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dc.contributor.authorRashid Nizam
dc.contributor.authorS. Mahdi A. Rizvi
dc.contributor.authorAmeer Azam
dc.date.accessioned2017-05-09T00:46:24Z
dc.date.available2017-05-09T00:46:24Z
dc.date.copyrightFebruary, 2011
dc.date.issued2011
dc.identifier.issn1949-2944
dc.identifier.otherJNEMAA-28051#011014_1.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl/handle/yetl/147342
dc.description.abstractThe structural Raman spectra and NMR of the fullerene derivative (C60Br6) were simulated at room temperature from the tight-binding method and the first-principles calculations, respectively. The calculated Raman spectra results are compared with available experimental fullerene derivative (C60Br6) data. The simulated Raman spectrum of C60Br6 obtained almost all frequencies that are observed in experimental data; besides, some other frequencies are also obtained, which are not observed in the experimental data. In addition to these frequencies, further simulation to give P-polarization and U-polarization more accuracy and the polarization of experimental sample acquired become a complicated task. Besides the spectroscopic characterization of fullerene derivative (C60Br6), it also includes the prediction of C13 NMR fullerene derivative (C60Br6).
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleA Tight-Binding for Calculating the Raman Spectra and the Hartree–Fock Method Treatment for C13 NMR Spectra of Fullerenes C60Br6
dc.typeJournal Paper
dc.journal.volume2
dc.journal.issue1
dc.journal.titleJournal of Nanotechnology in Engineering and Medicine
dc.identifier.doi10.1115/1.4003258
dc.journal.fristpage11014
dc.identifier.eissn1949-2952
dc.keywordsSpectra (Spectroscopy)
dc.keywordsNuclear magnetic resonance
dc.keywordsFullerenes
dc.keywordsRaman spectra
dc.keywordsTensors
dc.keywordsPolarization (Electricity) AND Tight-binding model
dc.treeJournal of Nanotechnology in Engineering and Medicine:;2011:;volume( 002 ):;issue: 001
dc.contenttypeFulltext


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