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42414.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/Bottani_EPL1998.pdf8 Dec 2006: Our results differ considerably from those reported in [24]. c. e. ... 24] Pailard V., Melinon P., Perez J. P., Dupuis V., Perez A., Loubet J. -
INSTITUTE OF PHYSICS PUBLISHING NANOTECHNOLOGY Nanotechnology 16…
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NT2005.pdf23 Nov 2006: Rev. Mater. Res.24 83. [2] Duan X, Huang Y, Agarwal R and Lieber C M 2003 Nature421 241. -
Thermal conductivity of diamond-like carbon filmsM. Shamsa, W. L. ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Shamsha_APL2006.pdf13 Nov 2006: and E by laser induced acoustic waves and/or by surfaceBrillouin scattering.22–24 Visible and UV Raman measure-ments were performed using Renishaw Ramanspectrometers.1,25 Table I summarizes the ... 374 412GLCH 2 24 0.248 379ta-C:H 2.2 30 250 0.77 -
VOLUME 93, NUMBER 18 P H Y S I ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Piscanec_PRL2004.pdf27 Nov 2006: The EPCs near K between bands [24] allow theaccurate determination of the intensity and shape of theRaman D peak. ... Jianget al., Chem. Phys. Lett. 392, 383 (2004). [24] For the branch near A01 at K, jg2Kk0q0;Kk0j2 hg2KiF1 cos'00. -
INSTITUTE OF PHYSICS PUBLISHING NANOTECHNOLOGY Nanotechnology 17…
www-g.eng.cam.ac.uk/nms/publications/pdf/Colli_NT2006.pdf13 Nov 2006: of CdSeis only a function of the powder temperature and is independentof the Ar partial pressure [24]. ... 94 6005. [24] Merten U and Bell W E 1967 The Characterization ofHigh-Temperature Vapors (New York: Margrave) chapter 4. -
doi:10.1016/j.diamond.2005.10.049
www-g.eng.cam.ac.uk/nms/publications/pdf/Boutroy_DRM2006.pdf13 Nov 2006: C2H2 60 nm/s 0.002 cc/Package/24 H 20. CH4 4 nm/s 0.030 cc/Package/24 H 1.3. ... C2H4 25 nm/s 0.012 cc/Pckage/24 H 3.3. a BIF: Barrier Improvement Factor is the ratio of a non-coated bottle to a. -
No Job Name
www-g.eng.cam.ac.uk/nms/publications/pdf/Cantoro_NL2006.pdf13 Nov 2006: device operation.50 An optimized (pregrowth)catalyst nanostructuring, a lower C2H2 partial pressure,10,24. ... Small 2005, 1, 1180.(24) Lin, M.; YingTan, J. P.; Boothroyd, C.; Loh, K. -
PII: S0925-9635(99)00271-X
www-g.eng.cam.ac.uk/nms/publications/pdf/Conway_DRM2000.pdf6 Dec 2006: decreases,E0 is measured at lower energies and no longer over a gap defects that could not be measured by ESR [ 24 ]. Robertson [ 25 ] demonstrated that it is possible to fit ... Robertson, Phys. Rev. B 53 (1996 ) 1594. [ 24 ] F. -
PRL 95, 236802 (2005) P H Y S I ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Lazzeri_PRL2005.pdf20 Nov 2006: DFTcalculations are done with the gradient corrected functionalof Ref. [24]. We use plane waves (40 Ry cutoff ) andpseudopotential approaches [25]. ... 24] J. P. Perdew, K. Burke, and M. Ernzerhof, Phys. Rev. -
doi:10.1016/j.diamond.2003.12.018
www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_DRM2004b.pdf27 Nov 2006: Fig. 2b shows the G peakdispersion of HCA(t)a-C:N films against N content.Here the G dispersion decreases from 0.24 to 0.1cm ynm, with increasing N ... b). This can be understood if we consider the crosssectional structure of ta-C filmsw13,24,25x.
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