Experimental implementation of a four-level N-type scheme for the observation of electromagnetically induced transparency
Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated a...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Éntin, V. M. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2000 |
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| Anmerkung: |
© MAIK "Nauka/Interperiodica" 2000 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of experimental and theoretical physics / JETP letters - Nauka/Interperiodica, 1993, 71(2000), 5 vom: März, Seite 175-177 |
|---|---|
| Übergeordnetes Werk: |
volume:71 ; year:2000 ; number:5 ; month:03 ; pages:175-177 |
| Links: |
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| DOI / URN: |
10.1134/1.568308 |
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OLC2085741665 |
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| 520 | |a Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. | ||
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10.1134/1.568308 doi (DE-627)OLC2085741665 (DE-He213)1.568308-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Éntin, V. M. verfasserin aut Experimental implementation of a four-level N-type scheme for the observation of electromagnetically induced transparency 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2000 Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. Ryabtsev, I. I. aut Boguslavskii, A. E. aut Beterov, I. M. aut Enthalten in Journal of experimental and theoretical physics / JETP letters Nauka/Interperiodica, 1993 71(2000), 5 vom: März, Seite 175-177 (DE-627)182384713 (DE-600)917787-5 (DE-576)053745841 0021-3640 nnns volume:71 year:2000 number:5 month:03 pages:175-177 https://doi.org/10.1134/1.568308 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 71 2000 5 03 175-177 |
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10.1134/1.568308 doi (DE-627)OLC2085741665 (DE-He213)1.568308-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Éntin, V. M. verfasserin aut Experimental implementation of a four-level N-type scheme for the observation of electromagnetically induced transparency 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2000 Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. Ryabtsev, I. I. aut Boguslavskii, A. E. aut Beterov, I. M. aut Enthalten in Journal of experimental and theoretical physics / JETP letters Nauka/Interperiodica, 1993 71(2000), 5 vom: März, Seite 175-177 (DE-627)182384713 (DE-600)917787-5 (DE-576)053745841 0021-3640 nnns volume:71 year:2000 number:5 month:03 pages:175-177 https://doi.org/10.1134/1.568308 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 71 2000 5 03 175-177 |
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10.1134/1.568308 doi (DE-627)OLC2085741665 (DE-He213)1.568308-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Éntin, V. M. verfasserin aut Experimental implementation of a four-level N-type scheme for the observation of electromagnetically induced transparency 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2000 Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. Ryabtsev, I. I. aut Boguslavskii, A. E. aut Beterov, I. M. aut Enthalten in Journal of experimental and theoretical physics / JETP letters Nauka/Interperiodica, 1993 71(2000), 5 vom: März, Seite 175-177 (DE-627)182384713 (DE-600)917787-5 (DE-576)053745841 0021-3640 nnns volume:71 year:2000 number:5 month:03 pages:175-177 https://doi.org/10.1134/1.568308 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 71 2000 5 03 175-177 |
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10.1134/1.568308 doi (DE-627)OLC2085741665 (DE-He213)1.568308-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Éntin, V. M. verfasserin aut Experimental implementation of a four-level N-type scheme for the observation of electromagnetically induced transparency 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2000 Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. Ryabtsev, I. I. aut Boguslavskii, A. E. aut Beterov, I. M. aut Enthalten in Journal of experimental and theoretical physics / JETP letters Nauka/Interperiodica, 1993 71(2000), 5 vom: März, Seite 175-177 (DE-627)182384713 (DE-600)917787-5 (DE-576)053745841 0021-3640 nnns volume:71 year:2000 number:5 month:03 pages:175-177 https://doi.org/10.1134/1.568308 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 71 2000 5 03 175-177 |
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10.1134/1.568308 doi (DE-627)OLC2085741665 (DE-He213)1.568308-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Éntin, V. M. verfasserin aut Experimental implementation of a four-level N-type scheme for the observation of electromagnetically induced transparency 2000 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2000 Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. Ryabtsev, I. I. aut Boguslavskii, A. E. aut Beterov, I. M. aut Enthalten in Journal of experimental and theoretical physics / JETP letters Nauka/Interperiodica, 1993 71(2000), 5 vom: März, Seite 175-177 (DE-627)182384713 (DE-600)917787-5 (DE-576)053745841 0021-3640 nnns volume:71 year:2000 number:5 month:03 pages:175-177 https://doi.org/10.1134/1.568308 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 71 2000 5 03 175-177 |
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Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. © MAIK "Nauka/Interperiodica" 2000 |
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Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. © MAIK "Nauka/Interperiodica" 2000 |
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Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field. © MAIK "Nauka/Interperiodica" 2000 |
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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">OLC2085741665</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230504104335.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">230302s2000 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1134/1.568308</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2085741665</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)1.568308-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">Éntin, V. M.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Experimental implementation of a four-level N-type scheme for the observation of electromagnetically induced transparency</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2000</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">© MAIK "Nauka/Interperiodica" 2000</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract A nondegenerate four-level N-type scheme was experimentally implemented to observe electromagnetically induced transparency (EIT) at the 87Rb D2 line. Radiations of two independent external-cavity semiconductor lasers were used in the experiment, the current of one of them being modulated at a frequency equal to the hyperfine-splitting frequency of the excited 5P3/2 level. In this case, apart from the main EIT dip corresponding to the two-photon Raman resonance in a three-level L-scheme, additional dips detuned from the main dip by a frequency equal to the frequency of the HF generator were observed in the absorption spectrum. These dips were due to an increase in the medium transparency at frequencies corresponding to the three-photon Raman resonances in four-level N-type schemes. The resonance shapes are analyzed as functions of generator frequency and magnetic field.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ryabtsev, I. I.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Boguslavskii, A. 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M.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of experimental and theoretical physics / JETP letters</subfield><subfield code="d">Nauka/Interperiodica, 1993</subfield><subfield code="g">71(2000), 5 vom: März, Seite 175-177</subfield><subfield code="w">(DE-627)182384713</subfield><subfield code="w">(DE-600)917787-5</subfield><subfield code="w">(DE-576)053745841</subfield><subfield code="x">0021-3640</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:71</subfield><subfield code="g">year:2000</subfield><subfield code="g">number:5</subfield><subfield code="g">month:03</subfield><subfield code="g">pages:175-177</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/1.568308</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.00</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">71</subfield><subfield code="j">2000</subfield><subfield code="e">5</subfield><subfield code="c">03</subfield><subfield code="h">175-177</subfield></datafield></record></collection>
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