On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark
Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Paryev, E.Ya. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2023 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Nuclear physics |
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| Übergeordnetes Werk: |
volume:1037 |
| DOI / URN: |
10.1016/j.nuclphysa.2023.122687 |
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| Katalog-ID: |
ELV059986891 |
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| 100 | 1 | |a Paryev, E.Ya. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark |
| 264 | 1 | |c 2023 | |
| 336 | |a nicht spezifiziert |b zzz |2 rdacontent | ||
| 337 | |a Computermedien |b c |2 rdamedia | ||
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| 520 | |a Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... | ||
| 650 | 4 | |a Antikaon-induced reactions | |
| 650 | 4 | |a Hidden-charm strange pentaquarks | |
| 650 | 4 | |a Charmonium production | |
| 773 | 0 | 8 | |i Enthalten in |t Nuclear physics <Amsterdam> / A |d Amsterdam : North-Holland Publ. Co., 1967 |g 1037 |h Online-Ressource |w (DE-627)266014755 |w (DE-600)1466542-6 |w (DE-576)074959778 |x 1873-1554 |7 nnns |
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| 936 | b | k | |a 33.40 |j Kernphysik |q VZ |
| 936 | b | k | |a 33.50 |j Physik der Elementarteilchen und Felder: Allgemeines |q VZ |
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10.1016/j.nuclphysa.2023.122687 doi (DE-627)ELV059986891 (ELSEVIER)S0375-9474(23)00090-8 DE-627 ger DE-627 rda eng 530 VZ 33.40 bkl 33.50 bkl Paryev, E.Ya. verfasserin aut On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... Antikaon-induced reactions Hidden-charm strange pentaquarks Charmonium production Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 1037 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:1037 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 Kernphysik VZ 33.50 Physik der Elementarteilchen und Felder: Allgemeines VZ AR 1037 |
| spelling |
10.1016/j.nuclphysa.2023.122687 doi (DE-627)ELV059986891 (ELSEVIER)S0375-9474(23)00090-8 DE-627 ger DE-627 rda eng 530 VZ 33.40 bkl 33.50 bkl Paryev, E.Ya. verfasserin aut On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... Antikaon-induced reactions Hidden-charm strange pentaquarks Charmonium production Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 1037 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:1037 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 Kernphysik VZ 33.50 Physik der Elementarteilchen und Felder: Allgemeines VZ AR 1037 |
| allfields_unstemmed |
10.1016/j.nuclphysa.2023.122687 doi (DE-627)ELV059986891 (ELSEVIER)S0375-9474(23)00090-8 DE-627 ger DE-627 rda eng 530 VZ 33.40 bkl 33.50 bkl Paryev, E.Ya. verfasserin aut On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... Antikaon-induced reactions Hidden-charm strange pentaquarks Charmonium production Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 1037 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:1037 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 Kernphysik VZ 33.50 Physik der Elementarteilchen und Felder: Allgemeines VZ AR 1037 |
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10.1016/j.nuclphysa.2023.122687 doi (DE-627)ELV059986891 (ELSEVIER)S0375-9474(23)00090-8 DE-627 ger DE-627 rda eng 530 VZ 33.40 bkl 33.50 bkl Paryev, E.Ya. verfasserin aut On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... Antikaon-induced reactions Hidden-charm strange pentaquarks Charmonium production Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 1037 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:1037 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 Kernphysik VZ 33.50 Physik der Elementarteilchen und Felder: Allgemeines VZ AR 1037 |
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10.1016/j.nuclphysa.2023.122687 doi (DE-627)ELV059986891 (ELSEVIER)S0375-9474(23)00090-8 DE-627 ger DE-627 rda eng 530 VZ 33.40 bkl 33.50 bkl Paryev, E.Ya. verfasserin aut On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... Antikaon-induced reactions Hidden-charm strange pentaquarks Charmonium production Enthalten in Nuclear physics <Amsterdam> / A Amsterdam : North-Holland Publ. Co., 1967 1037 Online-Ressource (DE-627)266014755 (DE-600)1466542-6 (DE-576)074959778 1873-1554 nnns volume:1037 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 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_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 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_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 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_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 Kernphysik VZ 33.50 Physik der Elementarteilchen und Felder: Allgemeines VZ AR 1037 |
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Paryev, E.Ya. ddc 530 bkl 33.40 bkl 33.50 misc Antikaon-induced reactions misc Hidden-charm strange pentaquarks misc Charmonium production On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark |
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530 VZ 33.40 bkl 33.50 bkl On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark Antikaon-induced reactions Hidden-charm strange pentaquarks Charmonium production |
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on the possibility of testing the two-peak structure of the lhcb hidden-charm strange pentaquark |
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On the possibility of testing the two-peak structure of the LHCb hidden-charm strange pentaquark |
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Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... |
| abstractGer |
Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... |
| abstract_unstemmed |
Accounting for the LHCb observation that the reported hidden-charm strange pentaquark P c s ( 4459 ) 0 can split into two substructures, P c s ( 4455 ) 0 and P c s ( 4468 ) 0 , with a mass difference of 13 MeV as well as the newly observed hidden-charm pentaquark resonance P c s ( 4338 ) 0 with strangeness, we study within the double-peak scenario for the P c s ( 4459 ) 0 state the near-threshold J / ψ meson production from protons and nuclei by considering incoherent direct non-resonant ( K − p → J / ψ Λ ) and two-step resonant ( K − p → P c s i 0 → J / ψ Λ , i = 1 , 2, 3; P c s 1 0 = P c s ( 4338 ) 0 , P c s 2 0 = P c s ( 4455 ) 0 , P c s 3 0 = P c s ( 4468 ) 0 ) charmonium production processes with the main goal of clarifying the possibility to observe within this scenario both above two substructures contributing to the P c s ( 4459 ) 0 state and the P c s ( 4338 ) 0 resonance in this production. We calculate the absolute excitation functions, energy and momentum distributions for the non-resonant, resonant and for the combined (non-resonant plus resonant) production of J / ψ mesons on protons as well as on carbon and tungsten target nuclei at near-threshold incident antikaon beam momenta by assuming the spin-parity assignments of the hidden-charm resonances P c s ( 4338 ) 0 , P c s ( 4455 ) 0 and P c s ( 4468 ) 0 as J P = ( 1 ... |
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|
| score |
7.400667 |