Auger Resonant Raman Scattering in Strontium Compounds

Teikichi A. SASAKI; Yuji BABA; Kenji YOSHII; Hiroyuki YAMAMOTO

doi:10.1380/jsssj.17.370

ストロンチウ厶化合物におけるオージェ共鳴ラマン散乱

佐々木貞吉, 馬場祐治, 吉井賢資, 山本博之

著者情報

ジャーナルフリー

1996 年 17 巻 7 号 p. 370-374

DOI https://doi.org/10.1380/jsssj.17.370

詳細

発行日: 1996/07/10 受付日: 1996/02/15 J-STAGE公開日: 2009/08/07 受理日: 1996/02/28 早期公開日: - 改訂日: -
訂正情報
訂正日: 2009/08/07 訂正理由: - 訂正箇所: 論文抄録訂正内容: Wrong : Sr-L₃M_{4, 5}M_{4, 5} Auger transitions in SrO, SrF₂, SrTiO₃, SrSi₂ and SrAg were studied by tuning the synchrotron radiation at the Sr2p_3/2 absorption edge (&sim;1945 eV). It was observed that the Sr-L₃M_{4, 5}M_{4, 5} spectator Auger line (&sim;1645 eV) shifts to higher electron energy side in proportion to the exciting photon energy. Detailed examination of the spectator Auger line showed that the spectral narrowings occur as well. These phenomena are discussed in relation to the localized Sr4d^*-dominant states having a band-like character and are interpreted in terms of a new type of the Auger resonant Raman scattering.
Right : Sr-L₃M_{4, 5}M_{4, 5} Auger transitions in SrO, SrF₂, SrTiO₃, SrSi₂ and SrAg were studied by tuning the synchrotron radiation at the Sr2p_3/2 absorption edge (∼1945 eV). It was observed that the Sr-L₃M_{4, 5}M_{4, 5} spectator Auger line (∼1645 eV) shifts to higher electron energy side in proportion to the exciting photon energy. Detailed examination of the spectator Auger line showed that the spectral narrowings occur as well. These phenomena are discussed in relation to the localized Sr4d^*-dominant states having a band-like character and are interpreted in terms of a new type of the Auger resonant Raman scattering.

訂正日: 2009/08/07 訂正理由: - 訂正箇所: 引用文献情報訂正内容: Wrong : 2) Y. Baba, T.A. Sasaki and H. Yamamoto: Phys. Rev. B49, 709 (1994).
3) Y. Baba, H. Yamamoto and T.A. Sasaki: Surf. Sci. 307-309, 896 (1994).
4) T.A. Sasaki, Y. Baba, K. Yoshii, H. Yamamoto and T. Nakatani: Phys. Rev. B50, 15519 (1994).
5) T.A. Sasaki, Y. Baba, K. Yoshii and H. Yamamoto: J. Phys. Cond. Matter 7, 463 (1995).
7) K. Yoshii, Y. Baba and T.A. Sasaki: J. Electron Spectrosc. Relat. Phenom. 72, 107 (1995).
9) Y. Baba, K. Yoshii, T.A. Sasaki: Surf. Sci. 341, 190 (1995).
10) T.A. Sasaki, Y. Baba, K. Yoshii and H. Yamamoto: J. Phys. Cond. Matter 7, 4385 (1995).
11) G.G. Kleiman, R. Randers, P.A.P. Nascente and S.G.C. de Castro: Phys. Rev. B46, 4405 (1992).
12) M. Elango, A. Ausmees, A. Kikas, E. Nõmmiste, R. Ruus, A. Saar, J.F. van Acker, J.N. Andersen, R. Nyholm and I. Martinson: Phys. Rev. B47, 11736 (1993).
13) W. Drube, A. Lessmann and G. Materlik: “Resonant Anomalous X-ray Scattering: Theory and Applications” ed. by G. Materlik, C.J. Sparks and K. Fischer, (North-Holland, 1994) p. 473.
14) H. Wong, J.C. Woicik, T. Åberg, M.H. Chen, A.H. Gomez, T. Kendelewicz, A. Manttykentta, K.E. Miyano, S. South-worth and B. Crasemann: Phys. Rev. B50,1359 (1994).
15) P. Eisenberger, P.M. Platzman and H. Winick: Phys. Rev. Lett. 36, 623 (1976).
16) T. Åberg and B. Crasemann: “Resonant Anomalous X-ray Scattering: Theory and Applications” ed. by G. Materlik, C.J. Sparks and K. Fischer, (North-Holland, 1994) p. 431.

Right : 2) Y. Baba, T.A. Sasaki and H. Yamamoto: Phys. Rev. B49, 709 (1994).
3) Y. Baba, H. Yamamoto and T.A. Sasaki: Surf. Sci. 307-309, 896 (1994).
4) T.A. Sasaki, Y. Baba, K. Yoshii, H. Yamamoto and T. Nakatani: Phys. Rev. B50, 15519 (1994).
5) T.A. Sasaki, Y. Baba, K. Yoshii and H. Yamamoto: J. Phys. Cond. Matter 7, 463 (1995).
7) K. Yoshii, Y. Baba and T.A. Sasaki: J. Electron Spectrosc. Relat. Phenom. 72, 107 (1995).
9) Y. Baba, K. Yoshii, T.A. Sasaki: Surf. Sci. 341, 190 (1995).
10) T.A. Sasaki, Y. Baba, K. Yoshii and H. Yamamoto: J. Phys. Cond. Matter 7, 4385 (1995).
11) G.G. Kleiman, R. Randers, P.A.P. Nascente and S.G.C. de Castro: Phys. Rev. B46, 4405 (1992).
12) M. Elango, A. Ausmees, A. Kikas, E. Nõmmiste, R. Ruus, A. Saar, J.F. van Acker, J.N. Andersen, R. Nyholm and I. Martinson: Phys. Rev. B47, 11736 (1993).
13) W. Drube, A. Lessmann and G. Materlik: “Resonant Anomalous X-ray Scattering: Theory and Applications” ed. by G. Materlik, C.J. Sparks and K. Fischer, (North-Holland, 1994) p. 473.
14) H. Wong, J.C. Woicik, T. Åberg, M.H. Chen, A.H. Gomez, T. Kendelewicz, A. Manttykentta, K.E. Miyano, S. South-worth and B. Crasemann: Phys. Rev. B50,1359 (1994).
15) P. Eisenberger, P.M. Platzman and H. Winick: Phys. Rev. Lett. 36, 623 (1976).
16) T. Åberg and B. Crasemann: “Resonant Anomalous X-ray Scattering: Theory and Applications” ed. by G. Materlik, C.J. Sparks and K. Fischer, (North-Holland, 1994) p. 431.

抄録

Sr-L₃M_{4, 5}M_{4, 5} Auger transitions in SrO, SrF₂, SrTiO₃, SrSi₂ and SrAg were studied by tuning the synchrotron radiation at the Sr2p_3/2 absorption edge (∼1945 eV). It was observed that the Sr-L₃M_{4, 5}M_{4, 5} spectator Auger line (∼1645 eV) shifts to higher electron energy side in proportion to the exciting photon energy. Detailed examination of the spectator Auger line showed that the spectral narrowings occur as well. These phenomena are discussed in relation to the localized Sr4d^*-dominant states having a band-like character and are interpreted in terms of a new type of the Auger resonant Raman scattering.

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