S. Ravi P. Silva

Prof. S. Ravi P. Silva

Advanced Technology Institute, University of Surrey, Guildford GU2 7XH, UK

Research Focus & Metrics

Academic Career Length

36Years (1991-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 July 1996 in Journal of Applied Physics
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JSJ. Schwan
J. Schwan
SUS. Ulrich
S. Ulrich
VBV. Batori
V. Batori
HEH. Ehrhardt
H. Ehrhardt
S. Ravi P. SilvaS. Ravi P. Silva
S. Ravi P. Silva
The origin and interpretation of the Raman features of amorphous (hydrogenated) carbon films deposited at room temperature in the region of 1000–1700 cm−1 is discussed in this paper. Possible interpretations of the linewidths, positions of the ‘‘G’’ graphite peak and ‘‘D’’ disordered peak, and their intensity ratios are examined using results obtained from magnetron sputtered and magnetic field enhanced plasma deposited films. It is shown that even small ‘‘clusters’’ of condensed benzene rings (cluster size below 20 Å) in carbon films can explain the observed Raman scattering. Besides the care that should be taken in the correct interpretation of Raman results, the utility of Raman scattering in obtaining an estimate of cluster sizes in amorphous (hydrogenated) carbon films is discussed. Carbon films prepared by magnetron sputtering show two additional Raman features at 1180 and 1490 cm−1 in addition to the G and D peaks. It is shown that a correlation exists between the 1180 cm−1 peak and the sp3 content in the films.

1 May 1996 in Nature
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KOKen Okano
Ken Okano
SKSatoshi Koizumi
Satoshi Koizumi
S. Ravi P. SilvaS. Ravi P. Silva
S. Ravi P. Silva
GAGehan A. J. Amaratunga
Gehan A. J. Amaratunga

29 April 1996 in Applied Physics Letters
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GAGehan A. J. Amaratunga
Gehan A. J. Amaratunga
S. Ravi P. SilvaS. Ravi P. Silva
S. Ravi P. Silva
Field emission measurements using 0.3 μm thick nitrogen containing hydrogenated amorphous carbon films (a‐C:H:N) on n++‐Si cathodes are reported. Onset emission fields as low as 4 V μm−1 have been obtained using a flat plate anode configuration. Uniform emission is observed over the entire cathode area at current densities below 7×10−2 mA cm−2. At higher current density preferential emission from spots is observed. The spot emission is imaged using the ITO coated plate anode. A model based on the a‐C:H:N acting as a space charge interlayer on the n++‐Si is proposed to explain the emission at low electric fields.

14 October 2013 in Nanoscale
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MAMohammad R Alenezi
Mohammad R Alenezi
SHSimon J. Henley
Simon J. Henley
NENeil G. Emerson
Neil G. Emerson
S. Ravi P. SilvaS. Ravi P. Silva
S. Ravi P. Silva
Facile and low cost hydrothermal routes are developed to fabricate three-dimensional (3D) hierarchical ZnO structures with high surface-to-volume ratios and an increased fraction of (0001) polar surfaces. Hierarchical ZnO nanowires (ZNWs) and nanodisks (ZNDs) assembled from initial ZnO nanostructures are prepared from sequential nucleation and growth following a hydrothermal process. These hierarchical ZnO structures display an enhancement of gas sensing performance and exhibit significantly improved sensitivity and fast response to acetone in comparison to other mono-morphological ZnO, such as nanoparticles, NWs, or NDs. In addition to the high surface-to-volume ratio due to its small size, the nanowire building blocks show the enhanced gas sensing properties mainly ascribed to the increased proportion of exposed active (0001) planes, and the formation of many nanojunctions at the interface between the initial ZnO nanostructure and secondary NWs. This work provides the route for structure induced enhancement of gas sensing performance by designing a desirable nanostructure, which could also be extended to synthesize other metal oxide nanostructures with superior gas sensing performance.

1 January 1997 in Journal of Applied Physics
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MCM. Chhowalla
M. Chhowalla
JRJ. Robertson
J. Robertson
CCC. W. Chen
C. W. Chen
S. Ravi P. SilvaS. Ravi P. Silva
S. Ravi P. Silva
CDC. A. Davis
C. A. Davis
WMW. I. Milne
W. I. Milne
The properties of amorphous carbon (a-C) deposited using a filtered cathodic vacuum arc as a function of the ion energy and substrate temperature are reported. The sp3 fraction was found to strongly depend on the ion energy, giving a highly sp3 bonded a-C denoted as tetrahedral amorphous carbon (ta-C) at ion energies around 100 eV. The optical band gap was found to follow similar trends to other diamondlike carbon films, varying almost linearly with sp2 fraction. The dependence of the electronic properties are discussed in terms of models of the electronic structure of a-C. The structure of ta-C was also strongly dependent on the deposition temperature, changing sharply to sp2 above a transition temperature, T1, of ≈200 °C. Furthermore, T1 was found to decrease with increasing ion energy. Most film properties, such as compressive stress and plasmon energy, were correlated to the sp3 fraction. However, the optical and electrical properties were found to undergo a more gradual transition with the deposition temperature which we attribute to the medium range order of sp2 sites. We attribute the variation in film properties with the deposition temperature to diffusion of interstitials to the surface above T1 due to thermal activation, leading to the relaxation of density in context of a growth model.

15 March 1997 in Journal of Applied Physics
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S. Ravi P. SilvaS. Ravi P. Silva
S. Ravi P. Silva
JRJ. Robertson
J. Robertson
GAG. A. J. Amaratunga
G. A. J. Amaratunga
BRB. Rafferty
B. Rafferty
LBL. M. Brown
L. M. Brown
GMG. Mariotto
G. Mariotto
The effect of nitrogen addition on the structural and electronic properties of hydrogenated amorphous carbon (a-C:H) films has been characterized in terms of its composition, sp3 bonding fraction, infrared and Raman spectra, optical band gap, conductivity, and paramagnetic defect. The variation of conductivity with nitrogen content suggests that N acts as a weak donor, with the conductivity first decreasing and then increasing as the Fermi level moves up in the band gap. Compensated behavior is found at about 7 at. % N, for the deposition conditions used here, where a number of properties show extreme behavior. The paramagnetic defect density and the Urbach tailwidth are each found to decrease with increasing N content. It is unusual to find alloy additions decreasing disorder in this manner.