Overview of spectroscopies I (MC) - TDDFT.org

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7.37.27.4ΔE = 0.7 eVClassical molecular dynamicsLowest direct gap<strong>of</strong> diamond (E ‘ o) ,Γ 25‘ Γ 157.1Measured,Logothetidis et al.PRB 46, 4483 (1992)1000Ramírez et al.PRB 73,2452022006Squares ,Quantum (path integral)MD calculations.For diamond the volume effectis negligible:0.03eV at T=0compared with 0.7 eV total16
Because <strong>of</strong> strong electron-phonon interaction, superconductivitypossibleSuperconductivity in boron-doped (~2x10 21 cm -3 )diamond films produced by CVDMore recent T c =11.4 KY. Takano et al.Diamond and rel.mat.16, 911 (2007)Y.Takano et al., APL 85, 2851 (2004);Ekimov E.A. et al. Nature 424, 542(2004)17
Page 1 and 2: Manuel Cardona, Max-Planck- Institu
Page 3 and 4: Benedict, Shirley, Bohn, PRB 57, R9
Page 5 and 6: Albrecht et al. PRL 80.4510(1998)Ca
Page 7 and 8: Comparison of calculated with measu
Page 9 and 10: Three electron-phonon interaction t
Page 11: A single crystal of 29 Si (5% natur
Page 14 and 15: 2.9meVParks et al. PRB49,14244(1994
Page 18 and 19: Although no isotope effect measurem
Page 20 and 21: Fermi Surface of diamond and electr
Page 22 and 23: Why is the electron-phonon interact
Page 24 and 25: 2.9meVParks et al. PRB49,14244(1994
Page 26 and 27: Superconductivity in boron-doped si
Page 28 and 29: Specific heat of diamond vs.T: Eins
Page 30 and 31: Luis Viňa (Stuttgart, 1981)Patrici
Page 32 and 33: Contribution of zinc and oxygen to
Page 34 and 35: Periodic Table ( Section)Mg Al Si P
Page 36 and 37: Sharp indirect edge luminescence in
Page 38 and 39: DIAMONDT. Sato et al. PRB 65, 09210
Page 40 and 41: 90 meV, confirmed by isotope measur

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