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Integral representation of solutions of the wave equation based on Poincaré wavelets. / Perel, Maria V.

Proceedings of the International Conference Days on Diffraction 2009. Institute of Electrical and Electronics Engineers Inc., 2009. стр. 159-161.

Результаты исследований: Публикации в книгах, отчётах, сборниках, трудах конференций › статья в сборнике материалов конференции › научная

Harvard

Perel, MV 2009, Integral representation of solutions of the wave equation based on Poincaré wavelets. в Proceedings of the International Conference Days on Diffraction 2009. Institute of Electrical and Electronics Engineers Inc., стр. 159-161, 2009 International Conference Days on Diffraction, DD 2009, St. Petersburg, Российская Федерация, 26/05/09.

APA

Perel, M. V. (2009). Integral representation of solutions of the wave equation based on Poincaré wavelets. в Proceedings of the International Conference Days on Diffraction 2009 (стр. 159-161). Institute of Electrical and Electronics Engineers Inc..

Vancouver

Perel MV. Integral representation of solutions of the wave equation based on Poincaré wavelets. в Proceedings of the International Conference Days on Diffraction 2009. Institute of Electrical and Electronics Engineers Inc. 2009. стр. 159-161

Author

Perel, Maria V. / Integral representation of solutions of the wave equation based on Poincaré wavelets. Proceedings of the International Conference Days on Diffraction 2009. Institute of Electrical and Electronics Engineers Inc., 2009. стр. 159-161

BibTeX

@inproceedings{2fce7fcd27a1424bb9e12f7935aa4330,
title = "Integral representation of solutions of the wave equation based on Poincar{\'e} wavelets",
abstract = "We present here an exact integral representation of solutions of the wave equation with constant coefficients in two spatial dimensions in terms of localized solutions. A solution is given as a superposition of localized solutions each of which lives in the reference system, which moves in the x direction with velocity v. To obtain any solution, we must take into account all |v| ≤ c, where c is the velocity of wave propagation, and use also shifts and scaling. The representation is constructed by means of space-temporal wavelet theory which is applied to the section of a solution in the plane y = 0.",
author = "Perel, {Maria V.}",
note = "M. V. Perel, {"}Integral representation of solutions of the wave equation based on Poincar{\'e} wavelets,{"} Proceedings of the International Conference Days on Diffraction 2009, St. Petersburg, Russia, 2009, pp. 159-161.; 2009 International Conference Days on Diffraction, DD 2009 ; Conference date: 26-05-2009 Through 29-05-2009",
year = "2009",
language = "English",
isbn = "9781424448746",
pages = "159--161",
booktitle = "Proceedings of the International Conference Days on Diffraction 2009",
publisher = "Institute of Electrical and Electronics Engineers Inc.",
address = "United States",

}

RIS

TY - GEN

T1 - Integral representation of solutions of the wave equation based on Poincaré wavelets

AU - Perel, Maria V.

N1 - M. V. Perel, "Integral representation of solutions of the wave equation based on Poincaré wavelets," Proceedings of the International Conference Days on Diffraction 2009, St. Petersburg, Russia, 2009, pp. 159-161.

PY - 2009

Y1 - 2009

N2 - We present here an exact integral representation of solutions of the wave equation with constant coefficients in two spatial dimensions in terms of localized solutions. A solution is given as a superposition of localized solutions each of which lives in the reference system, which moves in the x direction with velocity v. To obtain any solution, we must take into account all |v| ≤ c, where c is the velocity of wave propagation, and use also shifts and scaling. The representation is constructed by means of space-temporal wavelet theory which is applied to the section of a solution in the plane y = 0.

AB - We present here an exact integral representation of solutions of the wave equation with constant coefficients in two spatial dimensions in terms of localized solutions. A solution is given as a superposition of localized solutions each of which lives in the reference system, which moves in the x direction with velocity v. To obtain any solution, we must take into account all |v| ≤ c, where c is the velocity of wave propagation, and use also shifts and scaling. The representation is constructed by means of space-temporal wavelet theory which is applied to the section of a solution in the plane y = 0.

UR - https://ieeexplore.ieee.org/document/5562609/authors#authors

M3 - Conference contribution

SN - 9781424448746

SP - 159

EP - 161

BT - Proceedings of the International Conference Days on Diffraction 2009

PB - Institute of Electrical and Electronics Engineers Inc.

T2 - 2009 International Conference Days on Diffraction, DD 2009

Y2 - 26 May 2009 through 29 May 2009

ER -

ID: 4467240