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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.

20 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.

14 Dec 2006: Barborini et al.r Chemical Physics Letters 300 1999 633–638 637. w xcoordination 24,25.

13 Nov 2006: Peng et al. [24] reported a root. mean square (rms) roughness of 0.11 nm in a-C:H deposited. ... Technol. 174–175 (2003) 1135. [24] X.L. Peng, Z.H. Barber, T.W. Clyne, Surf.

13 Nov 2006: like,thick CNFs at temperatures as low as 200 C [24]. ... Phys. 44 (2005) 1558. [24] M. Cantoro, S. Hofmann, et al.

22 Nov 2006: obtained here compared to previous films produced by the. small ECWR [24] can be explained by the relatively high. ... 24] A.C. Ferrari, J. Robertson, M.G. Beghi, C.E. Bottani, R. Ferulano, R.

13 Nov 2006: corresponding bulkmaterial.24 However, an increasing temperature softens theE2g phonons,25 whereas we observe a hardening of the Ramanline in the nanotube-rich areas, Figure 3a. ... 24) Piscanec, S.; Cantoro, M.; Ferrari, A. C.; Zapien, J. A.; Lifshitz, Y

11 Dec 2006: Fisica and Unitaa INFM, Politecnico di Torino, Corso Duca degli Abruzzi 24, I-10129 Torino, Italyb Dip.

6 Dec 2006: 85 (av.) 31.4 (av.) 3.24 63.5ta-C:H Homog. 70 28.4 2.35 70 6 30ta-C:H Homog 70 28.4 2.35 43 8.4 ... cm3and a internal layer 63.5 nm thick, with density of3.24 g/cm3[ 12].

13 Nov 2006: Nominally sub-eutectic NW syn-thesis using Au as catalyst has been achieved for severalsemiconductor materials, including Ge [22], InP [23], andZnSe [24]. ... 5, 761 (2005)24 A. Colli, S. Hofmann, A.C. Ferrari, C. Ducati, F.

13 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.

13 Nov 2006: Fichet, W.T.S. Huck, Langmuir 19 (2003) 1963.[24] Y.N. Xia, G.M. Whitesides, Adv.

6 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.

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.

27 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.

4 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.

28 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!

13 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.

28 Nov 2006: Figure 2d! shows SiNWs grown from a colloidal Aususpension. As in previous reports,24 the SiNWs have diam-eters slightly larger than the colloidal diameter of 16 nDespite an initial homogenous

4 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

6 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.

12 Dec 2006: 0,24. 0,26. 0,28. 0,30. 0,32. 0,34. G Peak Dispersion (cm-1/nm). Fluence (J/cm-2)Fig. 7. G peak dispersion vs. ... The low frequency Raman spectra of low fluence filmsshow the low frequency double peak structure at about400 and 800 cm1, typical of

12 Dec 2006: There have been a number of strategies to reducestress in as-depositeda-C:H films, such as incorporatingmetals,24 silicon,25 or multilayers.26 However, metal incor-poration has drawbacks such

15 Jun 2006: 24. Recycling Statistics. 4%3%. 5%. 16%15%. Fiber57%. FiberStrappingFood/Beverage ContainersNon-Food containersFilm SheetOther.

6 Dec 2006: II. EXPERIMENTAL DETAILS. The amorphous carbon films were deposited withFCVA system described previously.24 The arc current waskept constant at 75 A and the magnetic field induced bycoils was 20 mT.

4 Dec 2006: the low frition coefficient ofa-C:H to a higher relative humidity.15–24.

4 Dec 2006: Yoshikawaet al.,24 Tamoret al.,25 and Pocsiket al.26 studieddiamondlike a-C:H. Callejaet al.15 made the first resonanRaman study of diamond, Wagner and co-workers23,27 gavethe MW

20 Nov 2006: tubes have outstanding elastical properties and are chemi-cally intert.23,24 They can thus be envisioned as a protectivecage in the nanoworld.

27 Nov 2006: 10.1098/rsta.2004.1452. Raman spectroscopy of amorphous,nanostructured, diamond-like. carbon, and nanodiamond. By A n d r e a C a r l o Ferrari a n d J o h n Robertson. Department of Engineering, University of Cambridge,Trumpington Street, Cambridge