Magnetic circular dichroism in soft X-ray resonant inelastic scattering: concepts and perspectives
Tài liệu tham khảo
Kotani, 2001, Rev. Mod. Phys., 73, 203, 10.1103/RevModPhys.73.203
Duda, 2000, J. Electron Spectrosc. Relat. Phenom., 110–111, 287, 10.1016/S0368-2048(00)00169-9
Yablonskikh, 2001, Phys. Rev. B, 63, 235117, 10.1103/PhysRevB.63.235117
Borgatti, 2002, Phys. Rev. B, 65, 094406, 10.1103/PhysRevB.65.094406
As a matter of fact the final 3s hole mixes via configuration interaction with the state with two final 3p holes (i.e. 3p4) so that the situation is more complicated in general terms. However, this configuration interaction is not important in the use of sum rules discussed below. This is demonstrated in Ref. [9].
Braicovich, 1998, Solid State Commun., 105, 263, 10.1016/S0038-1098(97)10108-9
In inner shell scattering the only price to pay is an increase of the saturation effects due to the low absorption in the emission channel with a modification of the measured L3/L2 branching ratio. This is a minor inconvenient since the L2 excitation is not used in this approach.
Braicovich, 1999, Phys. Rev. Lett., 82, 1566, 10.1103/PhysRevLett.82.1566
Taguchi, 2004, Phys. Rev. B, 69, 212414, 10.1103/PhysRevB.69.212414
Fukui, 2001, J. Phys. Soc. Jpn., 70, 3457, 10.1143/JPSJ.70.3457
Thole, 1995, Phys. Rev. Lett., 74, 237, 10.1103/PhysRevLett.74.2371
Braicovich, 2002, Phys. Rev. B, 66, 174435, 10.1103/PhysRevB.66.174435
van Veenendaal, 1996, Phys. Rev. B, 54, 16010, 10.1103/PhysRevB.54.16010
van der Laan, 1995, J. Phys.: Condens. Mat., 7, 9947, 10.1088/0953-8984/7/50/028
Braicovich, 2003, Phys. Rev. Lett., 90, 117401, 10.1103/PhysRevLett.90.117401
van der Laan, 2004, Phys. Rev. B, 69, 104427, 10.1103/PhysRevB.69.104427
Chassé, 2003, Phys. Rev. B, 68, 214402, 10.1103/PhysRevB.68.214402