Dynamical Casimir Effect and Collective Excitation Effect at Finite Temperature Without the Rotating-Wave Approximation
Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created...
Ausführliche Beschreibung
Autor*in: |
Asilibieke, Bahetiguli [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
2015 |
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Schlagwörter: |
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Anmerkung: |
© Springer Science+Business Media New York 2015 |
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Übergeordnetes Werk: |
Enthalten in: International journal of theoretical physics - Springer US, 1968, 54(2015), 8 vom: 22. Jan., Seite 2762-2770 |
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Übergeordnetes Werk: |
volume:54 ; year:2015 ; number:8 ; day:22 ; month:01 ; pages:2762-2770 |
Links: |
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DOI / URN: |
10.1007/s10773-015-2513-6 |
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Katalog-ID: |
OLC2052393080 |
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520 | |a Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. | ||
650 | 4 | |a Dynamical Casimir effect | |
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10.1007/s10773-015-2513-6 doi (DE-627)OLC2052393080 (DE-He213)s10773-015-2513-6-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Asilibieke, Bahetiguli verfasserin aut Dynamical Casimir Effect and Collective Excitation Effect at Finite Temperature Without the Rotating-Wave Approximation 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. Dynamical Casimir effect Collective excitation effect Counter-rotating wave approximation At finite temperature Xue, Zhang aut Jie, Fang aut Hui, Liu aut Mei, Pan Shu aut Yu, Zheng Tai aut Hui, Yang aut Enthalten in International journal of theoretical physics Springer US, 1968 54(2015), 8 vom: 22. Jan., Seite 2762-2770 (DE-627)129546097 (DE-600)218277-4 (DE-576)014996413 0020-7748 nnns volume:54 year:2015 number:8 day:22 month:01 pages:2762-2770 https://doi.org/10.1007/s10773-015-2513-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2005 33.00 VZ AR 54 2015 8 22 01 2762-2770 |
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10.1007/s10773-015-2513-6 doi (DE-627)OLC2052393080 (DE-He213)s10773-015-2513-6-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Asilibieke, Bahetiguli verfasserin aut Dynamical Casimir Effect and Collective Excitation Effect at Finite Temperature Without the Rotating-Wave Approximation 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. Dynamical Casimir effect Collective excitation effect Counter-rotating wave approximation At finite temperature Xue, Zhang aut Jie, Fang aut Hui, Liu aut Mei, Pan Shu aut Yu, Zheng Tai aut Hui, Yang aut Enthalten in International journal of theoretical physics Springer US, 1968 54(2015), 8 vom: 22. Jan., Seite 2762-2770 (DE-627)129546097 (DE-600)218277-4 (DE-576)014996413 0020-7748 nnns volume:54 year:2015 number:8 day:22 month:01 pages:2762-2770 https://doi.org/10.1007/s10773-015-2513-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2005 33.00 VZ AR 54 2015 8 22 01 2762-2770 |
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10.1007/s10773-015-2513-6 doi (DE-627)OLC2052393080 (DE-He213)s10773-015-2513-6-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Asilibieke, Bahetiguli verfasserin aut Dynamical Casimir Effect and Collective Excitation Effect at Finite Temperature Without the Rotating-Wave Approximation 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. Dynamical Casimir effect Collective excitation effect Counter-rotating wave approximation At finite temperature Xue, Zhang aut Jie, Fang aut Hui, Liu aut Mei, Pan Shu aut Yu, Zheng Tai aut Hui, Yang aut Enthalten in International journal of theoretical physics Springer US, 1968 54(2015), 8 vom: 22. Jan., Seite 2762-2770 (DE-627)129546097 (DE-600)218277-4 (DE-576)014996413 0020-7748 nnns volume:54 year:2015 number:8 day:22 month:01 pages:2762-2770 https://doi.org/10.1007/s10773-015-2513-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2005 33.00 VZ AR 54 2015 8 22 01 2762-2770 |
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10.1007/s10773-015-2513-6 doi (DE-627)OLC2052393080 (DE-He213)s10773-015-2513-6-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Asilibieke, Bahetiguli verfasserin aut Dynamical Casimir Effect and Collective Excitation Effect at Finite Temperature Without the Rotating-Wave Approximation 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. Dynamical Casimir effect Collective excitation effect Counter-rotating wave approximation At finite temperature Xue, Zhang aut Jie, Fang aut Hui, Liu aut Mei, Pan Shu aut Yu, Zheng Tai aut Hui, Yang aut Enthalten in International journal of theoretical physics Springer US, 1968 54(2015), 8 vom: 22. Jan., Seite 2762-2770 (DE-627)129546097 (DE-600)218277-4 (DE-576)014996413 0020-7748 nnns volume:54 year:2015 number:8 day:22 month:01 pages:2762-2770 https://doi.org/10.1007/s10773-015-2513-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2005 33.00 VZ AR 54 2015 8 22 01 2762-2770 |
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10.1007/s10773-015-2513-6 doi (DE-627)OLC2052393080 (DE-He213)s10773-015-2513-6-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Asilibieke, Bahetiguli verfasserin aut Dynamical Casimir Effect and Collective Excitation Effect at Finite Temperature Without the Rotating-Wave Approximation 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2015 Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. Dynamical Casimir effect Collective excitation effect Counter-rotating wave approximation At finite temperature Xue, Zhang aut Jie, Fang aut Hui, Liu aut Mei, Pan Shu aut Yu, Zheng Tai aut Hui, Yang aut Enthalten in International journal of theoretical physics Springer US, 1968 54(2015), 8 vom: 22. Jan., Seite 2762-2770 (DE-627)129546097 (DE-600)218277-4 (DE-576)014996413 0020-7748 nnns volume:54 year:2015 number:8 day:22 month:01 pages:2762-2770 https://doi.org/10.1007/s10773-015-2513-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2005 33.00 VZ AR 54 2015 8 22 01 2762-2770 |
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Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. © Springer Science+Business Media New York 2015 |
abstractGer |
Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. © Springer Science+Business Media New York 2015 |
abstract_unstemmed |
Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature. © Springer Science+Business Media New York 2015 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2052393080</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503084808.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s2015 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10773-015-2513-6</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2052393080</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s10773-015-2513-6-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Asilibieke, Bahetiguli</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Dynamical Casimir Effect and Collective Excitation Effect at Finite Temperature Without the Rotating-Wave Approximation</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2015</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Springer Science+Business Media New York 2015</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The dynamical Casimir effect and the collective excitation effect are investigated in a resonantly vibrating cavity filled with a gas of two-level atoms without the rotating-wave approximation at finite temperature. Compared with the condition of the rotating-wave approximation, the created photons and the created excitons are more under the non-rotating wave approximation at different temperatures and different total coupling strengths. The numerical results show that the counter-rotating wave terms enhance the dynamical Casimir effect and the collective excitation effect at finite temperature.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Dynamical Casimir effect</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Collective excitation effect</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Counter-rotating wave approximation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">At finite temperature</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Xue, Zhang</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jie, Fang</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Hui, Liu</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Mei, Pan Shu</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Yu, Zheng Tai</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Hui, Yang</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">International journal of theoretical physics</subfield><subfield code="d">Springer US, 1968</subfield><subfield code="g">54(2015), 8 vom: 22. 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