2007
DOI: 10.1134/s0965542507090059
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Computing the sums of Rayleigh-Schrödinger series of perturbed self-adjoint operators

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Cited by 6 publications
(4 citation statements)
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“…The method is based on the Bubnov-Galerkin scheme as applied to the eigenvalue problem , (2.41) which can be written as . (2.43) An approximate solution of problem (2.40) is sought in the form of the sum where are the eigenvalues of T, which form a basis in H. This method is justified in detail in [25]. Next, these general results are applied to the eigenvalue problem for the Orr-Sommerfeld operator in the case of a viscous incompressible plane parallel flow between two infinite parallel planes that move rel ative to each other at constant velocities or are at rest.…”
Section: Here Andmentioning
confidence: 99%
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“…The method is based on the Bubnov-Galerkin scheme as applied to the eigenvalue problem , (2.41) which can be written as . (2.43) An approximate solution of problem (2.40) is sought in the form of the sum where are the eigenvalues of T, which form a basis in H. This method is justified in detail in [25]. Next, these general results are applied to the eigenvalue problem for the Orr-Sommerfeld operator in the case of a viscous incompressible plane parallel flow between two infinite parallel planes that move rel ative to each other at constant velocities or are at rest.…”
Section: Here Andmentioning
confidence: 99%
“…In [19] the values of were com puted up to three decimals for n = 1(1)3, R = 100, 45, , , . The method of regularized traces for computing approximate eigenvalues of differential operators was further developed in [25]. Specifically, let Т be a discrete lower semibounded Hermitian operator and Р be a bounded operator both defined in a separable Hilbert space Н.…”
Section: Here Andmentioning
confidence: 99%
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“…Ключевые слова: асимптотические формулы; собственные значения и собственные функции; дискретные и самосопряженные операторы; обратные спектральные задачи; метод Галеркина. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18] 6) 52cos( 4) 75cos( 2) 9cos( 8))…”
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