Search for Bs → ϕµµ decay at the Large Hadron Collider

Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Singh, Supreet Pal [verfasserIn] Mazumdar, K. [verfasserIn] Singh, J. B. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2010

Schlagwörter:	-mesons Large Hadron Collider

Übergeordnetes Werk:	Enthalten in: Pramāna - Bangalore : Indian Inst. of Science, 1973, 75(2010), 4 vom: Okt., Seite 639-648
Übergeordnetes Werk:	volume:75 ; year:2010 ; number:4 ; month:10 ; pages:639-648

Links:	Volltext

DOI / URN:	10.1007/s12043-010-0144-2

Katalog-ID:	SPR024406740

Internformat


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520			\|a Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better.
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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_65
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_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_2001
912			\|a GBV_ILN_2003
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_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
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_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
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_2119
912			\|a GBV_ILN_2122
912			\|a GBV_ILN_2129
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_2190
912			\|a GBV_ILN_2232
912			\|a GBV_ILN_2336
912			\|a GBV_ILN_2446
912			\|a GBV_ILN_2470
912			\|a GBV_ILN_2472
912			\|a GBV_ILN_2507
912			\|a GBV_ILN_2522
912			\|a GBV_ILN_2548
912			\|a GBV_ILN_4012
912			\|a GBV_ILN_4035
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4046
912			\|a GBV_ILN_4112
912			\|a GBV_ILN_4125
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4242
912			\|a GBV_ILN_4246
912			\|a GBV_ILN_4249
912			\|a GBV_ILN_4251
912			\|a GBV_ILN_4305
912			\|a GBV_ILN_4306
912			\|a GBV_ILN_4307
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
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_4338
912			\|a GBV_ILN_4367
912			\|a GBV_ILN_4393
912			\|a GBV_ILN_4700
936	b	k	\|a 33.00 \|q ASE
951			\|a AR
952			\|d 75 \|j 2010 \|e 4 \|c 10 \|h 639-648

Indexfelder

author_variant	s p s sp sps k m km j b s jb jbs
matchkey_str	article:09737111:2010----::erhobdcythlrear
hierarchy_sort_str	2010
bklnumber	33.00
publishDate	2010
allfields	10.1007/s12043-010-0144-2 doi (DE-627)SPR024406740 (SPR)s12043-010-0144-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Singh, Supreet Pal verfasserin aut Search for Bs → ϕµµ decay at the Large Hadron Collider 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better. -mesons (dpeaa)DE-He213 Large Hadron Collider (dpeaa)DE-He213 Mazumdar, K. verfasserin aut Singh, J. B. verfasserin aut Enthalten in Pramāna Bangalore : Indian Inst. of Science, 1973 75(2010), 4 vom: Okt., Seite 639-648 (DE-627)328820806 (DE-600)2046354-6 0973-7111 nnns volume:75 year:2010 number:4 month:10 pages:639-648 https://dx.doi.org/10.1007/s12043-010-0144-2 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_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_206 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 75 2010 4 10 639-648
spelling	10.1007/s12043-010-0144-2 doi (DE-627)SPR024406740 (SPR)s12043-010-0144-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Singh, Supreet Pal verfasserin aut Search for Bs → ϕµµ decay at the Large Hadron Collider 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better. -mesons (dpeaa)DE-He213 Large Hadron Collider (dpeaa)DE-He213 Mazumdar, K. verfasserin aut Singh, J. B. verfasserin aut Enthalten in Pramāna Bangalore : Indian Inst. of Science, 1973 75(2010), 4 vom: Okt., Seite 639-648 (DE-627)328820806 (DE-600)2046354-6 0973-7111 nnns volume:75 year:2010 number:4 month:10 pages:639-648 https://dx.doi.org/10.1007/s12043-010-0144-2 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_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_206 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 75 2010 4 10 639-648
allfields_unstemmed	10.1007/s12043-010-0144-2 doi (DE-627)SPR024406740 (SPR)s12043-010-0144-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Singh, Supreet Pal verfasserin aut Search for Bs → ϕµµ decay at the Large Hadron Collider 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better. -mesons (dpeaa)DE-He213 Large Hadron Collider (dpeaa)DE-He213 Mazumdar, K. verfasserin aut Singh, J. B. verfasserin aut Enthalten in Pramāna Bangalore : Indian Inst. of Science, 1973 75(2010), 4 vom: Okt., Seite 639-648 (DE-627)328820806 (DE-600)2046354-6 0973-7111 nnns volume:75 year:2010 number:4 month:10 pages:639-648 https://dx.doi.org/10.1007/s12043-010-0144-2 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_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_206 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 75 2010 4 10 639-648
allfieldsGer	10.1007/s12043-010-0144-2 doi (DE-627)SPR024406740 (SPR)s12043-010-0144-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Singh, Supreet Pal verfasserin aut Search for Bs → ϕµµ decay at the Large Hadron Collider 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better. -mesons (dpeaa)DE-He213 Large Hadron Collider (dpeaa)DE-He213 Mazumdar, K. verfasserin aut Singh, J. B. verfasserin aut Enthalten in Pramāna Bangalore : Indian Inst. of Science, 1973 75(2010), 4 vom: Okt., Seite 639-648 (DE-627)328820806 (DE-600)2046354-6 0973-7111 nnns volume:75 year:2010 number:4 month:10 pages:639-648 https://dx.doi.org/10.1007/s12043-010-0144-2 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_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_206 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 75 2010 4 10 639-648
allfieldsSound	10.1007/s12043-010-0144-2 doi (DE-627)SPR024406740 (SPR)s12043-010-0144-2-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Singh, Supreet Pal verfasserin aut Search for Bs → ϕµµ decay at the Large Hadron Collider 2010 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better. -mesons (dpeaa)DE-He213 Large Hadron Collider (dpeaa)DE-He213 Mazumdar, K. verfasserin aut Singh, J. B. verfasserin aut Enthalten in Pramāna Bangalore : Indian Inst. of Science, 1973 75(2010), 4 vom: Okt., Seite 639-648 (DE-627)328820806 (DE-600)2046354-6 0973-7111 nnns volume:75 year:2010 number:4 month:10 pages:639-648 https://dx.doi.org/10.1007/s12043-010-0144-2 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_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_206 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_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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 33.00 ASE AR 75 2010 4 10 639-648
language	English
source	Enthalten in Pramāna 75(2010), 4 vom: Okt., Seite 639-648 volume:75 year:2010 number:4 month:10 pages:639-648
sourceStr	Enthalten in Pramāna 75(2010), 4 vom: Okt., Seite 639-648 volume:75 year:2010 number:4 month:10 pages:639-648
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	-mesons Large Hadron Collider
dewey-raw	530
isfreeaccess_bool	false
container_title	Pramāna
authorswithroles_txt_mv	Singh, Supreet Pal @@aut@@ Mazumdar, K. @@aut@@ Singh, J. B. @@aut@@
publishDateDaySort_date	2010-10-01T00:00:00Z
hierarchy_top_id	328820806
dewey-sort	3530
id	SPR024406740
language_de	englisch
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author	Singh, Supreet Pal
spellingShingle	Singh, Supreet Pal ddc 530 bkl 33.00 misc -mesons misc Large Hadron Collider Search for Bs → ϕµµ decay at the Large Hadron Collider
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topic_title	530 ASE 33.00 bkl Search for Bs → ϕµµ decay at the Large Hadron Collider -mesons (dpeaa)DE-He213 Large Hadron Collider (dpeaa)DE-He213
topic	ddc 530 bkl 33.00 misc -mesons misc Large Hadron Collider
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title	Search for Bs → ϕµµ decay at the Large Hadron Collider
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title_full	Search for Bs → ϕµµ decay at the Large Hadron Collider
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title_sort	search for bs → ϕµµ decay at the large hadron collider
title_auth	Search for Bs → ϕµµ decay at the Large Hadron Collider
abstract	Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better.
abstractGer	Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better.
abstract_unstemmed	Abstract As Bs-mesons will be produced abundantly at the LHC, the observability of the flavour-changing-neutral-current decay mode Bs → ϕ$ µ^{+} %$ µ^{−} $ has been studied in CMS at the LHC centre-of-mass energy of 10 TeV. With an integrated luminosity of 100 $ pb^{−1} $, an upper limit of 6.7 × $ 10^{−6} $ on the branching ratio is expected to be obtained. The potential at 7 TeV with a luminosity of 1 $ fb^{−1} $ is expected to be better.
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title_short	Search for Bs → ϕµµ decay at the Large Hadron Collider
url	https://dx.doi.org/10.1007/s12043-010-0144-2
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up_date	2024-07-04T00:48:44.038Z
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