1982
DOI: 10.1088/0022-3719/15/6/028
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The surface polaron and its phase diagram

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Cited by 16 publications
(14 citation statements)
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“…II.A) was particularly influential and became an important part of many subsequent publications. We mention Gross (1955);Haga (1955); Fulton (1956); Pines (1963); Dichtel (1966); Larsen (1966) and (1968); Roseler (1968); Barentzen (1975); Cahill (1975);Huybrechts (1976) and(1977); Tokuda (1980aTokuda ( , 1980band Bogoliubov, Kireev, and Kurbatov (1987). A significantly new development began with the advent of functional-integral methods (see the pioneering work of Feynman, 1955); in combination with refined variational procedures, they proved to be an extremely powerful tool, if not the most powerful.…”
Section: A-> Comentioning
confidence: 99%
“…II.A) was particularly influential and became an important part of many subsequent publications. We mention Gross (1955);Haga (1955); Fulton (1956); Pines (1963); Dichtel (1966); Larsen (1966) and (1968); Roseler (1968); Barentzen (1975); Cahill (1975);Huybrechts (1976) and(1977); Tokuda (1980aTokuda ( , 1980band Bogoliubov, Kireev, and Kurbatov (1987). A significantly new development began with the advent of functional-integral methods (see the pioneering work of Feynman, 1955); in combination with refined variational procedures, they proved to be an extremely powerful tool, if not the most powerful.…”
Section: A-> Comentioning
confidence: 99%
“…Before reporting the results systematically we should like to examine first the validity of replacing V(e, x ) by V(e, 7). It is easilydone by examining the 11 dependence of the crucial quantities like V (and energy).…”
Section: Resultsmentioning
confidence: 99%
“…With this assumption, the normalized !PA@) the GS eigenfunction of -7; -@/e) -v$ -(yfz) used in where a is approximately the thickness of the electronic density perpendicular and outside the surface. With (16), (13) (a constant) and (14) can now be evaluatc The SO phonon-induced attractive potential (14) is therefore given by M. BHATTACHARYA, S. MURHOPADHYAY, and T. K. MITRA Therefore, V(e, z) may be replaced in good approximation by V(e, 7 ) where q is a small constant parameter which replaces 6 + x. Although we make this assumption a priori for reasons of simplicity in this first investigation it will be found from actual (a posteriori) results that for two 7-values chosen two orders of magnitude different from each other, the change in the result is only fractional (= 5%), thus justifying our assumptions.…”
Section: Formulationsmentioning
confidence: 99%
“…The problem of an electron interacting with the surface elementary excitations on a semi-infinite medium has been the subject of considerable interest in the past decades [1][2][3][4][5][6][7][8][9][10]. This interaction is interesting from a technological viewpoint in the context of surface spectroscopy and the study of the optical properties of polar thin films and interfaces.…”
Section: Introductionmentioning
confidence: 99%
“…They considered the cases where the electron is outside and inside the crystal. Tokuda [2], and Bodas and Hipolito [3] considered only the case where the electron lies outside the crystal. They observed a phase--transition-like behavior from the quasi-free to the self--trapping electron state as the electron-phonon coupling constant exceeds a certain critical value.…”
Section: Introductionmentioning
confidence: 99%