Lasing without inversion due to cooling subsystem
Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the cohe...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Shakhmuratov, R.N. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1997 |
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| Schlagwörter: |
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| Anmerkung: |
© Kluwer Academic Publishers 1997 |
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| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 107(1997), 1-4 vom: Mai, Seite 205-211 |
|---|---|
| Übergeordnetes Werk: |
volume:107 ; year:1997 ; number:1-4 ; month:05 ; pages:205-211 |
| Links: |
|---|
| DOI / URN: |
10.1023/A:1012059806933 |
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OLC2076388281 |
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| 520 | |a Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. | ||
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10.1023/A:1012059806933 doi (DE-627)OLC2076388281 (DE-He213)A:1012059806933-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Shakhmuratov, R.N. verfasserin aut Lasing without inversion due to cooling subsystem 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. Reservoir Temperature Coherent Light Driving Field Giant Pulse Infinite Temperature Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 107(1997), 1-4 vom: Mai, Seite 205-211 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:107 year:1997 number:1-4 month:05 pages:205-211 https://doi.org/10.1023/A:1012059806933 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 107 1997 1-4 05 205-211 |
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10.1023/A:1012059806933 doi (DE-627)OLC2076388281 (DE-He213)A:1012059806933-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Shakhmuratov, R.N. verfasserin aut Lasing without inversion due to cooling subsystem 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. Reservoir Temperature Coherent Light Driving Field Giant Pulse Infinite Temperature Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 107(1997), 1-4 vom: Mai, Seite 205-211 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:107 year:1997 number:1-4 month:05 pages:205-211 https://doi.org/10.1023/A:1012059806933 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 107 1997 1-4 05 205-211 |
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10.1023/A:1012059806933 doi (DE-627)OLC2076388281 (DE-He213)A:1012059806933-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Shakhmuratov, R.N. verfasserin aut Lasing without inversion due to cooling subsystem 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. Reservoir Temperature Coherent Light Driving Field Giant Pulse Infinite Temperature Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 107(1997), 1-4 vom: Mai, Seite 205-211 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:107 year:1997 number:1-4 month:05 pages:205-211 https://doi.org/10.1023/A:1012059806933 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 107 1997 1-4 05 205-211 |
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10.1023/A:1012059806933 doi (DE-627)OLC2076388281 (DE-He213)A:1012059806933-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Shakhmuratov, R.N. verfasserin aut Lasing without inversion due to cooling subsystem 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. Reservoir Temperature Coherent Light Driving Field Giant Pulse Infinite Temperature Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 107(1997), 1-4 vom: Mai, Seite 205-211 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:107 year:1997 number:1-4 month:05 pages:205-211 https://doi.org/10.1023/A:1012059806933 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 107 1997 1-4 05 205-211 |
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10.1023/A:1012059806933 doi (DE-627)OLC2076388281 (DE-He213)A:1012059806933-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Shakhmuratov, R.N. verfasserin aut Lasing without inversion due to cooling subsystem 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. Reservoir Temperature Coherent Light Driving Field Giant Pulse Infinite Temperature Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 107(1997), 1-4 vom: Mai, Seite 205-211 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:107 year:1997 number:1-4 month:05 pages:205-211 https://doi.org/10.1023/A:1012059806933 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 107 1997 1-4 05 205-211 |
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Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. © Kluwer Academic Publishers 1997 |
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Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. © Kluwer Academic Publishers 1997 |
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Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. It is shown that lasing conditions strongly differ from conventional ones. © Kluwer Academic Publishers 1997 |
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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">OLC2076388281</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503073813.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s1997 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1023/A:1012059806933</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2076388281</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)A:1012059806933-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">Shakhmuratov, R.N.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Lasing without inversion due to cooling subsystem</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1997</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">© Kluwer Academic Publishers 1997</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The new possibility of inversionless lasing is discussed. We have considered the resonant interaction of a two-level system (TLS) with photons and the adiabatic interaction with an ensemble of Bose particles. It is found out that a TLS with equally populated energy levels amplifies the coherent light with Stokes-shifted frequency. This becomes possible as photon emission is accompanied by Bose particles excitation. The energy flow from the TLS to the photon subsystem is realized due to the Bose subsystem being at finite temperature and playing the cooler role. The advantage of this new lasing principle is discussed. 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