A. K. Santra
Indian Institute of Science
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Featured researches published by A. K. Santra.
Applied Surface Science | 1995
A. K. Santra; C. N. R. Rao
X-ray and UV photoemission along with Auger spectroscopic studies show the formation of surface alloys in the Pd/Ag and Cu/Au overlayers on polycrystalline substrates. Surface alloy formation also occurs in the Ni/Au overlayers although Au and Ni do not form bulk alloys over the entire range of compositions.
Applied Surface Science | 1996
K. R. Harikumar; A. K. Santra; C. N. R. Rao
Abstract Cu deposited on 5 or 10 A thick ZnO layers (grown on Zn metal), has been investigated as a function of Cu coverage by employing X-ray photoelectron and Auger electron spectroscopies. The 2p core-level binding energy of Cu increases with decreasing metal coverage, the maximum shift observed (with respect to bulk Cu metal) at the smallest coverage being ∼ 0.9 eV. Temperature dependent studies show that Cu diffuses through the ZnO layer with the rate of diffusion varying with the substrate temperature as well as the oxide layer thickness. The inward diffusion of Cu results in the formation of CuZn alloys. Diffusion kinetic experiments at different temperatures show that the activation energy for diffusion increases with the increasing oxide layer thickness.
Surface Science | 1994
A. K. Santra; G. N. Subbanna; C. N. R. Rao
Bimetallic clusters of Ni-Pd, Cu-Ni, Cu-Au and Au-Ni deposited on amorphized graphite have been in- vestigated by a combined use of photoelectron spectroscopy and electron microscopy. Metal core-level binding energies (Pd 3d, Au 4f and Ni/Cu 2p) of the bimetallic clusters deposited on amorphized graphite have been measured for different coverages or mean cluster sizes. When the cluster is large, the core-level binding energy the major metallic component in the bimetallic clusters
Solid State Communications | 1993
A. K. Santra; Ram Seshadri; V. Vijayakrishnan; C. N. R. Rao
(e.g. \hspace{2mm} Cu\hspace{2mm} in\hspace{2mm} Cu_3Au \hspace{2mm} or \hspace{2mm} Cu_7Ni_3)
Surface Science | 1992
V. Vijayakrishnan; A. K. Santra; Ram Seshadri; R. Nagarajan; T. Pradeep; C. N. R. Rao
is close to that of the bulk metal while that of the minor component
Topics in Catalysis | 1994
C. N. R. Rao; A. K. Santra; V. Vijayakrishnan
(e.g. \hspace{2mm} Au \hspace{2mm} in \hspace{2mm} Cu_3Au \hspace{2mm} or \hspace{2mm} Ni \hspace{2mm} in \hspace{2mm} Cu_7Ni_3)
Solid State Communications | 1996
K.R. Harikumar; A. K. Santra
shows the effect of alloying. The effect of alloying is found in the core-level energies of both Ni and Pd in the large clusters of
Fullerenes Nanotubes and Carbon Nanostructures | 1993
Ram Seshadri; V. Vijayakrishnan; A. K. Santra; A. Govindaraj; C. N. R. Rao
Ni_3Pd_2
Journal of The Chemical Society, Chemical Communications | 1992
V. Vijayakrishnan; A. K. Santra; T. Pradeep; Ram Seshadri; Rajamani Nagarajan; C. N. Ramachandra Rao
. With the decrease in cluster size or coverage, the core-level binding energies of both the metals increase, just as in the case of monometallic clusters. The present results show the occurrence of parallel shifts in the core-level binding energy of metals due to alloying and cluster size effects, both the effects manifesting themselves in the small clusters. It is noteworthy that the core-level binding energy shifts in bimetallic clusters are distinctly different from those in bimetallic overlayers. Although alloy formation does not occur in the Au-Ni system in the bulk, the
The Journal of Physical Chemistry | 1991
T. Pradeep; V. Vijayakrishnan; A. K. Santra; C. N. R. Rao
Au_3Ni