Modulation-free pump-probe spectroscopy of strontium atoms
Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type linesh...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Javaux, C. [verfasserIn] Hughes, I.G [verfasserIn] Lochead, G. [verfasserIn] Millen, J. [verfasserIn] Jones, M. P.A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2010 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: The European physical journal - Berlin : Springer, 1998, 57(2010), 2 vom: 16. Feb., Seite 151-154 |
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| Übergeordnetes Werk: |
volume:57 ; year:2010 ; number:2 ; day:16 ; month:02 ; pages:151-154 |
| Links: |
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| DOI / URN: |
10.1140/epjd/e2010-00029-4 |
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| Katalog-ID: |
SPR008404593 |
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| 520 | |a Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. | ||
| 650 | 4 | |a Probe Beam |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Pump Beam |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Polarize Beam Splitter |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Magnetic Sublevel |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Polarization Spectroscopy |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Hughes, I.G |e verfasserin |4 aut | |
| 700 | 1 | |a Lochead, G. |e verfasserin |4 aut | |
| 700 | 1 | |a Millen, J. |e verfasserin |4 aut | |
| 700 | 1 | |a Jones, M. P.A. |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t The European physical journal |d Berlin : Springer, 1998 |g 57(2010), 2 vom: 16. Feb., Seite 151-154 |w (DE-627)253722950 |w (DE-600)1459071-2 |x 1434-6079 |7 nnns |
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10.1140/epjd/e2010-00029-4 doi (DE-627)SPR008404593 (SPR)e2010-00029-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Javaux, C. verfasserin aut Modulation-free pump-probe spectroscopy of strontium atoms 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. Probe Beam (dpeaa)DE-He213 Pump Beam (dpeaa)DE-He213 Polarize Beam Splitter (dpeaa)DE-He213 Magnetic Sublevel (dpeaa)DE-He213 Polarization Spectroscopy (dpeaa)DE-He213 Hughes, I.G verfasserin aut Lochead, G. verfasserin aut Millen, J. verfasserin aut Jones, M. P.A. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2010), 2 vom: 16. Feb., Seite 151-154 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:57 year:2010 number:2 day:16 month:02 pages:151-154 https://dx.doi.org/10.1140/epjd/e2010-00029-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 57 2010 2 16 02 151-154 |
| spelling |
10.1140/epjd/e2010-00029-4 doi (DE-627)SPR008404593 (SPR)e2010-00029-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Javaux, C. verfasserin aut Modulation-free pump-probe spectroscopy of strontium atoms 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. Probe Beam (dpeaa)DE-He213 Pump Beam (dpeaa)DE-He213 Polarize Beam Splitter (dpeaa)DE-He213 Magnetic Sublevel (dpeaa)DE-He213 Polarization Spectroscopy (dpeaa)DE-He213 Hughes, I.G verfasserin aut Lochead, G. verfasserin aut Millen, J. verfasserin aut Jones, M. P.A. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2010), 2 vom: 16. Feb., Seite 151-154 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:57 year:2010 number:2 day:16 month:02 pages:151-154 https://dx.doi.org/10.1140/epjd/e2010-00029-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 57 2010 2 16 02 151-154 |
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10.1140/epjd/e2010-00029-4 doi (DE-627)SPR008404593 (SPR)e2010-00029-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Javaux, C. verfasserin aut Modulation-free pump-probe spectroscopy of strontium atoms 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. Probe Beam (dpeaa)DE-He213 Pump Beam (dpeaa)DE-He213 Polarize Beam Splitter (dpeaa)DE-He213 Magnetic Sublevel (dpeaa)DE-He213 Polarization Spectroscopy (dpeaa)DE-He213 Hughes, I.G verfasserin aut Lochead, G. verfasserin aut Millen, J. verfasserin aut Jones, M. P.A. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2010), 2 vom: 16. Feb., Seite 151-154 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:57 year:2010 number:2 day:16 month:02 pages:151-154 https://dx.doi.org/10.1140/epjd/e2010-00029-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 57 2010 2 16 02 151-154 |
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10.1140/epjd/e2010-00029-4 doi (DE-627)SPR008404593 (SPR)e2010-00029-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Javaux, C. verfasserin aut Modulation-free pump-probe spectroscopy of strontium atoms 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. Probe Beam (dpeaa)DE-He213 Pump Beam (dpeaa)DE-He213 Polarize Beam Splitter (dpeaa)DE-He213 Magnetic Sublevel (dpeaa)DE-He213 Polarization Spectroscopy (dpeaa)DE-He213 Hughes, I.G verfasserin aut Lochead, G. verfasserin aut Millen, J. verfasserin aut Jones, M. P.A. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2010), 2 vom: 16. Feb., Seite 151-154 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:57 year:2010 number:2 day:16 month:02 pages:151-154 https://dx.doi.org/10.1140/epjd/e2010-00029-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 57 2010 2 16 02 151-154 |
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10.1140/epjd/e2010-00029-4 doi (DE-627)SPR008404593 (SPR)e2010-00029-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Javaux, C. verfasserin aut Modulation-free pump-probe spectroscopy of strontium atoms 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. Probe Beam (dpeaa)DE-He213 Pump Beam (dpeaa)DE-He213 Polarize Beam Splitter (dpeaa)DE-He213 Magnetic Sublevel (dpeaa)DE-He213 Polarization Spectroscopy (dpeaa)DE-He213 Hughes, I.G verfasserin aut Lochead, G. verfasserin aut Millen, J. verfasserin aut Jones, M. P.A. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 57(2010), 2 vom: 16. Feb., Seite 151-154 (DE-627)253722950 (DE-600)1459071-2 1434-6079 nnns volume:57 year:2010 number:2 day:16 month:02 pages:151-154 https://dx.doi.org/10.1140/epjd/e2010-00029-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.30 ASE 33.38 ASE 33.80 ASE AR 57 2010 2 16 02 151-154 |
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Enthalten in The European physical journal 57(2010), 2 vom: 16. Feb., Seite 151-154 volume:57 year:2010 number:2 day:16 month:02 pages:151-154 |
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Probe Beam Pump Beam Polarize Beam Splitter Magnetic Sublevel Polarization Spectroscopy |
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Javaux, C. @@aut@@ Hughes, I.G @@aut@@ Lochead, G. @@aut@@ Millen, J. @@aut@@ Jones, M. P.A. @@aut@@ |
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Javaux, C. |
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Javaux, C. ddc 530 bkl 33.30 bkl 33.38 bkl 33.80 misc Probe Beam misc Pump Beam misc Polarize Beam Splitter misc Magnetic Sublevel misc Polarization Spectroscopy Modulation-free pump-probe spectroscopy of strontium atoms |
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530 ASE 33.30 bkl 33.38 bkl 33.80 bkl Modulation-free pump-probe spectroscopy of strontium atoms Probe Beam (dpeaa)DE-He213 Pump Beam (dpeaa)DE-He213 Polarize Beam Splitter (dpeaa)DE-He213 Magnetic Sublevel (dpeaa)DE-He213 Polarization Spectroscopy (dpeaa)DE-He213 |
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ddc 530 bkl 33.30 bkl 33.38 bkl 33.80 misc Probe Beam misc Pump Beam misc Polarize Beam Splitter misc Magnetic Sublevel misc Polarization Spectroscopy |
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ddc 530 bkl 33.30 bkl 33.38 bkl 33.80 misc Probe Beam misc Pump Beam misc Polarize Beam Splitter misc Magnetic Sublevel misc Polarization Spectroscopy |
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ddc 530 bkl 33.30 bkl 33.38 bkl 33.80 misc Probe Beam misc Pump Beam misc Polarize Beam Splitter misc Magnetic Sublevel misc Polarization Spectroscopy |
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Modulation-free pump-probe spectroscopy of strontium atoms |
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Modulation-free pump-probe spectroscopy of strontium atoms |
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Javaux, C. Hughes, I.G Lochead, G. Millen, J. Jones, M. P.A. |
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modulation-free pump-probe spectroscopy of strontium atoms |
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Modulation-free pump-probe spectroscopy of strontium atoms |
| abstract |
Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. |
| abstractGer |
Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. |
| abstract_unstemmed |
Abstract We have performed polarization spectroscopy on the $ 5s^{2} $1$ S_{0} $ →$ 5s5p^{1} %$ P_{1} $ transition of atomic strontium. The signal is generated by saturation effects, rather than optical pumping, as the ground state is non-degenerate. This technique generated a dispersion-type lineshape suitable for laser stabilization, without the need for frequency modulation. The dependence of the amplitude and gradient on intensity and magnetic field were also investigated, and compared to a related technique based on the circular dichroism induced by a magnetic field. |
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| title_short |
Modulation-free pump-probe spectroscopy of strontium atoms |
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https://dx.doi.org/10.1140/epjd/e2010-00029-4 |
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| author2 |
Hughes, I.G Lochead, G. Millen, J. Jones, M. P.A. |
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Hughes, I.G Lochead, G. Millen, J. Jones, M. P.A. |
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| doi_str |
10.1140/epjd/e2010-00029-4 |
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2024-07-03T20:48:21.964Z |
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|
| score |
7.4012003 |