Search

20 Feb 2006: 2419.5. 2324.5. 2208.94. 2206.19. 2108.67. 2097.96. 2042.24. 2038.81. 1984.96. 1819.94. 1815.18. ... 1211.24. 1176.47. 1147.32. 1080.84. 1012.11. 963.47. 771.78. 655.02. 509.12. 456.62. 456.58.

20 Feb 2006: 0.06. 0.28. 0.24. 1.22. 58.05. 0.98. 11.75. 469. 36.47. 43.89. Water Debt (km3/year).

14 Dec 2006: The sp3 content of the films isestimated at 10% from X-ray photoemission and electron energy loss spectroscopy [19, 24]. ... P., Phys. Rev. B, 35 (1987) 2946. [24] Li Bassi A., Piseri P., Milani P., Ferrari A.

11 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.

28 Nov 2006: 2Department of Physics and Materials Science, City University of Hong Kong, Hong Kong SAR, ChinaReceived 29 July 2003; revised manuscript received 5 September 2003; published 24 December 2003! ... 24. To summarize, RCF gives a downshift and

13 Nov 2006: 26] (see footnote 24, for qK, 00 0) andRef. [24]. This differs from the model of Ref. ... Pfeiffer et al., Phys. Rev. B 71, 155409 (2005).[24] J. Maultzsch, S.

28 Nov 2006: 1 10 10010. 100. β/α =0.24. Cor. rela. tion. leng. ht(n. ... D. Lempert, and E. Grossman, Phys. Rev.Lett. 72, 2753 (1994). [24] R.

28 Nov 2006: 23,24]. Furthermore, electronic Raman scattering introdu-. ces an extra dependence of the lineshape with the excitation. ... 24] N.H. Nickel, P. Lengsfeld, I. Sieber, Phys. Rev., B 61 (2000) 15558.

4 Dec 2006: study.24. The dispersion of thev 1 andv 3 modes arises naturally inthis model. ... was attributed to nanocrystalline diamond, due to its negligible dispersion.24 Although its posi-tion agrees with the maximum in the diamond VDOS, wdisagree with this

6 Dec 2006: Thepresence of a RamanD peak at;1350 cm21 indicates thatthe s p2 phase is clustering into aromatic rings.18 There is arelationship23,24 between the in-plane correlation lengthL a ofthe ... 2.24 I (D)/I (G) is derived from the Raman spectra

8 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.

13 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

23 Nov 2006: Rev. Mater. Res.24 83. [2] Duan X, Huang Y, Agarwal R and Lieber C M 2003 Nature421 241.

27 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.

13 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.

13 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.

13 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.

6 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.

27 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.

11 Jun 2006: Diesel. 0.25. 3164. 2.63. Petrol. 0.24. 3135. 2.30. Other Coal2.