Materials Map

Discover the materials research landscape. Find experts, partners, networks.

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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

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Materials Map under construction

The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

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University of Strathclyde

in Cooperation with on an Cooperation-Score of 37%

Topics

Publications (4/4 displayed)

  • 2021A universal polymer shell-isolated nanoparticle (SHIN) design for single particle spectro-electrochemical SERS sensing using different core shapes5citations
  • 2016Nondestructive Handheld Fourier Transform Infrared (FT-IR) Analysis of Spectroscopic Changes and Multivariate Modeling of Thermally Degraded Plain Portland Cement Concrete and its Slag and Fly Ash-Based Analogs12citations
  • 2012Lewis acid mediated polymerization of poly(dimethylsiloxane) polymers3citations
  • 2010Enhancement of the second harmonic signal from Hg1−xCdxTe (MCT) in the presence of an anodic oxide film2citations

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Chart of shared publication
Boccorh, Delali K.
1 / 1 shared
Macdonald, Peter A.
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Wark, Alastair
2 / 2 shared
Boyle, Colm W.
1 / 1 shared
Wain, Andrew J.
1 / 3 shared
Seelenbinder, John
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Tang, Pik Leung
1 / 2 shared
Alqassim, Mohammad
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Nicdaeid, Niamh
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Apedaile, Alistair
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Patel, Mogon
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Nikiforidis, George
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Parkinson, John Andrew
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Liggat, John J.
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Mcerlean, K.
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Cruickshank, F. R.
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Brevet, P. F.
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2016
2012
2010

Co-Authors (by relevance)

  • Boccorh, Delali K.
  • Macdonald, Peter A.
  • Wark, Alastair
  • Boyle, Colm W.
  • Wain, Andrew J.
  • Seelenbinder, John
  • Tang, Pik Leung
  • Alqassim, Mohammad
  • Nicdaeid, Niamh
  • Apedaile, Alistair
  • Patel, Mogon
  • Nikiforidis, George
  • Parkinson, John Andrew
  • Liggat, John J.
  • Mcerlean, K.
  • Cruickshank, F. R.
  • Brevet, P. F.
OrganizationsLocationPeople

article

Enhancement of the second harmonic signal from Hg1−xCdxTe (MCT) in the presence of an anodic oxide film

  • Wark, Alastair
  • Mcerlean, K.
  • Berlouis, Leonard
  • Cruickshank, F. R.
  • Brevet, P. F.
Abstract

Second harmonic generation (SHG) is now widely regarded as a valuable tool for investigating electrode surfaces. Typically, most studies have been limited to substrates which lack bulk symmetry and monitoring events such as sub-monolayer formation and surface reconstruction. Here, the development of a model that can be used to quantitatively describe the enhanced SH signal observed in the presence of an anodic oxide film on a non-centrosymmetric substrate, Hg1xCdxTe (MCT), is described. The aim is to further expand the utility of SHG for probing different electrode systems. The growth of the high quality oxide films was first followed by in-situ ellipsometry. For thin films (<100 nm) grown at a constant current density of 150 A cm2, an effectively uniform oxide layer is found with a refractive index n of ~2.15  0.05 and exhibiting no absorption of the incident radiation at 632.8 nm (1.96 eV). In the presence of such an oxide film of 58 nm thickness, the second harmonic (SH) signal intensity measured in reflection is found to be significantly enhanced in both the PIN-POUT and PIN-SOUT polarization configurations. To quantify the changes observed, each layer in the model is assigned its own symmetry and optical constants (at the fundamental,  and harmonic  (= 2) frequencies and a defined thickness. Modeling of the SH rotational anisotropy experiments carried out at different angles of incidence indicated that most of this increase could be accounted for by multiple reflections of the fundamental wave  = 1064 nm (1.17 eV) in the composite ambient/oxide/MCT layer, with little contribution from charge accumulation at the buried MCT/oxide interface for this oxide thickness.

Topics
  • density
  • impedance spectroscopy
  • surface
  • experiment
  • thin film
  • composite
  • ellipsometry
  • current density
  • monolayer formation