Please use this identifier to cite or link to this item:
http://hdl.handle.net/10397/5885
DC Field | Value | Language |
---|---|---|
dc.contributor | Institute of Textiles and Clothing | - |
dc.creator | Zhang, K | - |
dc.creator | Li, H | - |
dc.creator | Li, L | - |
dc.creator | Bian, XF | - |
dc.date.accessioned | 2014-12-11T08:24:27Z | - |
dc.date.available | 2014-12-11T08:24:27Z | - |
dc.identifier.issn | 0003-6951 | - |
dc.identifier.uri | http://hdl.handle.net/10397/5885 | - |
dc.language.iso | en | en_US |
dc.publisher | American Institute of Physics | en_US |
dc.rights | © 2013 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. The following article appeared in Zhang, K. et al., Appl. Phys. Lett. 102, 071907 (2013) and may be found at http://link.aip.org/link/?apl/102/071907 | en_US |
dc.subject | Copper | en_US |
dc.subject | Correlation methods | en_US |
dc.subject | Metallic thin films | en_US |
dc.subject | Molecular dynamics method | en_US |
dc.subject | Statistical analysis | en_US |
dc.title | Why does the second peak of pair correlation functions split in quasi-two-dimensional disordered films? | en_US |
dc.type | Journal/Magazine Article | en_US |
dc.description.otherinformation | Author name used in this publication: Li, L. | en_US |
dc.identifier.spage | 1 | - |
dc.identifier.epage | 4 | - |
dc.identifier.volume | 102 | - |
dc.identifier.issue | 7 | - |
dc.identifier.doi | 10.1063/1.4793187 | - |
dcterms.abstract | Molecular dynamics simulation has been performed to study the splitting of the second peak in pair correlation functions of quasi-two-dimensional disordered film. A quasi-two-dimensional inhomogeneous structural model, which contains both crystal-like and disordered regions, supports the hypothesis that the splitting of the second peak is result of a statistical average of crystal-like and disordered structural regions in the system, not just the amorphous structure. The second-peak splitting can be viewed as a prototype of the crystal-like peak exhibiting distorted and vestigial features. | - |
dcterms.accessRights | open access | en_US |
dcterms.bibliographicCitation | Applied physics letters, 18 Feb. 2013, v. 102, no. 7, 071907, p. 1-4 | - |
dcterms.isPartOf | Applied physics letters | - |
dcterms.issued | 2013-02-18 | - |
dc.identifier.isi | WOS:000315596700019 | - |
dc.identifier.scopus | 2-s2.0-84874524826 | - |
dc.identifier.eissn | 1077-3118 | - |
dc.description.oa | Version of Record | en_US |
dc.identifier.FolderNumber | OA_IR/PIRA | en_US |
dc.description.pubStatus | Published | en_US |
Appears in Collections: | Journal/Magazine Article |
Files in This Item:
File | Description | Size | Format | |
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Zhang_why_second_peak.pdf | 1.29 MB | Adobe PDF | View/Open |
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