Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/111303
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dc.contributorDepartment of Applied Physics-
dc.creatorZhao, XAen_US
dc.creatorOng, CWen_US
dc.creatorTsang, YCen_US
dc.creatorWong, YWen_US
dc.creatorChan, PWen_US
dc.creatorChoy, CLen_US
dc.date.accessioned2025-02-17T01:38:54Z-
dc.date.available2025-02-17T01:38:54Z-
dc.identifier.issn0003-6951en_US
dc.identifier.urihttp://hdl.handle.net/10397/111303-
dc.language.isoenen_US
dc.publisherAIP Publishing LLCen_US
dc.rights© 1995 American Institute of Physics.en_US
dc.rightsThis article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. This article appeared in Zhao, X. A., Ong, C. W., Tsang, Y. C., Wong, Y. W., Chan, P. W., & Choy, C. L. (1995). Reactive pulsed laser deposition of CNx films. Applied Physics Letters, 66(20), 2652-2654 and may be found at https://doi.org/10.1063/1.113114.en_US
dc.titleReactive pulsed laser deposition of CNₓ filmsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage2652en_US
dc.identifier.epage2654en_US
dc.identifier.volume66en_US
dc.identifier.issue20en_US
dc.identifier.doi10.1063/1.113114en_US
dcterms.abstractCarbon nitride (CNx) films were prepared by reactive pulsed laser deposition at nitrogen partial pressure PN2varying from 0 to 300 mTorr. It is found that the atomic fraction of nitrogen f in the films first increases with increasing PN2reaches a maximum of 0.32 at PN2=100 mTorr, and then decreases to a saturated value of 0.26 at PN2>200 mTorr. Because of the absence of energetic particles in reactive pulsed laser deposition, the limited nitrogen content cannot be attributed to preferential sputtering of nitrogen that is generally observed in particle-assisted deposition of CN x films. Infrared absorption experiments show the existence of CN bonds and graphitic sp2 bonds. The sp2 bonds become IR active because of symmetry breaking of graphitic rings as a consequence of nitrogen incorporation. CNx films deposited at low P N2 (e.g., 5 mTorr) are more graphitic than the diamondlike pure carbon sample deposited at PN2=0, so have a slightly narrower electron band gap Eopt and a significantly higher room-temperature electrical conductivity σR. At P N2>200 mTorr, nitrogenation of the films is very pronounced, leading to a wide band gap (Eopt>1.5 eV), long electron band tail (E0>0.7 eV), and extremely low σR(<1×10-13Ω-1 cm -1). In addition, both the hardness and Young's modulus are greatly reduced, for example, from 41.3 and 285 GPa for the pure carbon sample to 1.2 and 23.8 GPa, respectively, at f=0.32.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationApplied physics letters, 15 May 1995, v. 66, no. 20, p. 2652-2654en_US
dcterms.isPartOfApplied physics lettersen_US
dcterms.issued1995-05-15-
dc.identifier.scopus2-s2.0-51149218763-
dc.identifier.eissn1077-3118en_US
dc.description.validate202502 bcch-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_Others-
dc.description.fundingSourceOthersen_US
dc.description.fundingTextHong Kong Polytechnic Universityen_US
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryVoR alloweden_US
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