Double-strangeness production with antiprotons

Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics...
Ausführliche Beschreibung

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Autor*in:	Zmeskal, J. [verfasserIn] Bühler, P. [verfasserIn] Cargnelli, M. [verfasserIn] Ishiwatari, T. [verfasserIn] Kienle, P. [verfasserIn] Marton, J. [verfasserIn] Suzuki, K. [verfasserIn] Widmann, E. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2009

Schlagwörter:	Low-energy QCD High density nuclear systems

Übergeordnetes Werk:	Enthalten in: Hyperfine interactions - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975, 194(2009), 1-3 vom: 04. Sept.
Übergeordnetes Werk:	volume:194 ; year:2009 ; number:1-3 ; day:04 ; month:09

Links:	Volltext

DOI / URN:	10.1007/s10751-009-0082-x

Katalog-ID:	SPR01300154X

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520			\|a Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature.
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700	1		\|a Widmann, E. \|e verfasserin \|4 aut
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912			\|a GBV_ILN_95
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912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
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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
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912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
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912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
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912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2061
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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
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matchkey_str	article:15729540:2009----::obetagnspoutowt
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publishDate	2009
allfields	10.1007/s10751-009-0082-x doi (DE-627)SPR01300154X (SPR)s10751-009-0082-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Zmeskal, J. verfasserin aut Double-strangeness production with antiprotons 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature. Low-energy QCD (dpeaa)DE-He213 High density nuclear systems (dpeaa)DE-He213 Bühler, P. verfasserin aut Cargnelli, M. verfasserin aut Ishiwatari, T. verfasserin aut Kienle, P. verfasserin aut Marton, J. verfasserin aut Suzuki, K. verfasserin aut Widmann, E. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 194(2009), 1-3 vom: 04. Sept. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:194 year:2009 number:1-3 day:04 month:09 https://dx.doi.org/10.1007/s10751-009-0082-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 194 2009 1-3 04 09
spelling	10.1007/s10751-009-0082-x doi (DE-627)SPR01300154X (SPR)s10751-009-0082-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Zmeskal, J. verfasserin aut Double-strangeness production with antiprotons 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature. Low-energy QCD (dpeaa)DE-He213 High density nuclear systems (dpeaa)DE-He213 Bühler, P. verfasserin aut Cargnelli, M. verfasserin aut Ishiwatari, T. verfasserin aut Kienle, P. verfasserin aut Marton, J. verfasserin aut Suzuki, K. verfasserin aut Widmann, E. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 194(2009), 1-3 vom: 04. Sept. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:194 year:2009 number:1-3 day:04 month:09 https://dx.doi.org/10.1007/s10751-009-0082-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 194 2009 1-3 04 09
allfields_unstemmed	10.1007/s10751-009-0082-x doi (DE-627)SPR01300154X (SPR)s10751-009-0082-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Zmeskal, J. verfasserin aut Double-strangeness production with antiprotons 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature. Low-energy QCD (dpeaa)DE-He213 High density nuclear systems (dpeaa)DE-He213 Bühler, P. verfasserin aut Cargnelli, M. verfasserin aut Ishiwatari, T. verfasserin aut Kienle, P. verfasserin aut Marton, J. verfasserin aut Suzuki, K. verfasserin aut Widmann, E. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 194(2009), 1-3 vom: 04. Sept. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:194 year:2009 number:1-3 day:04 month:09 https://dx.doi.org/10.1007/s10751-009-0082-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 194 2009 1-3 04 09
allfieldsGer	10.1007/s10751-009-0082-x doi (DE-627)SPR01300154X (SPR)s10751-009-0082-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Zmeskal, J. verfasserin aut Double-strangeness production with antiprotons 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature. Low-energy QCD (dpeaa)DE-He213 High density nuclear systems (dpeaa)DE-He213 Bühler, P. verfasserin aut Cargnelli, M. verfasserin aut Ishiwatari, T. verfasserin aut Kienle, P. verfasserin aut Marton, J. verfasserin aut Suzuki, K. verfasserin aut Widmann, E. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 194(2009), 1-3 vom: 04. Sept. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:194 year:2009 number:1-3 day:04 month:09 https://dx.doi.org/10.1007/s10751-009-0082-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 194 2009 1-3 04 09
allfieldsSound	10.1007/s10751-009-0082-x doi (DE-627)SPR01300154X (SPR)s10751-009-0082-x-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Zmeskal, J. verfasserin aut Double-strangeness production with antiprotons 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature. Low-energy QCD (dpeaa)DE-He213 High density nuclear systems (dpeaa)DE-He213 Bühler, P. verfasserin aut Cargnelli, M. verfasserin aut Ishiwatari, T. verfasserin aut Kienle, P. verfasserin aut Marton, J. verfasserin aut Suzuki, K. verfasserin aut Widmann, E. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 194(2009), 1-3 vom: 04. Sept. (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:194 year:2009 number:1-3 day:04 month:09 https://dx.doi.org/10.1007/s10751-009-0082-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 194 2009 1-3 04 09
language	English
source	Enthalten in Hyperfine interactions 194(2009), 1-3 vom: 04. Sept. volume:194 year:2009 number:1-3 day:04 month:09
sourceStr	Enthalten in Hyperfine interactions 194(2009), 1-3 vom: 04. Sept. volume:194 year:2009 number:1-3 day:04 month:09
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Low-energy QCD High density nuclear systems
dewey-raw	530
isfreeaccess_bool	false
container_title	Hyperfine interactions
authorswithroles_txt_mv	Zmeskal, J. @@aut@@ Bühler, P. @@aut@@ Cargnelli, M. @@aut@@ Ishiwatari, T. @@aut@@ Kienle, P. @@aut@@ Marton, J. @@aut@@ Suzuki, K. @@aut@@ Widmann, E. @@aut@@
publishDateDaySort_date	2009-09-04T00:00:00Z
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author	Zmeskal, J.
spellingShingle	Zmeskal, J. ddc 530 bkl 33.00 misc Low-energy QCD misc High density nuclear systems Double-strangeness production with antiprotons
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topic_title	530 ASE 33.00 bkl Double-strangeness production with antiprotons Low-energy QCD (dpeaa)DE-He213 High density nuclear systems (dpeaa)DE-He213
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title	Double-strangeness production with antiprotons
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title_full	Double-strangeness production with antiprotons
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title_sort	double-strangeness production with antiprotons
title_auth	Double-strangeness production with antiprotons
abstract	Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature.
abstractGer	Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature.
abstract_unstemmed	Abstract The production of double-strangeness by antiproton annihilation in nuclei will be an exciting way to investigate whether the formation of deeply bound antikaonic nuclear clusters occurs. The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. If such dense systems are created, conditions in the phase diagram might be reached where phase transition to kaon condensation or colour superconductivity will occur at low temperature.
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title_short	Double-strangeness production with antiprotons
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The existence of deeply bound antikaonic nuclear clusters is a lively debated problem in hadron physics today, which can be solved only experimentally. At CERN with the Antiproton Decelerator (AD) and in future with the new FAIR facility at Darmstadt low energy antiprotons are available to perform this type of experiments. The use of antiprotons for the production of double-strangeness was recently discussed by Weise and Kienle and indeed, it would be very challenging to produce and study such “double-strange nuclei” in the view of the prediction of Akaishi and Yamazaki that double-antikaon bound nuclear systems with strangeness (S = − 2) will be formed with binding energies up to 200–300 MeV. Such binding energies might result in an increase of the average density to more than 3 times the average nuclear density. 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Double-strangeness production with antiprotons

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