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Volumn 65, Issue 9, 2002, Pages 1-10

Magnetic circular dichroism in resonant x-ray emission from impurities: Results at the (formula presented) edges of Mn in Ni

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EID: 84867967598     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.65.094406     Document Type: Article
Times cited : (1)

References (40)
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    • 0034895108 scopus 로고    scopus 로고
    • When our paper was ready to be submitted a more extensive account of the results on Mn alloys given already in the present Ref. 9 has been published, Since the basic messages are not changed in this new publication, our work on Mn impurities takes into account both contributions by M.V. Yablonskikh et al.
    • When our paper was ready to be submitted a more extensive account of the results on Mn alloys given already in the present Ref. 9 has been published: M. V. Yablonskikh, Yu. M. Yarmoshenko, V. I. Grebennikov, E. Z. Kurmaev, S. M. Butorin, L.-C. Duda, J. Nordgren, S. Plogmann, and M. Neumann, Phys. Rev. B 63, 235117 (2001). Since the basic messages are not changed in this new publication, our work on Mn impurities takes into account both contributions by M.V. Yablonskikh et al.
    • (2001) Phys. Rev. B , vol.63 , pp. 235117
    • Yablonskikh, M.V.1    Yarmoshenko, Y.M.2    Grebennikov, V.I.3    Kurmaev, E.Z.4    Butorin, S.M.5    Duda, L.-C.6    Nordgren, J.7    Plogmann, S.8    Neumann, M.9
  • 12
    • 85038284954 scopus 로고    scopus 로고
    • This also implies that no correction to the raw data will be needed in experiments possible not too far from now
    • This also implies that no correction to the raw data will be needed in experiments possible not too far from now.
  • 14
    • 85038308870 scopus 로고    scopus 로고
    • Some hints on the measurement of the outgoing polarization are given in Ref. 8
    • Some hints on the measurement of the outgoing polarization are given in Ref. 8.
  • 23
    • 85038292943 scopus 로고    scopus 로고
    • cases 10, 11, and 12 the spectrum is distributed in a wide energy range and in case 10 the scattering cross section is very low. Thus it has not been possible to obtain a statistics comparable to the other spectra as it is clear from Fig. 11. The spectra from cases 10 to 12 in Fig. 11 have roughly 50% more broadening since they have been numerically smoothed with a Gaussian convolution. This has no effect on the position of the main inelastic peak of spectrum 10
    • In cases 10, 11, and 12 the spectrum is distributed in a wide energy range and in case 10 the scattering cross section is very low. Thus it has not been possible to obtain a statistics comparable to the other spectra as it is clear from Fig. 11. The spectra from cases 10 to 12 in Fig. 11 have roughly 50% more broadening since they have been numerically smoothed with a Gaussian convolution. This has no effect on the position of the main inelastic peak of spectrum 10.
  • 28
    • 85038340557 scopus 로고    scopus 로고
    • For example, an optimized experiment at the new beam line ID08 of the ESRF can probably go close to this ideal condition. This new beam line is supporting the first experiments starting from spring 2001
    • For example, an optimized experiment at the new beam line ID08 of the ESRF can probably go close to this ideal condition. This new beam line is supporting the first experiments starting from spring 2001.
  • 32
    • 0000050315 scopus 로고    scopus 로고
    • We have done also the calculation in the “two-step model,” where absorption and emission processes are decoupled, by neglecting the cross products in the development of the square modulus of Eq. (1). We only mention that the full calculation gives much better agreement with the experiment than this approximation, especially for the intensity of the elastic peak compared to the inelastic part. A detailed comparison between the exact calculation and the “two-step” model is beyond the scope of the present work and will be given elsewhere. This comparison for a simpler nonmagnetic case is done in
    • We have done also the calculation in the “two-step model,” where absorption and emission processes are decoupled, by neglecting the cross products in the development of the square modulus of Eq. (1). We only mention that the full calculation gives much better agreement with the experiment than this approximation, especially for the intensity of the elastic peak compared to the inelastic part. A detailed comparison between the exact calculation and the “two-step” model is beyond the scope of the present work and will be given elsewhere. This comparison for a simpler nonmagnetic case is done in F. M. F. de Groot, Phys. Rev. B 53, 7099 (1996).
    • (1996) Phys. Rev. B , vol.53 , pp. 7099
    • De Groot, F.M.F.1
  • 39
    • 0034899997 scopus 로고    scopus 로고
    • The effect of the incident bandpass is a Gaussian convolution. The bandpass of the incident beam is accounted for in an exact way as done in
    • The effect of the incident bandpass is a Gaussian convolution. The bandpass of the incident beam is accounted for in an exact way as done in L. Braicovich, M. Taguchi, F. Borgatti, G. Ghiringhelli, A. Tagliaferri, N. B. Brookes, T. Uozumi, and A. Kotani, Phys. Rev. B 63, 245 115 (2001).
    • (2001) Phys. Rev. B , vol.63 , Issue.245 , pp. 115
    • Braicovich, L.1    Taguchi, M.2    Borgatti, F.3    Ghiringhelli, G.4    Tagliaferri, A.5    Brookes, N.B.6    Uozumi, T.7    Kotani, A.8


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.