Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−)

Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Sultanov, Renat A. [verfasserIn] Guster, D. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2014

Schlagwörter:	Ultra-slow antiproton Antihydrogen Muonic antihydrogen Few-body systems

Übergeordnetes Werk:	Enthalten in: Hyperfine interactions - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975, 228(2014), 1-3 vom: 15. Jan., Seite 47-52
Übergeordnetes Werk:	volume:228 ; year:2014 ; number:1-3 ; day:15 ; month:01 ; pages:47-52

Links:	Volltext

DOI / URN:	10.1007/s10751-013-1005-4

Katalog-ID:	SPR013011057

Internformat


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520			\|a Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach.
650		4	\|a Ultra-slow antiproton \|7 (dpeaa)DE-He213
650		4	\|a Antihydrogen \|7 (dpeaa)DE-He213
650		4	\|a Muonic antihydrogen \|7 (dpeaa)DE-He213
650		4	\|a Few-body systems \|7 (dpeaa)DE-He213
700	1		\|a Guster, D. \|e verfasserin \|4 aut
773	0	8	\|i Enthalten in \|t Hyperfine interactions \|d Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 \|g 228(2014), 1-3 vom: 15. Jan., Seite 47-52 \|w (DE-627)320612953 \|w (DE-600)2021614-2 \|x 1572-9540 \|7 nnns
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912			\|a GBV_ILN_22
912			\|a GBV_ILN_23
912			\|a GBV_ILN_24
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_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_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_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_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
936	b	k	\|a 33.00 \|q ASE
951			\|a AR
952			\|d 228 \|j 2014 \|e 1-3 \|b 15 \|c 01 \|h 47-52

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bklnumber	33.00
publishDate	2014
allfields	10.1007/s10751-013-1005-4 doi (DE-627)SPR013011057 (SPR)s10751-013-1005-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sultanov, Renat A. verfasserin aut Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−) 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach. Ultra-slow antiproton (dpeaa)DE-He213 Antihydrogen (dpeaa)DE-He213 Muonic antihydrogen (dpeaa)DE-He213 Few-body systems (dpeaa)DE-He213 Guster, D. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 228(2014), 1-3 vom: 15. Jan., Seite 47-52 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:228 year:2014 number:1-3 day:15 month:01 pages:47-52 https://dx.doi.org/10.1007/s10751-013-1005-4 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_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_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_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 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 228 2014 1-3 15 01 47-52
spelling	10.1007/s10751-013-1005-4 doi (DE-627)SPR013011057 (SPR)s10751-013-1005-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sultanov, Renat A. verfasserin aut Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−) 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach. Ultra-slow antiproton (dpeaa)DE-He213 Antihydrogen (dpeaa)DE-He213 Muonic antihydrogen (dpeaa)DE-He213 Few-body systems (dpeaa)DE-He213 Guster, D. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 228(2014), 1-3 vom: 15. Jan., Seite 47-52 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:228 year:2014 number:1-3 day:15 month:01 pages:47-52 https://dx.doi.org/10.1007/s10751-013-1005-4 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_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_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_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 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 228 2014 1-3 15 01 47-52
allfields_unstemmed	10.1007/s10751-013-1005-4 doi (DE-627)SPR013011057 (SPR)s10751-013-1005-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sultanov, Renat A. verfasserin aut Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−) 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach. Ultra-slow antiproton (dpeaa)DE-He213 Antihydrogen (dpeaa)DE-He213 Muonic antihydrogen (dpeaa)DE-He213 Few-body systems (dpeaa)DE-He213 Guster, D. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 228(2014), 1-3 vom: 15. Jan., Seite 47-52 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:228 year:2014 number:1-3 day:15 month:01 pages:47-52 https://dx.doi.org/10.1007/s10751-013-1005-4 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_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_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_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 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 228 2014 1-3 15 01 47-52
allfieldsGer	10.1007/s10751-013-1005-4 doi (DE-627)SPR013011057 (SPR)s10751-013-1005-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sultanov, Renat A. verfasserin aut Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−) 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach. Ultra-slow antiproton (dpeaa)DE-He213 Antihydrogen (dpeaa)DE-He213 Muonic antihydrogen (dpeaa)DE-He213 Few-body systems (dpeaa)DE-He213 Guster, D. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 228(2014), 1-3 vom: 15. Jan., Seite 47-52 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:228 year:2014 number:1-3 day:15 month:01 pages:47-52 https://dx.doi.org/10.1007/s10751-013-1005-4 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_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_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_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 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 228 2014 1-3 15 01 47-52
allfieldsSound	10.1007/s10751-013-1005-4 doi (DE-627)SPR013011057 (SPR)s10751-013-1005-4-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Sultanov, Renat A. verfasserin aut Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−) 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach. Ultra-slow antiproton (dpeaa)DE-He213 Antihydrogen (dpeaa)DE-He213 Muonic antihydrogen (dpeaa)DE-He213 Few-body systems (dpeaa)DE-He213 Guster, D. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 228(2014), 1-3 vom: 15. Jan., Seite 47-52 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:228 year:2014 number:1-3 day:15 month:01 pages:47-52 https://dx.doi.org/10.1007/s10751-013-1005-4 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_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_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_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2106 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 228 2014 1-3 15 01 47-52
language	English
source	Enthalten in Hyperfine interactions 228(2014), 1-3 vom: 15. Jan., Seite 47-52 volume:228 year:2014 number:1-3 day:15 month:01 pages:47-52
sourceStr	Enthalten in Hyperfine interactions 228(2014), 1-3 vom: 15. Jan., Seite 47-52 volume:228 year:2014 number:1-3 day:15 month:01 pages:47-52
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Ultra-slow antiproton Antihydrogen Muonic antihydrogen Few-body systems
dewey-raw	530
isfreeaccess_bool	false
container_title	Hyperfine interactions
authorswithroles_txt_mv	Sultanov, Renat A. @@aut@@ Guster, D. @@aut@@
publishDateDaySort_date	2014-01-15T00:00:00Z
hierarchy_top_id	320612953
dewey-sort	3530
id	SPR013011057
language_de	englisch
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author	Sultanov, Renat A.
spellingShingle	Sultanov, Renat A. ddc 530 bkl 33.00 misc Ultra-slow antiproton misc Antihydrogen misc Muonic antihydrogen misc Few-body systems Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−)
authorStr	Sultanov, Renat A.
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topic_title	530 ASE 33.00 bkl Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−) Ultra-slow antiproton (dpeaa)DE-He213 Antihydrogen (dpeaa)DE-He213 Muonic antihydrogen (dpeaa)DE-He213 Few-body systems (dpeaa)DE-He213
topic	ddc 530 bkl 33.00 misc Ultra-slow antiproton misc Antihydrogen misc Muonic antihydrogen misc Few-body systems
topic_unstemmed	ddc 530 bkl 33.00 misc Ultra-slow antiproton misc Antihydrogen misc Muonic antihydrogen misc Few-body systems
topic_browse	ddc 530 bkl 33.00 misc Ultra-slow antiproton misc Antihydrogen misc Muonic antihydrogen misc Few-body systems
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title	Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−)
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title_full	Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−)
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title_sort	antiproton low-energy collisions with ps-atoms and true muonium atoms (μ+μ−)
title_auth	Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−)
abstract	Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach.
abstractGer	Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach.
abstract_unstemmed	Abstract Three-charge-particle collisions with participation of ultra-slow antiprotons ($\overline {\rm {p}}$) is the subject of this work. Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach.
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title_short	Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−)
url	https://dx.doi.org/10.1007/s10751-013-1005-4
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Specifically we compute the total cross sections and corresponding thermal rates of the following three-body reactions: $\overline {\rm p}+(e^+e^-) \rightarrow \overline {\rm {H}} + e^-$ and $\overline {\rm p}+(\mu ^+\mu ^-) \rightarrow \overline {\rm {H}}_{\mu } + \mu ^-$, where $e^-(\mu ^-)$ is an electron (muon) and $e^+(\mu ^+)$ is a positron (antimuon) respectively, $\overline {\rm {H}}=(\overline {\rm p}e^+)$ is an antihydrogen atom and $\overline {\rm {H}}_{\mu }=(\overline {\rm p}\mu ^+)$ is a muonic antihydrogen atom, i.e. a bound state of $\overline {\rm {p}}$ and μ+. A set of two-coupled few-body Faddeev-Hahn-type (FH-type) equations is numerically solved in the framework of a modified close-coupling expansion approach.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Ultra-slow antiproton</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Antihydrogen</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Muonic antihydrogen</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Few-body systems</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Guster, D.</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">228(2014), 1-3 vom: 15. 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Antiproton low-energy collisions with Ps-atoms and true muonium atoms (μ+μ−)

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