Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies
In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide...
Ausführliche Beschreibung
Autor*in: |
Muzalevskii I.A. [verfasserIn] Bezbakh A.A. [verfasserIn] Nikolskii E.Yu. [verfasserIn] Chudoba V. [verfasserIn] Abakumov A.M. [verfasserIn] Krupko S.A. [verfasserIn] Belogurov S.G. [verfasserIn] Biare D. [verfasserIn] Fomichev A.S. [verfasserIn] Gazeeva E.M. [verfasserIn] Gorshkov A.V. [verfasserIn] Grigorenko L.V. [verfasserIn] Kaminski G. [verfasserIn] Kiselev O. [verfasserIn] Kostyleva D.A. [verfasserIn] Mauyey B. [verfasserIn] Mukha I. [verfasserIn] Quynh A.M. [verfasserIn] Sidorchuk S.I. [verfasserIn] Shulgina N.B. [verfasserIn] Slepnev R.S. [verfasserIn] Swiercz A. [verfasserIn] Ter-Akopian G.M. [verfasserIn] Wolski R. [verfasserIn] Zhukov M.V. [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2023 |
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Übergeordnetes Werk: |
In: EPJ Web of Conferences - EDP Sciences, 2010, 290, p 09001(2023) |
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Übergeordnetes Werk: |
volume:290, p 09001 ; year:2023 |
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DOI / URN: |
10.1051/epjconf/202329009001 |
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Katalog-ID: |
DOAJ096360275 |
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520 | |a In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. | ||
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700 | 0 | |a Mauyey B. |e verfasserin |4 aut | |
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10.1051/epjconf/202329009001 doi (DE-627)DOAJ096360275 (DE-599)DOAJ53b110ca0e234d029364d9d96b9fc228 DE-627 ger DE-627 rakwb eng QC1-999 Muzalevskii I.A. verfasserin aut Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. Physics Bezbakh A.A. verfasserin aut Nikolskii E.Yu. verfasserin aut Chudoba V. verfasserin aut Abakumov A.M. verfasserin aut Krupko S.A. verfasserin aut Belogurov S.G. verfasserin aut Biare D. verfasserin aut Fomichev A.S. verfasserin aut Gazeeva E.M. verfasserin aut Gorshkov A.V. verfasserin aut Grigorenko L.V. verfasserin aut Kaminski G. verfasserin aut Kiselev O. verfasserin aut Kostyleva D.A. verfasserin aut Mauyey B. verfasserin aut Mukha I. verfasserin aut Quynh A.M. verfasserin aut Sidorchuk S.I. verfasserin aut Shulgina N.B. verfasserin aut Slepnev R.S. verfasserin aut Swiercz A. verfasserin aut Ter-Akopian G.M. verfasserin aut Wolski R. verfasserin aut Zhukov M.V. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 09001(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 09001 year:2023 https://doi.org/10.1051/epjconf/202329009001 kostenfrei https://doaj.org/article/53b110ca0e234d029364d9d96b9fc228 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_09001.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2005 GBV_ILN_2009 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2055 GBV_ILN_2111 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 290, p 09001 2023 |
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10.1051/epjconf/202329009001 doi (DE-627)DOAJ096360275 (DE-599)DOAJ53b110ca0e234d029364d9d96b9fc228 DE-627 ger DE-627 rakwb eng QC1-999 Muzalevskii I.A. verfasserin aut Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. Physics Bezbakh A.A. verfasserin aut Nikolskii E.Yu. verfasserin aut Chudoba V. verfasserin aut Abakumov A.M. verfasserin aut Krupko S.A. verfasserin aut Belogurov S.G. verfasserin aut Biare D. verfasserin aut Fomichev A.S. verfasserin aut Gazeeva E.M. verfasserin aut Gorshkov A.V. verfasserin aut Grigorenko L.V. verfasserin aut Kaminski G. verfasserin aut Kiselev O. verfasserin aut Kostyleva D.A. verfasserin aut Mauyey B. verfasserin aut Mukha I. verfasserin aut Quynh A.M. verfasserin aut Sidorchuk S.I. verfasserin aut Shulgina N.B. verfasserin aut Slepnev R.S. verfasserin aut Swiercz A. verfasserin aut Ter-Akopian G.M. verfasserin aut Wolski R. verfasserin aut Zhukov M.V. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 09001(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 09001 year:2023 https://doi.org/10.1051/epjconf/202329009001 kostenfrei https://doaj.org/article/53b110ca0e234d029364d9d96b9fc228 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_09001.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2005 GBV_ILN_2009 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2055 GBV_ILN_2111 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 290, p 09001 2023 |
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10.1051/epjconf/202329009001 doi (DE-627)DOAJ096360275 (DE-599)DOAJ53b110ca0e234d029364d9d96b9fc228 DE-627 ger DE-627 rakwb eng QC1-999 Muzalevskii I.A. verfasserin aut Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. Physics Bezbakh A.A. verfasserin aut Nikolskii E.Yu. verfasserin aut Chudoba V. verfasserin aut Abakumov A.M. verfasserin aut Krupko S.A. verfasserin aut Belogurov S.G. verfasserin aut Biare D. verfasserin aut Fomichev A.S. verfasserin aut Gazeeva E.M. verfasserin aut Gorshkov A.V. verfasserin aut Grigorenko L.V. verfasserin aut Kaminski G. verfasserin aut Kiselev O. verfasserin aut Kostyleva D.A. verfasserin aut Mauyey B. verfasserin aut Mukha I. verfasserin aut Quynh A.M. verfasserin aut Sidorchuk S.I. verfasserin aut Shulgina N.B. verfasserin aut Slepnev R.S. verfasserin aut Swiercz A. verfasserin aut Ter-Akopian G.M. verfasserin aut Wolski R. verfasserin aut Zhukov M.V. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 09001(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 09001 year:2023 https://doi.org/10.1051/epjconf/202329009001 kostenfrei https://doaj.org/article/53b110ca0e234d029364d9d96b9fc228 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_09001.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2005 GBV_ILN_2009 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2055 GBV_ILN_2111 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 290, p 09001 2023 |
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10.1051/epjconf/202329009001 doi (DE-627)DOAJ096360275 (DE-599)DOAJ53b110ca0e234d029364d9d96b9fc228 DE-627 ger DE-627 rakwb eng QC1-999 Muzalevskii I.A. verfasserin aut Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. Physics Bezbakh A.A. verfasserin aut Nikolskii E.Yu. verfasserin aut Chudoba V. verfasserin aut Abakumov A.M. verfasserin aut Krupko S.A. verfasserin aut Belogurov S.G. verfasserin aut Biare D. verfasserin aut Fomichev A.S. verfasserin aut Gazeeva E.M. verfasserin aut Gorshkov A.V. verfasserin aut Grigorenko L.V. verfasserin aut Kaminski G. verfasserin aut Kiselev O. verfasserin aut Kostyleva D.A. verfasserin aut Mauyey B. verfasserin aut Mukha I. verfasserin aut Quynh A.M. verfasserin aut Sidorchuk S.I. verfasserin aut Shulgina N.B. verfasserin aut Slepnev R.S. verfasserin aut Swiercz A. verfasserin aut Ter-Akopian G.M. verfasserin aut Wolski R. verfasserin aut Zhukov M.V. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 09001(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 09001 year:2023 https://doi.org/10.1051/epjconf/202329009001 kostenfrei https://doaj.org/article/53b110ca0e234d029364d9d96b9fc228 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_09001.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2005 GBV_ILN_2009 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2055 GBV_ILN_2111 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 290, p 09001 2023 |
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10.1051/epjconf/202329009001 doi (DE-627)DOAJ096360275 (DE-599)DOAJ53b110ca0e234d029364d9d96b9fc228 DE-627 ger DE-627 rakwb eng QC1-999 Muzalevskii I.A. verfasserin aut Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. Physics Bezbakh A.A. verfasserin aut Nikolskii E.Yu. verfasserin aut Chudoba V. verfasserin aut Abakumov A.M. verfasserin aut Krupko S.A. verfasserin aut Belogurov S.G. verfasserin aut Biare D. verfasserin aut Fomichev A.S. verfasserin aut Gazeeva E.M. verfasserin aut Gorshkov A.V. verfasserin aut Grigorenko L.V. verfasserin aut Kaminski G. verfasserin aut Kiselev O. verfasserin aut Kostyleva D.A. verfasserin aut Mauyey B. verfasserin aut Mukha I. verfasserin aut Quynh A.M. verfasserin aut Sidorchuk S.I. verfasserin aut Shulgina N.B. verfasserin aut Slepnev R.S. verfasserin aut Swiercz A. verfasserin aut Ter-Akopian G.M. verfasserin aut Wolski R. verfasserin aut Zhukov M.V. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 09001(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 09001 year:2023 https://doi.org/10.1051/epjconf/202329009001 kostenfrei https://doaj.org/article/53b110ca0e234d029364d9d96b9fc228 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_09001.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2005 GBV_ILN_2009 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2055 GBV_ILN_2111 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 290, p 09001 2023 |
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Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies |
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Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies |
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Muzalevskii I.A. Bezbakh A.A. Nikolskii E.Yu. Chudoba V. Abakumov A.M. Krupko S.A. Belogurov S.G. Biare D. Fomichev A.S. Gazeeva E.M. Gorshkov A.V. Grigorenko L.V. Kaminski G. Kiselev O. Kostyleva D.A. Mauyey B. Mukha I. Quynh A.M. Sidorchuk S.I. Shulgina N.B. Slepnev R.S. Swiercz A. Ter-Akopian G.M. Wolski R. Zhukov M.V. |
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Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies |
abstract |
In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. |
abstractGer |
In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. |
abstract_unstemmed |
In the recent work [Nikolskii et al., Phys. Rev. C 105, 064605 (2022)] the 2H(8He,4He)6H reaction was used for the study of the extreme neutron-rich 6H isotope. A broad bump was observed in the measured 6H spectrum interpreted as the broad overlapping ground and some low-lying states of this nuclide. There could be certain doubts in the interpretation of this work: in conditions of the limited phase space it is not impossible that the structure in the missing mass spectrum of 6H is actually induced by the resonant states populated by some other channels opened in the 8He+2H interaction. This work provides a body of the evidence for the correct channel identification and for the absence of the 6H resonances at energy ET = 0 − 3.5 MeV above the 3H+3n decay threshold. In addition the first strong experimental evidence is given that the 6H → 5H*+n → 3H+3n sequential decay is the dominating 6H decay channel. |
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Interfering reaction channels observed in the 2H(8He,4He)6H reaction studies |
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https://doi.org/10.1051/epjconf/202329009001 https://doaj.org/article/53b110ca0e234d029364d9d96b9fc228 https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_09001.pdf https://doaj.org/toc/2100-014X |
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Bezbakh A.A. Nikolskii E.Yu Chudoba V. Abakumov A.M. Krupko S.A. Belogurov S.G. Biare D. Fomichev A.S. Gazeeva E.M. Gorshkov A.V. Grigorenko L.V. Kaminski G. Kiselev O. Kostyleva D.A. Mauyey B. Mukha I. Quynh A.M. Sidorchuk S.I. Shulgina N.B. Slepnev R.S. Swiercz A. Ter-Akopian G.M. Wolski R. Zhukov M.V. |
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Bezbakh A.A. Nikolskii E.Yu Chudoba V. Abakumov A.M. Krupko S.A. Belogurov S.G. Biare D. Fomichev A.S. Gazeeva E.M. Gorshkov A.V. Grigorenko L.V. Kaminski G. Kiselev O. Kostyleva D.A. Mauyey B. Mukha I. Quynh A.M. Sidorchuk S.I. Shulgina N.B. Slepnev R.S. Swiercz A. Ter-Akopian G.M. Wolski R. Zhukov M.V. |
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