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Volumn 55, Issue 12, 1997, Pages 7889-7903

Photoemission and electron-energy-loss-spectroscopy study of monolayers adsorbed on Cs-precovered Au(110) and of bulk distille

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EID: 0000855369     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.55.7889     Document Type: Article
Times cited : (31)

References (77)
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  • 24
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    • Science and Technology of Fullerene Materials, edited by P. Bernier, T. W. Ebbesen, V. S. Bethuri, R. M. Metzger, L. Y. Chiang, and J. W. Mintmire, MRS Symposia Proceedings No. 359 (Materials Research Society, Pittsburgh, 1995). p. 285
    • T. T. M. Palstra. O. Zhou, Y. Iwasa, P. E. Sulewski, R. M. Fleming and B. R. Zegarski, Solid State Commun. 93, 327 (1995); and in Science and Technology of Fullerene Materials, edited by P. Bernier, T. W. Ebbesen, V. S. Bethuri, R. M. Metzger, L. Y. Chiang, and J. W. Mintmire, MRS Symposia Proceedings No. 359 (Materials Research Society, Pittsburgh, 1995). p. 285.
    • (1995) Solid State Commun. , vol.93 , pp. 327
    • Palstra, T.1    Zhou, O.2    Iwasa, Y.3    Sulewski, P.4    Fleming, R.5    Zegarski, B.6
  • 39
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    • M.-Z. Huang, Y.-N. Xu and W. Y. Ching, Phys. Rev. B 46, 6752 (1992).
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    • Ching, W.1
  • 53
    • 0026960529 scopus 로고
    • The interpretation of the observed shift of the (Formula presented)(2) vibrational mode observed for K doping, x, between x=0.8 and x=1.9 of a (Formula presented) thin film as arising from continuous doping may well be incorrect. The frequency shift manifested in the (Formula presented)(2) mode between x=1.1 and x=1.9 is apparently only 2.8 (Formula presented) compared to an average frequency shift of approximately -7 (Formula presented) per extra electron per molecule over the entire range of stoichiometry. It is therefore quite possible that what is in fact being observed is a state of x≈2, as observed as an intermediate by Winter and Kuzmany [J. Winter and H. Kuzmany Solid State Commun. 84, 935 (1992)]. The x=2 phase of Winter and Kuzmany manifested a 13.3-(Formula presented) shift in the (Formula presented)(2) mode frequency with respect to undoped (Formula presented), compared to shifts of 14 (Formula presented) to 16.8 (Formula presented) observed in the range x=1.1-1.9 by Mitch, Chase, and Lannin. Shifts of the (Formula presented)(2) mode frequency are by cited Mitch, Chase, and Lannin as further evidence of solid solution formation, but the data show clearly that these frequencies cannot be adequately determined over the concentration range of interest.
    • (1992) as observed as an intermediate by Winter and Kuzmany [J. Winter and H. Kuzmany Solid State Commun. , vol.84 , pp. 935
  • 62
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    • M. J. Rice and H.-Y. Choi, Phys. Rev. B 45, 10 173 (1992).
    • (1992) Phys. Rev. B , vol.45 , pp. 10173
    • Rice, M.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.