Cross sections for $ K^{−} $−p interactions

Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Glasser, R. G. [verfasserIn] Seeman, N. Snow, G. A.

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	1958

Anmerkung:	© Società Italiana di Fisica 1958

Übergeordnetes Werk:	Enthalten in: Il nuovo cimento - Pisa, 1855, 7(1958), 2 vom: Jan., Seite 142-146
Übergeordnetes Werk:	volume:7 ; year:1958 ; number:2 ; month:01 ; pages:142-146

Links:	Volltext

DOI / URN:	10.1007/BF02744193

Katalog-ID:	SPR03730755X

Internformat


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008	201007s1958 xx \|\|\|\|\|o 00\| \|\|eng c
024	7		\|a 10.1007/BF02744193 \|2 doi
035			\|a (DE-627)SPR03730755X
035			\|a (SPR)BF02744193-e
040			\|a DE-627 \|b ger \|c DE-627 \|e rakwb
041			\|a eng
100	1		\|a Glasser, R. G. \|e verfasserin \|4 aut
245	1	0	\|a Cross sections for $ K^{−} $−p interactions
264		1	\|c 1958
336			\|a Text \|b txt \|2 rdacontent
337			\|a Computermedien \|b c \|2 rdamedia
338			\|a Online-Ressource \|b cr \|2 rdacarrier
500			\|a © Società Italiana di Fisica 1958
520			\|a Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases.
700	1		\|a Seeman, N. \|4 aut
700	1		\|a Snow, G. A. \|4 aut
773	0	8	\|i Enthalten in \|t Il nuovo cimento \|d Pisa, 1855 \|g 7(1958), 2 vom: Jan., Seite 142-146 \|w (DE-627)626757762 \|w (DE-600)2554784-7 \|x 1827-6121 \|7 nnns
773	1	8	\|g volume:7 \|g year:1958 \|g number:2 \|g month:01 \|g pages:142-146
856	4	0	\|u https://dx.doi.org/10.1007/BF02744193 \|z lizenzpflichtig \|3 Volltext
912			\|a GBV_USEFLAG_A
912			\|a SYSFLAG_A
912			\|a GBV_SPRINGER
912			\|a GBV_ILN_11
912			\|a GBV_ILN_20
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_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_121
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_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_374
912			\|a GBV_ILN_602
912			\|a GBV_ILN_647
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_2018
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_2043
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
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_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_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_2158
912			\|a GBV_ILN_2188
912			\|a GBV_ILN_2190
912			\|a GBV_ILN_2193
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_2808
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_4277
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_4328
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_4346
912			\|a GBV_ILN_4367
912			\|a GBV_ILN_4393
912			\|a GBV_ILN_4700
912			\|a GBV_ILN_4753
951			\|a AR
952			\|d 7 \|j 1958 \|e 2 \|c 01 \|h 142-146

Indexfelder

author_variant	r g g rg rgg n s ns g a s ga gas
matchkey_str	article:18276121:1958----::rsscinfrpn
hierarchy_sort_str	1958
publishDate	1958
allfields	10.1007/BF02744193 doi (DE-627)SPR03730755X (SPR)BF02744193-e DE-627 ger DE-627 rakwb eng Glasser, R. G. verfasserin aut Cross sections for $ K^{−} $−p interactions 1958 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1958 Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases. Seeman, N. aut Snow, G. A. aut Enthalten in Il nuovo cimento Pisa, 1855 7(1958), 2 vom: Jan., Seite 142-146 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:7 year:1958 number:2 month:01 pages:142-146 https://dx.doi.org/10.1007/BF02744193 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 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_4277 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_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 7 1958 2 01 142-146
spelling	10.1007/BF02744193 doi (DE-627)SPR03730755X (SPR)BF02744193-e DE-627 ger DE-627 rakwb eng Glasser, R. G. verfasserin aut Cross sections for $ K^{−} $−p interactions 1958 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1958 Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases. Seeman, N. aut Snow, G. A. aut Enthalten in Il nuovo cimento Pisa, 1855 7(1958), 2 vom: Jan., Seite 142-146 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:7 year:1958 number:2 month:01 pages:142-146 https://dx.doi.org/10.1007/BF02744193 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 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_4277 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_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 7 1958 2 01 142-146
allfields_unstemmed	10.1007/BF02744193 doi (DE-627)SPR03730755X (SPR)BF02744193-e DE-627 ger DE-627 rakwb eng Glasser, R. G. verfasserin aut Cross sections for $ K^{−} $−p interactions 1958 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1958 Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases. Seeman, N. aut Snow, G. A. aut Enthalten in Il nuovo cimento Pisa, 1855 7(1958), 2 vom: Jan., Seite 142-146 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:7 year:1958 number:2 month:01 pages:142-146 https://dx.doi.org/10.1007/BF02744193 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 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_4277 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_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 7 1958 2 01 142-146
allfieldsGer	10.1007/BF02744193 doi (DE-627)SPR03730755X (SPR)BF02744193-e DE-627 ger DE-627 rakwb eng Glasser, R. G. verfasserin aut Cross sections for $ K^{−} $−p interactions 1958 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1958 Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases. Seeman, N. aut Snow, G. A. aut Enthalten in Il nuovo cimento Pisa, 1855 7(1958), 2 vom: Jan., Seite 142-146 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:7 year:1958 number:2 month:01 pages:142-146 https://dx.doi.org/10.1007/BF02744193 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 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_4277 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_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 7 1958 2 01 142-146
allfieldsSound	10.1007/BF02744193 doi (DE-627)SPR03730755X (SPR)BF02744193-e DE-627 ger DE-627 rakwb eng Glasser, R. G. verfasserin aut Cross sections for $ K^{−} $−p interactions 1958 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1958 Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases. Seeman, N. aut Snow, G. A. aut Enthalten in Il nuovo cimento Pisa, 1855 7(1958), 2 vom: Jan., Seite 142-146 (DE-627)626757762 (DE-600)2554784-7 1827-6121 nnns volume:7 year:1958 number:2 month:01 pages:142-146 https://dx.doi.org/10.1007/BF02744193 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_121 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_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2043 GBV_ILN_2044 GBV_ILN_2048 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_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_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 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_4277 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_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 7 1958 2 01 142-146
language	English
source	Enthalten in Il nuovo cimento 7(1958), 2 vom: Jan., Seite 142-146 volume:7 year:1958 number:2 month:01 pages:142-146
sourceStr	Enthalten in Il nuovo cimento 7(1958), 2 vom: Jan., Seite 142-146 volume:7 year:1958 number:2 month:01 pages:142-146
format_phy_str_mv	Article
institution	findex.gbv.de
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container_title	Il nuovo cimento
authorswithroles_txt_mv	Glasser, R. G. @@aut@@ Seeman, N. @@aut@@ Snow, G. A. @@aut@@
publishDateDaySort_date	1958-01-01T00:00:00Z
hierarchy_top_id	626757762
id	SPR03730755X
language_de	englisch
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G.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Cross sections for $ K^{−} $−p interactions</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1958</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Società Italiana di Fisica 1958</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. 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author	Glasser, R. G.
spellingShingle	Glasser, R. G. Cross sections for $ K^{−} $−p interactions
authorStr	Glasser, R. G.
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topic_title	Cross sections for $ K^{−} $−p interactions
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title	Cross sections for $ K^{−} $−p interactions
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title_full	Cross sections for $ K^{−} $−p interactions
author_sort	Glasser, R. G.
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author_browse	Glasser, R. G. Seeman, N. Snow, G. A.
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author-letter	Glasser, R. G.
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title_sort	cross sections for $ k^{−} $−p interactions
title_auth	Cross sections for $ K^{−} $−p interactions
abstract	Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases. © Società Italiana di Fisica 1958
abstractGer	Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases. © Società Italiana di Fisica 1958
abstract_unstemmed	Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. These events yield Σ(k−+ p→ $ k^{−} $+ p) = 33−9+12mb and Σ(k−+ p → $ ɛ^{+−} $ + $ π^{−+} $)= 29−9+12mb averaged over the energy region 0/82 MeV. The data indicate that Σ(k− + p → $ ɛ^{+−} $ + $ π^{−+} $)rises as the $ K^{−} $ energy decreases. © Società Italiana di Fisica 1958
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title_short	Cross sections for $ K^{−} $−p interactions
url	https://dx.doi.org/10.1007/BF02744193
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up_date	2024-07-03T22:09:48.539Z
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G.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Cross sections for $ K^{−} $−p interactions</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1958</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Società Italiana di Fisica 1958</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Summary Nine $ K^{−} $+p elastic scattering events and eight $ K^{−} $ + p → → $ ɛ^{±} $+$ π^{∓} $ avents have been observed in nuclear emulsion. 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Cross sections for $ K^{−} $−p interactions

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