Standard

Spin-wave dark soliton pairs in magnetic thin films. / Wang, Z.; Cherkasskii, M.; Kalinikos, B.; Wu, M.

2015 IEEE International Magnetics Conference, INTERMAG 2015. Institute of Electrical and Electronics Engineers Inc., 2015. 7157009 (2015 IEEE International Magnetics Conference, INTERMAG 2015).

Результаты исследований: Публикации в книгах, отчётах, сборниках, трудах конференцийстатья в сборнике материалов конференциинаучнаяРецензирование

Harvard

Wang, Z, Cherkasskii, M, Kalinikos, B & Wu, M 2015, Spin-wave dark soliton pairs in magnetic thin films. в 2015 IEEE International Magnetics Conference, INTERMAG 2015., 7157009, 2015 IEEE International Magnetics Conference, INTERMAG 2015, Institute of Electrical and Electronics Engineers Inc., 2015 IEEE International Magnetics Conference, INTERMAG 2015, Beijing, Китай, 11/05/15. https://doi.org/10.1109/INTMAG.2015.7157009

APA

Wang, Z., Cherkasskii, M., Kalinikos, B., & Wu, M. (2015). Spin-wave dark soliton pairs in magnetic thin films. в 2015 IEEE International Magnetics Conference, INTERMAG 2015 [7157009] (2015 IEEE International Magnetics Conference, INTERMAG 2015). Institute of Electrical and Electronics Engineers Inc.. https://doi.org/10.1109/INTMAG.2015.7157009

Vancouver

Wang Z, Cherkasskii M, Kalinikos B, Wu M. Spin-wave dark soliton pairs in magnetic thin films. в 2015 IEEE International Magnetics Conference, INTERMAG 2015. Institute of Electrical and Electronics Engineers Inc. 2015. 7157009. (2015 IEEE International Magnetics Conference, INTERMAG 2015). https://doi.org/10.1109/INTMAG.2015.7157009

Author

Wang, Z. ; Cherkasskii, M. ; Kalinikos, B. ; Wu, M. / Spin-wave dark soliton pairs in magnetic thin films. 2015 IEEE International Magnetics Conference, INTERMAG 2015. Institute of Electrical and Electronics Engineers Inc., 2015. (2015 IEEE International Magnetics Conference, INTERMAG 2015).

BibTeX

@inproceedings{421497c53b5240df86262870441ce8ed,
title = "Spin-wave dark soliton pairs in magnetic thin films",
abstract = "One way to excite a dark envelope soliton is to use a dark input pulse - a narrow dip in the amplitude of a continuous wave background. This approach has been used previously to excite dark solitons for surface spin waves in yttrium iron garnet (YIG) thin film strips1 and for lasers in photorefractive crystals.2 Theoretically, however, an initial dark signal should not evolve into a single dark soliton, but a pair of dark solitons that have opposite phase jumps and an overall phase change of zero.3,4,5,6 Experimentally, such dark soliton pairs have been observed for solitons in various systems,7,8,9,10 but their phase signature has never been demonstrated so far.",
author = "Z. Wang and M. Cherkasskii and B. Kalinikos and M. Wu",
year = "2015",
month = jul,
day = "14",
doi = "10.1109/INTMAG.2015.7157009",
language = "English",
series = "2015 IEEE International Magnetics Conference, INTERMAG 2015",
publisher = "Institute of Electrical and Electronics Engineers Inc.",
booktitle = "2015 IEEE International Magnetics Conference, INTERMAG 2015",
address = "United States",
note = "2015 IEEE International Magnetics Conference, INTERMAG 2015 ; Conference date: 11-05-2015 Through 15-05-2015",

}

RIS

TY - GEN

T1 - Spin-wave dark soliton pairs in magnetic thin films

AU - Wang, Z.

AU - Cherkasskii, M.

AU - Kalinikos, B.

AU - Wu, M.

PY - 2015/7/14

Y1 - 2015/7/14

N2 - One way to excite a dark envelope soliton is to use a dark input pulse - a narrow dip in the amplitude of a continuous wave background. This approach has been used previously to excite dark solitons for surface spin waves in yttrium iron garnet (YIG) thin film strips1 and for lasers in photorefractive crystals.2 Theoretically, however, an initial dark signal should not evolve into a single dark soliton, but a pair of dark solitons that have opposite phase jumps and an overall phase change of zero.3,4,5,6 Experimentally, such dark soliton pairs have been observed for solitons in various systems,7,8,9,10 but their phase signature has never been demonstrated so far.

AB - One way to excite a dark envelope soliton is to use a dark input pulse - a narrow dip in the amplitude of a continuous wave background. This approach has been used previously to excite dark solitons for surface spin waves in yttrium iron garnet (YIG) thin film strips1 and for lasers in photorefractive crystals.2 Theoretically, however, an initial dark signal should not evolve into a single dark soliton, but a pair of dark solitons that have opposite phase jumps and an overall phase change of zero.3,4,5,6 Experimentally, such dark soliton pairs have been observed for solitons in various systems,7,8,9,10 but their phase signature has never been demonstrated so far.

UR - http://www.scopus.com/inward/record.url?scp=84942474613&partnerID=8YFLogxK

U2 - 10.1109/INTMAG.2015.7157009

DO - 10.1109/INTMAG.2015.7157009

M3 - Conference contribution

AN - SCOPUS:84942474613

T3 - 2015 IEEE International Magnetics Conference, INTERMAG 2015

BT - 2015 IEEE International Magnetics Conference, INTERMAG 2015

PB - Institute of Electrical and Electronics Engineers Inc.

T2 - 2015 IEEE International Magnetics Conference, INTERMAG 2015

Y2 - 11 May 2015 through 15 May 2015

ER -

ID: 51669533