Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter

Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 me...
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Autor*in:	Engels, R. [verfasserIn] Grigoryev, K. [verfasserIn] Mikirtytchyants, M. [verfasserIn] Paetz gen. Schieck, H. [verfasserIn] Rathmann, F. [verfasserIn] Schug, G. [verfasserIn] Ströher, H. [verfasserIn] Vasilyev, A. [verfasserIn] Westig, M. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2009

Schlagwörter:	Lamb shift Hyperfine Splitting Spinfilter

Übergeordnetes Werk:	Enthalten in: Hyperfine interactions - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975, 193(2009), 1-3 vom: 28. Aug.
Übergeordnetes Werk:	volume:193 ; year:2009 ; number:1-3 ; day:28 ; month:08

Links:	Volltext

DOI / URN:	10.1007/s10751-009-0021-x

Katalog-ID:	SPR013000756

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520			\|a Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested.
650		4	\|a Lamb shift \|7 (dpeaa)DE-He213
650		4	\|a Hyperfine Splitting \|7 (dpeaa)DE-He213
650		4	\|a Spinfilter \|7 (dpeaa)DE-He213
700	1		\|a Grigoryev, K. \|e verfasserin \|4 aut
700	1		\|a Mikirtytchyants, M. \|e verfasserin \|4 aut
700	1		\|a Paetz gen. Schieck, H. \|e verfasserin \|4 aut
700	1		\|a Rathmann, F. \|e verfasserin \|4 aut
700	1		\|a Schug, G. \|e verfasserin \|4 aut
700	1		\|a Ströher, H. \|e verfasserin \|4 aut
700	1		\|a Vasilyev, A. \|e verfasserin \|4 aut
700	1		\|a Westig, M. \|e verfasserin \|4 aut
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912			\|a GBV_ILN_31
912			\|a GBV_ILN_32
912			\|a GBV_ILN_39
912			\|a GBV_ILN_40
912			\|a GBV_ILN_60
912			\|a GBV_ILN_62
912			\|a GBV_ILN_63
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_206
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_266
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
912			\|a GBV_ILN_2111
912			\|a GBV_ILN_2112
912			\|a GBV_ILN_2113
912			\|a GBV_ILN_2116
912			\|a GBV_ILN_2118
912			\|a GBV_ILN_2122
912			\|a GBV_ILN_2143
912			\|a GBV_ILN_2144
912			\|a GBV_ILN_2147
912			\|a GBV_ILN_2148
912			\|a GBV_ILN_2152
912			\|a GBV_ILN_2153
912			\|a GBV_ILN_2188
912			\|a GBV_ILN_2232
912			\|a GBV_ILN_2336
912			\|a GBV_ILN_2446
912			\|a GBV_ILN_2470
912			\|a GBV_ILN_2507
912			\|a GBV_ILN_2522
912			\|a GBV_ILN_4012
912			\|a GBV_ILN_4035
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4046
912			\|a GBV_ILN_4242
912			\|a GBV_ILN_4246
912			\|a GBV_ILN_4249
912			\|a GBV_ILN_4251
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4326
912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4336
912			\|a GBV_ILN_4700
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Indexfelder

author_variant	r e re k g kg m m mm g s h p gsh gshp f r fr g s gs h s hs a v av m w mw
matchkey_str	article:15729540:2009----::rcsosetocpomtsalhdoeadniyrgnih
hierarchy_sort_str	2009
bklnumber	33.00
publishDate	2009
allfields	10.1007/s10751-009-0021-x doi (DE-627)SPR013000756 (SPR)s10751-009-0021-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Engels, R. verfasserin aut Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested. Lamb shift (dpeaa)DE-He213 Hyperfine Splitting (dpeaa)DE-He213 Spinfilter (dpeaa)DE-He213 Grigoryev, K. verfasserin aut Mikirtytchyants, M. verfasserin aut Paetz gen. Schieck, H. verfasserin aut Rathmann, F. verfasserin aut Schug, G. verfasserin aut Ströher, H. verfasserin aut Vasilyev, A. verfasserin aut Westig, M. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 193(2009), 1-3 vom: 28. Aug. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:193 year:2009 number:1-3 day:28 month:08 https://dx.doi.org/10.1007/s10751-009-0021-x 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_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2021 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 193 2009 1-3 28 08
spelling	10.1007/s10751-009-0021-x doi (DE-627)SPR013000756 (SPR)s10751-009-0021-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Engels, R. verfasserin aut Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested. Lamb shift (dpeaa)DE-He213 Hyperfine Splitting (dpeaa)DE-He213 Spinfilter (dpeaa)DE-He213 Grigoryev, K. verfasserin aut Mikirtytchyants, M. verfasserin aut Paetz gen. Schieck, H. verfasserin aut Rathmann, F. verfasserin aut Schug, G. verfasserin aut Ströher, H. verfasserin aut Vasilyev, A. verfasserin aut Westig, M. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 193(2009), 1-3 vom: 28. Aug. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:193 year:2009 number:1-3 day:28 month:08 https://dx.doi.org/10.1007/s10751-009-0021-x 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_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2021 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 193 2009 1-3 28 08
allfields_unstemmed	10.1007/s10751-009-0021-x doi (DE-627)SPR013000756 (SPR)s10751-009-0021-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Engels, R. verfasserin aut Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested. Lamb shift (dpeaa)DE-He213 Hyperfine Splitting (dpeaa)DE-He213 Spinfilter (dpeaa)DE-He213 Grigoryev, K. verfasserin aut Mikirtytchyants, M. verfasserin aut Paetz gen. Schieck, H. verfasserin aut Rathmann, F. verfasserin aut Schug, G. verfasserin aut Ströher, H. verfasserin aut Vasilyev, A. verfasserin aut Westig, M. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 193(2009), 1-3 vom: 28. Aug. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:193 year:2009 number:1-3 day:28 month:08 https://dx.doi.org/10.1007/s10751-009-0021-x 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_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2021 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 193 2009 1-3 28 08
allfieldsGer	10.1007/s10751-009-0021-x doi (DE-627)SPR013000756 (SPR)s10751-009-0021-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Engels, R. verfasserin aut Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested. Lamb shift (dpeaa)DE-He213 Hyperfine Splitting (dpeaa)DE-He213 Spinfilter (dpeaa)DE-He213 Grigoryev, K. verfasserin aut Mikirtytchyants, M. verfasserin aut Paetz gen. Schieck, H. verfasserin aut Rathmann, F. verfasserin aut Schug, G. verfasserin aut Ströher, H. verfasserin aut Vasilyev, A. verfasserin aut Westig, M. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 193(2009), 1-3 vom: 28. Aug. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:193 year:2009 number:1-3 day:28 month:08 https://dx.doi.org/10.1007/s10751-009-0021-x 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_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2021 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 193 2009 1-3 28 08
allfieldsSound	10.1007/s10751-009-0021-x doi (DE-627)SPR013000756 (SPR)s10751-009-0021-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Engels, R. verfasserin aut Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested. Lamb shift (dpeaa)DE-He213 Hyperfine Splitting (dpeaa)DE-He213 Spinfilter (dpeaa)DE-He213 Grigoryev, K. verfasserin aut Mikirtytchyants, M. verfasserin aut Paetz gen. Schieck, H. verfasserin aut Rathmann, F. verfasserin aut Schug, G. verfasserin aut Ströher, H. verfasserin aut Vasilyev, A. verfasserin aut Westig, M. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 193(2009), 1-3 vom: 28. Aug. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:193 year:2009 number:1-3 day:28 month:08 https://dx.doi.org/10.1007/s10751-009-0021-x 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_266 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2021 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4313 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4700 33.00 ASE AR 193 2009 1-3 28 08
language	English
source	Enthalten in Hyperfine interactions 193(2009), 1-3 vom: 28. Aug. volume:193 year:2009 number:1-3 day:28 month:08
sourceStr	Enthalten in Hyperfine interactions 193(2009), 1-3 vom: 28. Aug. volume:193 year:2009 number:1-3 day:28 month:08
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Lamb shift Hyperfine Splitting Spinfilter
dewey-raw	530
isfreeaccess_bool	false
container_title	Hyperfine interactions
authorswithroles_txt_mv	Engels, R. @@aut@@ Grigoryev, K. @@aut@@ Mikirtytchyants, M. @@aut@@ Paetz gen. Schieck, H. @@aut@@ Rathmann, F. @@aut@@ Schug, G. @@aut@@ Ströher, H. @@aut@@ Vasilyev, A. @@aut@@ Westig, M. @@aut@@
publishDateDaySort_date	2009-08-28T00:00:00Z
hierarchy_top_id	320612953
dewey-sort	3530
id	SPR013000756
language_de	englisch
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author	Engels, R.
spellingShingle	Engels, R. ddc 530 bkl 33.00 misc Lamb shift misc Hyperfine Splitting misc Spinfilter Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter
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topic_title	530 ASE 33.00 bkl Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter Lamb shift (dpeaa)DE-He213 Hyperfine Splitting (dpeaa)DE-He213 Spinfilter (dpeaa)DE-He213
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title	Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter
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title_full	Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter
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author_browse	Engels, R. Grigoryev, K. Mikirtytchyants, M. Paetz gen. Schieck, H. Rathmann, F. Schug, G. Ströher, H. Vasilyev, A. Westig, M.
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title_sort	precision spectroscopy of metastable hydrogen and antihydrogen with a lamb-shift polarimeter
title_auth	Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter
abstract	Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested.
abstractGer	Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested.
abstract_unstemmed	Abstract A spinfilter, the most important component of a Lamb-shift polarimeter, can be used to produce a beam of metastable hydrogen (deuterium) atoms in one hyperfine state (α1, α2 and together with the Sona transition β3). As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. Application of this method to anti-hydrogen atoms are suggested.
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title_short	Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter
url	https://dx.doi.org/10.1007/s10751-009-0021-x
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author2	Grigoryev, K. Mikirtytchyants, M. Paetz gen. Schieck, H. Rathmann, F. Schug, G. Ströher, H. Vasilyev, A. Westig, M.
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As function of a magnetic field separated transitions between the 2S1/2 metastable hyperfine states seem to be observable as well as single transitions into the short-lived 2P1/2 and 2P3/2 states. The Breit-Rabi diagrams for these states can be measured with good precision. Furthermore, the hyperfine splittings and the Lamb shift can be observed as well. 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Schieck, H.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Rathmann, F.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Schug, G.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ströher, H.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Vasilyev, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Westig, M.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Hyperfine interactions</subfield><subfield code="d">Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975</subfield><subfield code="g">193(2009), 1-3 vom: 28. 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Precision spectroscopy of metastable hydrogen and antihydrogen with a Lamb-shift polarimeter

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