1971
DOI: 10.1103/physrevb.3.3487
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Dynamical Theory of the Large Polaron: Fock Approximation

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Cited by 46 publications
(17 citation statements)
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“…Concerning the classical version of this technique (characterized by Feynman diagrams and analytical partial summation procedures) only very few applications can be found. The early paper of Matz and Burkey [10] may serve as a representative example which clearly indicates the reason: it fails to provide a smooth interpolation between the well known weak-and strong-coupling limits of the ground-state energy. On the other hand, such an interpolation was proven to exist (see the work of Fraehlich [11], Spohn [12] and Ref.…”
mentioning
confidence: 97%
“…Concerning the classical version of this technique (characterized by Feynman diagrams and analytical partial summation procedures) only very few applications can be found. The early paper of Matz and Burkey [10] may serve as a representative example which clearly indicates the reason: it fails to provide a smooth interpolation between the well known weak-and strong-coupling limits of the ground-state energy. On the other hand, such an interpolation was proven to exist (see the work of Fraehlich [11], Spohn [12] and Ref.…”
mentioning
confidence: 97%
“…It is well known that polaron models often support the self-trapping phenomenon, when the ground state changes in a relatively narrow interval of parameters from light-to heavy-mass state with a sharp increase in the number of phonons contributing to the polaronic cloud. The same phenomenon was advocated for the Fröhlich model by a number of authors [5][6][7][8][9][10][11], including the statement that more than one stable polaron state exists in the region of intermediate α. Clearly, if there were a sharp transformation of the polaronic ground state, it would have been immediately seen in the phonon statistics.…”
Section: B Structure Of Polaronic Cloudmentioning
confidence: 73%
“…Moreover, as any linear combination of sufficiently large number R of randomly chosen parent configurations C fin η , η = 1, ..., R smoothes the saw-tooth noise, the deviation of a summary configuration C fin ref is normally lower than that of each additive one. 6. Elementary updates of class I (A) Shift of rectangular.…”
Section: Final Solution and Refinementmentioning
confidence: 99%
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“…This shows that both approaches, Eqs. (43) and (39), lead to the same wavefunction and the same Pekar energy, Eq. (42).…”
Section: B Self-localizationmentioning
confidence: 99%