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27 Sep 2007: Other spots in Fig. 1(a)are related to exciton-phonon sidebands [18– 20]. ... 95, 247401 (2005).[20] Y. Miyauchi and S. Maruyama, Phys. Rev. B 74, 035415.

11 May 2007: ess: ps427@cam.ac.uk (P. Servati). along the high mobility NW core. However, carrierextraction in dye-synthesized solar cells [1,4] is stillhampered by electrode separation of more than 20 ... The light source is aBausch and Lomb 20 W halogen lamp with

28 Nov 2007: Delay (ps). SH. GIn. tens. ity(a. u.). (b). (c). 0 10 20 30 40 50 60. ... 20] M. J. O’Connell et al., Science 297, 593 (2002). [21] P.

27 Mar 2007: 1540 1560. -40. -20. 0. -3 0 3. 1570 nm. SWNT-PVA EDFA no composite/ pure PVA. ... 5a EDFA curve).The two spectral features at 1552 and 1570 nm are causedby the dispersion and non-linear processes in the fibreunder high power pumping conditions [20].

10 Dec 2007: By using the folding approach described in Refs. [20,22], we numerically integrate Eq. ... 93, 177401 (2004).[19] A. Jorio et al., Phys. Rev. Lett. 86, 1118 (2001).[20] S.

12 Feb 2007: 13,15,17–20 where kF is the wave vector for which theelectron gap is null. ... 20 300 M y. OPTICAL PHONONS IN CARBON NANOTUBES: KOHN… PHYSICAL REVIEW B 75, 035427 2007.

27 Mar 2007: in thebulk and at defects, respectively [20]. ... A 23 (2005) 1152. [20] J.A. Moulijn, A.E. van Diepen, F.

2 Mar 2007: LETTERS. 1,580 1,585 1,590 1,595. Inte. nsity. (a.u. ). – 20 V. – ... 20 and Supplementary Information):. (k, π/π, u) = h̄vF|k s(u)| (1).

18 Dec 2007: Phys. Lett.2004, 385, 298. (18) Sharma, R.J. Mater. Res.2005, 20, 1695.(19) Sharma, R.; Rez, P.; Treacy, M. ... M. J.; Stuart, S. J.J. Electron. Microsc. 2005, 54, 231.(20) Sharma, R.; Iqbal, Z.Appl.

22 Jan 2007: and 3c! Aspongelike structure is visible, formed by aggregates wdimensions ranging from several hundreds of nanomedown to 20 nm, randomly stacked. ... It should be reminded that severalmers are present in the cluster beam with different structuand