Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant
Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment,...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Cadoret, M. [verfasserIn] de Mirandes, E. [verfasserIn] Cladé, P. [verfasserIn] Guellati-Khélifa, S. [verfasserIn] Schwob, C. [verfasserIn] Nez, F. [verfasserIn] Julien, L. [verfasserIn] Biraben, F. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2008 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: European physical journal special topics - Berlin : Springer, 2007, 163(2008), 1 vom: Okt., Seite 101-111 |
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| Übergeordnetes Werk: |
volume:163 ; year:2008 ; number:1 ; month:10 ; pages:101-111 |
| Links: |
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| DOI / URN: |
10.1140/epjst/e2008-00813-9 |
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| Katalog-ID: |
SPR02204969X |
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| 245 | 1 | 0 | |a Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant |
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| 520 | |a Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. | ||
| 650 | 4 | |a European Physical Journal Special Topic |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Relative Uncertainty |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Structure Constant |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Raman Transition |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Level Shift |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a de Mirandes, E. |e verfasserin |4 aut | |
| 700 | 1 | |a Cladé, P. |e verfasserin |4 aut | |
| 700 | 1 | |a Guellati-Khélifa, S. |e verfasserin |4 aut | |
| 700 | 1 | |a Schwob, C. |e verfasserin |4 aut | |
| 700 | 1 | |a Nez, F. |e verfasserin |4 aut | |
| 700 | 1 | |a Julien, L. |e verfasserin |4 aut | |
| 700 | 1 | |a Biraben, F. |e verfasserin |4 aut | |
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10.1140/epjst/e2008-00813-9 doi (DE-627)SPR02204969X (SPR)e2008-00813-9-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Cadoret, M. verfasserin aut Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. European Physical Journal Special Topic (dpeaa)DE-He213 Relative Uncertainty (dpeaa)DE-He213 Structure Constant (dpeaa)DE-He213 Raman Transition (dpeaa)DE-He213 Level Shift (dpeaa)DE-He213 de Mirandes, E. verfasserin aut Cladé, P. verfasserin aut Guellati-Khélifa, S. verfasserin aut Schwob, C. verfasserin aut Nez, F. verfasserin aut Julien, L. verfasserin aut Biraben, F. verfasserin aut Enthalten in European physical journal special topics Berlin : Springer, 2007 163(2008), 1 vom: Okt., Seite 101-111 (DE-627)523571909 (DE-600)2267176-6 1951-6401 nnns volume:163 year:2008 number:1 month:10 pages:101-111 https://dx.doi.org/10.1140/epjst/e2008-00813-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_65 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 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_2018 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_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 31.00 ASE 33.00 ASE AR 163 2008 1 10 101-111 |
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10.1140/epjst/e2008-00813-9 doi (DE-627)SPR02204969X (SPR)e2008-00813-9-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Cadoret, M. verfasserin aut Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. European Physical Journal Special Topic (dpeaa)DE-He213 Relative Uncertainty (dpeaa)DE-He213 Structure Constant (dpeaa)DE-He213 Raman Transition (dpeaa)DE-He213 Level Shift (dpeaa)DE-He213 de Mirandes, E. verfasserin aut Cladé, P. verfasserin aut Guellati-Khélifa, S. verfasserin aut Schwob, C. verfasserin aut Nez, F. verfasserin aut Julien, L. verfasserin aut Biraben, F. verfasserin aut Enthalten in European physical journal special topics Berlin : Springer, 2007 163(2008), 1 vom: Okt., Seite 101-111 (DE-627)523571909 (DE-600)2267176-6 1951-6401 nnns volume:163 year:2008 number:1 month:10 pages:101-111 https://dx.doi.org/10.1140/epjst/e2008-00813-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_65 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 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_2018 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_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 31.00 ASE 33.00 ASE AR 163 2008 1 10 101-111 |
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10.1140/epjst/e2008-00813-9 doi (DE-627)SPR02204969X (SPR)e2008-00813-9-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Cadoret, M. verfasserin aut Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. European Physical Journal Special Topic (dpeaa)DE-He213 Relative Uncertainty (dpeaa)DE-He213 Structure Constant (dpeaa)DE-He213 Raman Transition (dpeaa)DE-He213 Level Shift (dpeaa)DE-He213 de Mirandes, E. verfasserin aut Cladé, P. verfasserin aut Guellati-Khélifa, S. verfasserin aut Schwob, C. verfasserin aut Nez, F. verfasserin aut Julien, L. verfasserin aut Biraben, F. verfasserin aut Enthalten in European physical journal special topics Berlin : Springer, 2007 163(2008), 1 vom: Okt., Seite 101-111 (DE-627)523571909 (DE-600)2267176-6 1951-6401 nnns volume:163 year:2008 number:1 month:10 pages:101-111 https://dx.doi.org/10.1140/epjst/e2008-00813-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_65 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 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_2018 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_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 31.00 ASE 33.00 ASE AR 163 2008 1 10 101-111 |
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10.1140/epjst/e2008-00813-9 doi (DE-627)SPR02204969X (SPR)e2008-00813-9-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Cadoret, M. verfasserin aut Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. European Physical Journal Special Topic (dpeaa)DE-He213 Relative Uncertainty (dpeaa)DE-He213 Structure Constant (dpeaa)DE-He213 Raman Transition (dpeaa)DE-He213 Level Shift (dpeaa)DE-He213 de Mirandes, E. verfasserin aut Cladé, P. verfasserin aut Guellati-Khélifa, S. verfasserin aut Schwob, C. verfasserin aut Nez, F. verfasserin aut Julien, L. verfasserin aut Biraben, F. verfasserin aut Enthalten in European physical journal special topics Berlin : Springer, 2007 163(2008), 1 vom: Okt., Seite 101-111 (DE-627)523571909 (DE-600)2267176-6 1951-6401 nnns volume:163 year:2008 number:1 month:10 pages:101-111 https://dx.doi.org/10.1140/epjst/e2008-00813-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_65 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 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_2018 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_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 31.00 ASE 33.00 ASE AR 163 2008 1 10 101-111 |
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10.1140/epjst/e2008-00813-9 doi (DE-627)SPR02204969X (SPR)e2008-00813-9-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Cadoret, M. verfasserin aut Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant 2008 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. European Physical Journal Special Topic (dpeaa)DE-He213 Relative Uncertainty (dpeaa)DE-He213 Structure Constant (dpeaa)DE-He213 Raman Transition (dpeaa)DE-He213 Level Shift (dpeaa)DE-He213 de Mirandes, E. verfasserin aut Cladé, P. verfasserin aut Guellati-Khélifa, S. verfasserin aut Schwob, C. verfasserin aut Nez, F. verfasserin aut Julien, L. verfasserin aut Biraben, F. verfasserin aut Enthalten in European physical journal special topics Berlin : Springer, 2007 163(2008), 1 vom: Okt., Seite 101-111 (DE-627)523571909 (DE-600)2267176-6 1951-6401 nnns volume:163 year:2008 number:1 month:10 pages:101-111 https://dx.doi.org/10.1140/epjst/e2008-00813-9 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_65 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 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_2018 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_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 31.00 ASE 33.00 ASE AR 163 2008 1 10 101-111 |
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Cadoret, M. @@aut@@ de Mirandes, E. @@aut@@ Cladé, P. @@aut@@ Guellati-Khélifa, S. @@aut@@ Schwob, C. @@aut@@ Nez, F. @@aut@@ Julien, L. @@aut@@ Biraben, F. @@aut@@ |
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Cadoret, M. |
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Cadoret, M. ddc 530 bkl 31.00 bkl 33.00 misc European Physical Journal Special Topic misc Relative Uncertainty misc Structure Constant misc Raman Transition misc Level Shift Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant |
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530 ASE 31.00 bkl 33.00 bkl Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant European Physical Journal Special Topic (dpeaa)DE-He213 Relative Uncertainty (dpeaa)DE-He213 Structure Constant (dpeaa)DE-He213 Raman Transition (dpeaa)DE-He213 Level Shift (dpeaa)DE-He213 |
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Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant |
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Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant |
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Cadoret, M. de Mirandes, E. Cladé, P. Guellati-Khélifa, S. Schwob, C. Nez, F. Julien, L. Biraben, F. |
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precise determination of h/$ m_{rb} $ using bloch oscillations and atomic interferometry: a mean to deduce the fine structure constant |
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Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant |
| abstract |
Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. |
| abstractGer |
Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. |
| abstract_unstemmed |
Abstract We use Bloch oscillations to transfer coherently many photon momenta to atoms. Then we can measure accurately the ratio h/$ m_{Rb} $ and deduce the fine structure constant α. The velocity variation due to the Bloch oscillations is measured thanks to Raman transitions. In a first experiment, two Raman π pulses are used to select and measure a very narrow velocity class. This method yields to a value of the fine structure constant $ α^{-1} $= 137.03599884(91) with a relative uncertainty of about 6.6 ppb. More recently we use an atomic interferometer consisting in two pairs of π/2 pulses. We present here the first results obtained with this method. |
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Precise determination of h/$ m_{Rb} $ using Bloch oscillations and atomic interferometry: A mean to deduce the fine structure constant |
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https://dx.doi.org/10.1140/epjst/e2008-00813-9 |
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de Mirandes, E. Cladé, P. Guellati-Khélifa, S. Schwob, C. Nez, F. Julien, L. Biraben, F. |
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de Mirandes, E. Cladé, P. Guellati-Khélifa, S. Schwob, C. Nez, F. Julien, L. Biraben, F. |
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|
| score |
7.401971 |