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Phonon linewidths and electron-phonon coupling in graphite and…
www-g.eng.cam.ac.uk/nms/publications/pdf/Lazzeri_PRB2006.pdf13 Nov 2006: 2Cambridge University, Engineering Department, 9 JJ Thompson Avenue, Cambridge CB3 0FA, United KingdomReceived 29 August 2005; revised manuscript received 24 February 2006; published 25 April 2006. ... S. Dresselhaus, Phys. Rev. B 71,045417 2005. 24 P. B. -
doi:10.1016/j.diamond.2005.12.045
www-g.eng.cam.ac.uk/nms/publications/pdf/Golovko_DRM2006.pdf13 Nov 2006: Fichet, W.T.S. Huck, Langmuir 19 (2003) 1963.[24] Y.N. Xia, G.M. Whitesides, Adv. -
PII: S0925-9635(99)00233-2
www-g.eng.cam.ac.uk/nms/publications/pdf/LiBassi_DRM2000.pdf6 Dec 2006: Diamond and Related Materials 9 (2000 ) 771–776www.elsevier.com/locate/diamond. Density, sp3 content and internal layering of DLC films byX-ray reflectivity and electron energy loss spectroscopy. A. LiBassi a, A.C. Ferrari b,, V. Stolojan c, B.K. -
PHYSICAL REVIEW B 67, 155306 ~2003! Interpretation of infrared ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_PRB2003.pdf28 Nov 2006: F. 04510 MexicoReceived 12 June 2002; revised manuscript received 24 January 2003; published 9 April 2003! ... matic groups. TheG peak position varies roughly linearlwith excitation wavelength.24 Figure 17b! -
doi:10.1016/j.diamond.2003.10.086
www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_DRM2004.pdf27 Nov 2006: Byplotting j vs. time, this givesbya;0.24 w34x. Usingour a value, we find an independent value ofb between0.006 and 0.12. -
Renewable Electricity ImpEE IMPRO VIN G ENG INEERIN G ...
www-g.eng.cam.ac.uk/impee/topics/RenewElectricity/files/Renewable%20Electricity%20v4%20PDF%20WITH%20NOTES.pdf11 Jun 2006: litre. Grid Electricity1 0.43 - -Natural Gas 0.19 - -. Fuel Oil 0.27 3223 -Diesel 0.25 3164 2.63Petrol 0.24 3135 2.30. -
Using JPF1 format
www-g.eng.cam.ac.uk/nms/publications/pdf/Rodil_JAP2001.pdf4 Dec 2006: For rings containing N a contribu-tion between 1400 and 1500 cm21 from NvN vibrations hasbeen suggested,24 but it seems unphysical at low nitrogecontents. -
Raman spectroscopy of hydrogenated amorphous carbons C. Casiraghi, A. …
www-g.eng.cam.ac.uk/nms/publications/pdf/Casiraghi_PRB2005.pdf13 Nov 2006: Further information. FIG. 24. Color online a DispG and b FWHMG@244 asa function of the H content for amorphous carbons, includingGLCHH. ... Met. 139, 885 2003.24 S. Piscanec, M. Lazzeri, F. Mauri, A. -
USING STANDARD SYSTE
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_PRB2000b.pdf6 Dec 2006: Received 24 November 1999! The model and theoretical understanding of the Raman spectra in disordered and amorphous carbon aregiven. ... become localized.24 Olefinic CvCbonds are shorter than aromatic bonds, so they have hi. -
JOURNAL OF APPLIED PHYSICS VOLUME 90, NUMBER 4 15 ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Ilie_JAP2001.pdf4 Dec 2006: The anisotropy in bonding can also be deteby EELS.24. The surface work functionf was measured usingKelvin probe in order to correlate it with changes in thes p2. ... Thisconclusion is further supported byK-edge EELSmeasurements.24. Figure 4 shows the
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