a positive bias on the gates dramatically reduces this noise, while an asymmetric bias exacerbates it. Our model is that the noise originates from a leakage current of electrons that tunnel through the Schottky barrier under the gate into the conduction band and become trapped near the active region of the device. The key to reducing noise is to keep the barrier opaque under experimental conditions. Cooling with a positive bias on the gates reduces the density of ionized donors. This builds in an effective negative gate voltage so that a smaller negative bias is needed to reach the desired operating point. This suppresses tunneling from the gate and hence the noise. The reduction in the density of ionized donors also strengthens the barrier to tunneling at a given applied voltage. Further support for the model comes from our direct observation of the leakage current into a closed quantum dot, around
Journal of Vacuum Science & Technology B | 2007
M. Holland; C.R. Stanley; W Reid; R.J.W. Hill; David A. J. Moran; I.G. Thayne; G. W. Paterson; A. R. Long
{10}^{\ensuremath{-}20}\phantom{\rule{0.3em}{0ex}}\mathrm{A}
Journal of Applied Physics | 2012
G. W. Paterson; S. Bentley; M. Holland; I.G. Thayne; Jaesoo Ahn; Rathnait Long; Paul C. McIntyre; A. R. Long
for this device. The current was detected by a neighboring quantum point contact, which showed monotonic steps in time associated with the tunneling of single electrons into the dot. If asymmetric gate voltages are applied, our model suggests that the noise will increase as a consequence of the more negative gate voltage applied to one of the gates to maintain the same device conductance. We observe exactly this behavior in our experiments.
Journal of Applied Physics | 2008
G. W. Paterson; P. Longo; J.A. Wilson; A.J. Craven; A. R. Long; I.G. Thayne; Matthias Passlack; R. Droopad
The potential performance of implant free heterostructure In0.3Ga0.7As channel MOSFETs with gate lengths of 30, 20, and 15 nm is investigated using state-of-the-art Monte Carlo (MC) device simulations. The simulations are carefully calibrated against the electron mobility and sheet density measured on fabricated III-V MOSFET structures with a high-kappa dielectric. The MC simulations show that the 30 nm gate length implant free MOSFET can deliver a drive current of 2174 muA/mum at 0.7 V supply voltage. The drive current increases to 2542 muA/mum in the 20 nm gate length device, saturating at 2535 muA/mum in the 15 nm gate length one. When quantum confinement corrections are included into MC simulations, they have a negligible effect on the drive current in the 30 and 20 nm gate length transistors but lower the 15 nm gate length device drive current at 0.7 V supply voltage by 10%. When compared to equivalent Si based MOSFETs, the implant free heterostructure MOSFETs can deliver a very high performance at low supply voltage, making them suitable for low-power high-performance CMOS applications