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Effective masses and conformal mappings. / Kargaev, P.; Korotyaev, E.

In: Communications in Mathematical Physics, Vol. 169, No. 3, 05.1995, p. 597-625.

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Harvard

Kargaev, P & Korotyaev, E 1995, 'Effective masses and conformal mappings', Communications in Mathematical Physics, vol. 169, no. 3, pp. 597-625. https://doi.org/10.1007/BF02099314

APA

Kargaev, P., & Korotyaev, E. (1995). Effective masses and conformal mappings. Communications in Mathematical Physics, 169(3), 597-625. https://doi.org/10.1007/BF02099314

Vancouver

Kargaev P, Korotyaev E. Effective masses and conformal mappings. Communications in Mathematical Physics. 1995 May;169(3):597-625. https://doi.org/10.1007/BF02099314

Author

Kargaev, P. ; Korotyaev, E. / Effective masses and conformal mappings. In: Communications in Mathematical Physics. 1995 ; Vol. 169, No. 3. pp. 597-625.

BibTeX

@article{fb23698ea8284ac3b5dde4eb70674952,
title = "Effective masses and conformal mappings",
abstract = "Let Gn, N∞N, denote the set of gaps of the Hill operator. We solve the following problems: 1) find the effective masses Mn±, 2) compare the effective mass Mn± with the length of the gap Gn, and with the height of the corresponding slit on the quasimomentum plane (both with fixed number n and their sums), 3) consider the problems 1), 2) for more general cases (the Dirac operator with periodic coefficients, the Schr{\"o}dinger operator with a limit periodic potential). To obtain 1)-3) we use a conformal mapping corresponding to the quasimomentum of the Hill operator or the Dirac operator.",
author = "P. Kargaev and E. Korotyaev",
year = "1995",
month = may,
doi = "10.1007/BF02099314",
language = "English",
volume = "169",
pages = "597--625",
journal = "Communications in Mathematical Physics",
issn = "0010-3616",
publisher = "Springer Nature",
number = "3",

}

RIS

TY - JOUR

T1 - Effective masses and conformal mappings

AU - Kargaev, P.

AU - Korotyaev, E.

PY - 1995/5

Y1 - 1995/5

N2 - Let Gn, N∞N, denote the set of gaps of the Hill operator. We solve the following problems: 1) find the effective masses Mn±, 2) compare the effective mass Mn± with the length of the gap Gn, and with the height of the corresponding slit on the quasimomentum plane (both with fixed number n and their sums), 3) consider the problems 1), 2) for more general cases (the Dirac operator with periodic coefficients, the Schrödinger operator with a limit periodic potential). To obtain 1)-3) we use a conformal mapping corresponding to the quasimomentum of the Hill operator or the Dirac operator.

AB - Let Gn, N∞N, denote the set of gaps of the Hill operator. We solve the following problems: 1) find the effective masses Mn±, 2) compare the effective mass Mn± with the length of the gap Gn, and with the height of the corresponding slit on the quasimomentum plane (both with fixed number n and their sums), 3) consider the problems 1), 2) for more general cases (the Dirac operator with periodic coefficients, the Schrödinger operator with a limit periodic potential). To obtain 1)-3) we use a conformal mapping corresponding to the quasimomentum of the Hill operator or the Dirac operator.

UR - http://www.scopus.com/inward/record.url?scp=0002254974&partnerID=8YFLogxK

U2 - 10.1007/BF02099314

DO - 10.1007/BF02099314

M3 - Article

AN - SCOPUS:0002254974

VL - 169

SP - 597

EP - 625

JO - Communications in Mathematical Physics

JF - Communications in Mathematical Physics

SN - 0010-3616

IS - 3

ER -

ID: 86258333