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Taylor, RW; Esteban, R; Mahajan, S; Coulston, R;Scherman, OA; Aizpunia, J; Baumberg, JJ SimpleComposite Dipole Model for the Optical Modesof Strongly-Coupled Plasmonic Nanoparticle Aggregates,JOURNAL OF PHYSICAL CHEMISTRY C, 116(47):25044-25051; 10.1021/jp308986c NOV 29 2012Artículo:Microscopic theory of electron transitions at Si(111)-7×7:optical properties and energy-loss spectra, Cecilia Noguez,A.I. Shkrebtii y R. Del Sole, Surface Science 331- 333, 1349 – 1354 (1994).Lo citan(20):34. J.F. McGlip, Optical characterization of semiconductorsurface and interface, Progress in Surface Science49, 1 (1995).35. Zorn M, Jonsson J, Richter W, Zettler JT, PloskaK, Anisotropic reflectance from semiconductor surfacesfor in-situ monitoring in epitaxial growth systems,Physica Status Solidi A-Applied Research 152 (1): 23-34 NOV 16 199536. K. Pedersen and P. Morgen, Dispersion of 2nd harmonicgeneration on Si(111)-7×7, Physical Review B 52,R2277 (1995).37. R. Del Sole en Photonic Probes of Surfaces, Vol.2 pags.131-174, editado por P. Halevi, North-Holland (1995).38. McGlip J.F. A review of optical 2nd-Harmonic andSum-Frequency Generation at Surfaces and Interfaces,Journal of Physics D: Applied Physics 29 1812 (1996).39. K. Pedersen and P. Morgen, Optical 2nd-HarmonicGeneration Spectrsocopy on Si(111)-7×7, Surf. Sci.377, 393 (1997).40. D. Fick, R. Veith, H. D. Ebinger, H. J. Jänsch, C. Weindel,H. Winnefeld, and J. J. Paggel Electron correlationsin the clean and hydrogen-covered Si(111)-(7×7)surface at extremely low Li coverages, Phys. Rev. B6087831999.41. McGilp JF, Optical second-harmonic generation as asemiconductor surface and interface probe, Phys StatusSolidi A 175: (1) 153-167 (1999).

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