1989
DOI: 10.1002/pssb.2221550114
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Phase Transition and Padé Approximants for Fröhlich Polarons

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Cited by 31 publications
(26 citation statements)
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“…Among the most important shortcomings of Padé approximants, we may mention the following: the necessity of having many perturbative terms, the appearance of unphysical poles, the ability of dealing only with the so-called compatible variables, the possibility of describing only those functions that have at infinity a power-law behaviour with rational powers, and the impossibility to correctly treat nonmonotonic crossover. These difficulties are well known and repeatedly discussed in literature [10][11][12][13][14][15][16][17][18]. In addition, we remind that Padé approximation is rather a numerical method.…”
Section: Introductionmentioning
confidence: 90%
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“…Among the most important shortcomings of Padé approximants, we may mention the following: the necessity of having many perturbative terms, the appearance of unphysical poles, the ability of dealing only with the so-called compatible variables, the possibility of describing only those functions that have at infinity a power-law behaviour with rational powers, and the impossibility to correctly treat nonmonotonic crossover. These difficulties are well known and repeatedly discussed in literature [10][11][12][13][14][15][16][17][18]. In addition, we remind that Padé approximation is rather a numerical method.…”
Section: Introductionmentioning
confidence: 90%
“…[51][52][53]. The motion in the space of approximations, near a quasifixed point, is described by the evolution integral (15), which can be written as…”
Section: General Approachmentioning
confidence: 99%
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“…A solution in the weak coupling limit was given by Froehlich [11], and that in the strong coupling one was found by Pekar [1], [12]. By now rather an exact solution has been obtained for the energy of the polaron ground state in the weak coupling limit [13], [14] :…”
mentioning
confidence: 92%
“…The polaron effects of electron-interface-optical-phonon interaction result in some changes to the electron self-energy and the effective mass which are very different from those in 3D system, and have been investigated extensively. In the past years, many works on the properties of interface polaron were studied using the perturbation-theory method [3][4][5], the Lee-Low-Pines(LLP) variational method [6][7][8] and the Feynman path integral approach [9][10][11]. Hai [5], for example, investigated the polaron energy and effective mass in a quantum well by applying the perturbation-theory method, Li and Gu [7] investigated intermediate-coupling polaron in a polar-crystal slab by using LLP variational method.…”
Section: Introductionmentioning
confidence: 99%