Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE
Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Scordo, A. [verfasserIn] Curceanu, C. [verfasserIn] Piscicchia, K. [verfasserIn] Tucakovic, I. [verfasserIn] Vazquez Doce, O. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2014 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Few-body systems - Wien [u.a.] : Springer, 1986, 55(2014), 8-10 vom: 10. Jan., Seite 741-744 |
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| Übergeordnetes Werk: |
volume:55 ; year:2014 ; number:8-10 ; day:10 ; month:01 ; pages:741-744 |
| Links: |
|---|
| DOI / URN: |
10.1007/s00601-013-0783-1 |
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| Katalog-ID: |
SPR007056389 |
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| 245 | 1 | 0 | |a Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE |
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| 520 | |a Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. | ||
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| 650 | 4 | |a Invariant Mass Spectrum |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Neutral Cluster |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Curceanu, C. |e verfasserin |4 aut | |
| 700 | 1 | |a Piscicchia, K. |e verfasserin |4 aut | |
| 700 | 1 | |a Tucakovic, I. |e verfasserin |4 aut | |
| 700 | 1 | |a Vazquez Doce, O. |e verfasserin |4 aut | |
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10.1007/s00601-013-0783-1 doi (DE-627)SPR007056389 (SPR)s00601-013-0783-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Scordo, A. verfasserin aut Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. Invariant Mass (dpeaa)DE-He213 Decay Channel (dpeaa)DE-He213 Drift Chamber (dpeaa)DE-He213 Invariant Mass Spectrum (dpeaa)DE-He213 Neutral Cluster (dpeaa)DE-He213 Curceanu, C. verfasserin aut Piscicchia, K. verfasserin aut Tucakovic, I. verfasserin aut Vazquez Doce, O. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 55(2014), 8-10 vom: 10. Jan., Seite 741-744 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:55 year:2014 number:8-10 day:10 month:01 pages:741-744 https://dx.doi.org/10.1007/s00601-013-0783-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_267 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 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_4320 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_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 55 2014 8-10 10 01 741-744 |
| spelling |
10.1007/s00601-013-0783-1 doi (DE-627)SPR007056389 (SPR)s00601-013-0783-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Scordo, A. verfasserin aut Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. Invariant Mass (dpeaa)DE-He213 Decay Channel (dpeaa)DE-He213 Drift Chamber (dpeaa)DE-He213 Invariant Mass Spectrum (dpeaa)DE-He213 Neutral Cluster (dpeaa)DE-He213 Curceanu, C. verfasserin aut Piscicchia, K. verfasserin aut Tucakovic, I. verfasserin aut Vazquez Doce, O. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 55(2014), 8-10 vom: 10. Jan., Seite 741-744 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:55 year:2014 number:8-10 day:10 month:01 pages:741-744 https://dx.doi.org/10.1007/s00601-013-0783-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_267 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 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_4320 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_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 55 2014 8-10 10 01 741-744 |
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10.1007/s00601-013-0783-1 doi (DE-627)SPR007056389 (SPR)s00601-013-0783-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Scordo, A. verfasserin aut Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. Invariant Mass (dpeaa)DE-He213 Decay Channel (dpeaa)DE-He213 Drift Chamber (dpeaa)DE-He213 Invariant Mass Spectrum (dpeaa)DE-He213 Neutral Cluster (dpeaa)DE-He213 Curceanu, C. verfasserin aut Piscicchia, K. verfasserin aut Tucakovic, I. verfasserin aut Vazquez Doce, O. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 55(2014), 8-10 vom: 10. Jan., Seite 741-744 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:55 year:2014 number:8-10 day:10 month:01 pages:741-744 https://dx.doi.org/10.1007/s00601-013-0783-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_267 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 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_4320 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_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 55 2014 8-10 10 01 741-744 |
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10.1007/s00601-013-0783-1 doi (DE-627)SPR007056389 (SPR)s00601-013-0783-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Scordo, A. verfasserin aut Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. Invariant Mass (dpeaa)DE-He213 Decay Channel (dpeaa)DE-He213 Drift Chamber (dpeaa)DE-He213 Invariant Mass Spectrum (dpeaa)DE-He213 Neutral Cluster (dpeaa)DE-He213 Curceanu, C. verfasserin aut Piscicchia, K. verfasserin aut Tucakovic, I. verfasserin aut Vazquez Doce, O. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 55(2014), 8-10 vom: 10. Jan., Seite 741-744 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:55 year:2014 number:8-10 day:10 month:01 pages:741-744 https://dx.doi.org/10.1007/s00601-013-0783-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_267 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 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_4320 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_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 55 2014 8-10 10 01 741-744 |
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10.1007/s00601-013-0783-1 doi (DE-627)SPR007056389 (SPR)s00601-013-0783-1-e DE-627 ger DE-627 rakwb eng 530 ASE 31.00 bkl 33.00 bkl Scordo, A. verfasserin aut Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. Invariant Mass (dpeaa)DE-He213 Decay Channel (dpeaa)DE-He213 Drift Chamber (dpeaa)DE-He213 Invariant Mass Spectrum (dpeaa)DE-He213 Neutral Cluster (dpeaa)DE-He213 Curceanu, C. verfasserin aut Piscicchia, K. verfasserin aut Tucakovic, I. verfasserin aut Vazquez Doce, O. verfasserin aut Enthalten in Few-body systems Wien [u.a.] : Springer, 1986 55(2014), 8-10 vom: 10. Jan., Seite 741-744 (DE-627)25372323X (DE-600)1459107-8 1432-5411 nnns volume:55 year:2014 number:8-10 day:10 month:01 pages:741-744 https://dx.doi.org/10.1007/s00601-013-0783-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE 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_267 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_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 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_4320 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_4393 GBV_ILN_4700 31.00 ASE 33.00 ASE AR 55 2014 8-10 10 01 741-744 |
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Enthalten in Few-body systems 55(2014), 8-10 vom: 10. Jan., Seite 741-744 volume:55 year:2014 number:8-10 day:10 month:01 pages:741-744 |
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Enthalten in Few-body systems 55(2014), 8-10 vom: 10. Jan., Seite 741-744 volume:55 year:2014 number:8-10 day:10 month:01 pages:741-744 |
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Invariant Mass Decay Channel Drift Chamber Invariant Mass Spectrum Neutral Cluster |
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Scordo, A. @@aut@@ Curceanu, C. @@aut@@ Piscicchia, K. @@aut@@ Tucakovic, I. @@aut@@ Vazquez Doce, O. @@aut@@ |
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The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Invariant Mass</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Decay Channel</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Drift Chamber</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Invariant Mass Spectrum</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Neutral Cluster</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Curceanu, C.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Piscicchia, K.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Tucakovic, I.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Vazquez Doce, O.</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">Few-body systems</subfield><subfield code="d">Wien [u.a.] : Springer, 1986</subfield><subfield code="g">55(2014), 8-10 vom: 10. 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Scordo, A. |
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Scordo, A. ddc 530 bkl 31.00 bkl 33.00 misc Invariant Mass misc Decay Channel misc Drift Chamber misc Invariant Mass Spectrum misc Neutral Cluster Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE |
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530 ASE 31.00 bkl 33.00 bkl Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE Invariant Mass (dpeaa)DE-He213 Decay Channel (dpeaa)DE-He213 Drift Chamber (dpeaa)DE-He213 Invariant Mass Spectrum (dpeaa)DE-He213 Neutral Cluster (dpeaa)DE-He213 |
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Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE |
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study of the λ(1405) resonance through its neutral and charged decay channels by amadeus at daφne |
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Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE |
| abstract |
Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. |
| abstractGer |
Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. |
| abstract_unstemmed |
Abstract The AMADEUS collaboration has the goal to perform unprecedented measurements in the field of the low-energy charged kaons-nuclei interactions, by implementing the existing KLOE detector with a dedicated setup in the inner region. The KLOE detector at DAΦNE represents a unique opportunity to perform a complete study of the Λ(1405) resonance through all its three Σπ decay channels. The importance of these measurements relies on the possibility to compare the different results for the various decay channels, investigating their contributions to the final resonance shape. In particular, one of the main differences between the neutral and charged Σπ channels is the presence of a second resonance, the Σ(1385), whose contribution to the final Λ(1405) spectra has to be evaluated and subtracted. Very promising preliminary results have been already obtained for the Σ0$ π^{0} $ decay channel to which, for isospin selection rules, the Σ(1385) resonance can not decay, and for the Σ+$ π^{−} $ decay channel analysis, and will be presented in this work. |
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Study of the Λ(1405) Resonance Through its Neutral and Charged Decay Channels by AMADEUS at DAΦNE |
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Curceanu, C. Piscicchia, K. Tucakovic, I. Vazquez Doce, O. |
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| score |
7.402112 |