z-logo
open-access-imgOpen Access
Magnetic circular dichroism of 3 d 5/2 → 2 p 3/2 resonant inelastic X‐ray scattering at the Ho L III ‐edge in Ho 3 Fe 5 O 12
Author(s) -
Nakamura Tetsuya,
Kawamura Naomi,
Iwazumi Toshiaki,
Maruyama Hiroshi,
Urata Akiri,
Shoji Hironobu,
Nanao Susumu,
Kishimoto Shunji,
Katano Rintaro,
Isozumi Yasuhito
Publication year - 2001
Publication title -
journal of synchrotron radiation
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.172
H-Index - 99
ISSN - 1600-5775
DOI - 10.1107/s0909049500018392
Subject(s) - resonant inelastic x ray scattering , magnetic circular dichroism , scattering , spectral line , physics , atomic physics , absorption edge , x ray absorption spectroscopy , inelastic scattering , k edge , x ray raman scattering , wiggler , absorption spectroscopy , condensed matter physics , optics , band gap , electron , quantum mechanics , astronomy , cathode ray
Magnetic circular dichroism (MCD) of resonant inelastic X‐ray scattering (RIXS) of 3 d 5/2 → 2 p 3/2 decay (Ho L α 1 ) was measured at the Ho L III ‐edge in Ho 3 Fe 5 O 12 . The MCD‐RIXS, in which the intermediate state has the 2 p 4 f n + 1 configuration due to the quadrupolar transition of 2 p → 4 f , was also observed at the pre‐edge region of the Ho L III ‐edge. The obvious superposition of two peaks, which comes from the high‐energy off‐resonant Raman scattering and the fluorescence, could be found in both the RIXS and the MCD‐RIXS when the energy of the incoming X‐ray was 7eV higher than the white line. The dependence of the integration of the MCD‐RIXS spectra on the incident x‐ray energy could roughly reproduce the MCD of X‐ray absorption spectra (XAS).

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here