Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal

The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction betwe...
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Autor*in:	De Paolis L. [verfasserIn] Bosnar D. [verfasserIn] Bragadireanu M. [verfasserIn] Cargnelli M. [verfasserIn] Carminati M. [verfasserIn] Clozza A. [verfasserIn] Deda G. [verfasserIn] Del Grande R. [verfasserIn] Dulski K. [verfasserIn] Fiorini C. [verfasserIn] Friščić I. [verfasserIn] Guaraldo C. [verfasserIn] Iliescu M. [verfasserIn] Iwasaki M. [verfasserIn] Khreptak A. [verfasserIn] Manti S. [verfasserIn] Marton J. [verfasserIn] Miliucci M. [verfasserIn] Moskal P. [verfasserIn] Napolitano F. [verfasserIn] Niedźwiecki S. [verfasserIn] Ohnishi O. [verfasserIn] Piscicchia K. [verfasserIn] Sada Y. [verfasserIn] Scordo A. [verfasserIn] Sgaramella F. [verfasserIn] Silarski M. [verfasserIn] Sirghi D.L. [verfasserIn] Sirghi F. [verfasserIn] Skurzok M. [verfasserIn] Wycech S. [verfasserIn] Spallone A. [verfasserIn] Toho K. [verfasserIn] Tüchler M. [verfasserIn] Yoshida C. [verfasserIn] Zmeskal J. [verfasserIn] Curceanu C. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2023

Übergeordnetes Werk:	In: EPJ Web of Conferences - EDP Sciences, 2010, 290, p 06003(2023)
Übergeordnetes Werk:	volume:290, p 06003 ; year:2023

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc

DOI / URN:	10.1051/epjconf/202329006003

Katalog-ID:	DOAJ096359978

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520			\|a The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions.
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allfields	10.1051/epjconf/202329006003 doi (DE-627)DOAJ096359978 (DE-599)DOAJc7665b8662224ddb8501415577722ad7 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions. Physics Bosnar D. verfasserin aut Bragadireanu M. verfasserin aut Cargnelli M. verfasserin aut Carminati M. verfasserin aut Clozza A. verfasserin aut Deda G. verfasserin aut Del Grande R. verfasserin aut Dulski K. verfasserin aut Fiorini C. verfasserin aut Friščić I. verfasserin aut Guaraldo C. verfasserin aut Iliescu M. verfasserin aut Iwasaki M. verfasserin aut Khreptak A. verfasserin aut Manti S. verfasserin aut Marton J. verfasserin aut Miliucci M. verfasserin aut Moskal P. verfasserin aut Napolitano F. verfasserin aut Niedźwiecki S. verfasserin aut Ohnishi O. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Wycech S. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 06003(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 06003 year:2023 https://doi.org/10.1051/epjconf/202329006003 kostenfrei https://doaj.org/article/c7665b8662224ddb8501415577722ad7 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_06003.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 06003 2023
spelling	10.1051/epjconf/202329006003 doi (DE-627)DOAJ096359978 (DE-599)DOAJc7665b8662224ddb8501415577722ad7 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions. Physics Bosnar D. verfasserin aut Bragadireanu M. verfasserin aut Cargnelli M. verfasserin aut Carminati M. verfasserin aut Clozza A. verfasserin aut Deda G. verfasserin aut Del Grande R. verfasserin aut Dulski K. verfasserin aut Fiorini C. verfasserin aut Friščić I. verfasserin aut Guaraldo C. verfasserin aut Iliescu M. verfasserin aut Iwasaki M. verfasserin aut Khreptak A. verfasserin aut Manti S. verfasserin aut Marton J. verfasserin aut Miliucci M. verfasserin aut Moskal P. verfasserin aut Napolitano F. verfasserin aut Niedźwiecki S. verfasserin aut Ohnishi O. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Wycech S. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 06003(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 06003 year:2023 https://doi.org/10.1051/epjconf/202329006003 kostenfrei https://doaj.org/article/c7665b8662224ddb8501415577722ad7 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_06003.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 06003 2023
allfields_unstemmed	10.1051/epjconf/202329006003 doi (DE-627)DOAJ096359978 (DE-599)DOAJc7665b8662224ddb8501415577722ad7 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions. Physics Bosnar D. verfasserin aut Bragadireanu M. verfasserin aut Cargnelli M. verfasserin aut Carminati M. verfasserin aut Clozza A. verfasserin aut Deda G. verfasserin aut Del Grande R. verfasserin aut Dulski K. verfasserin aut Fiorini C. verfasserin aut Friščić I. verfasserin aut Guaraldo C. verfasserin aut Iliescu M. verfasserin aut Iwasaki M. verfasserin aut Khreptak A. verfasserin aut Manti S. verfasserin aut Marton J. verfasserin aut Miliucci M. verfasserin aut Moskal P. verfasserin aut Napolitano F. verfasserin aut Niedźwiecki S. verfasserin aut Ohnishi O. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Wycech S. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 06003(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 06003 year:2023 https://doi.org/10.1051/epjconf/202329006003 kostenfrei https://doaj.org/article/c7665b8662224ddb8501415577722ad7 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_06003.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 06003 2023
allfieldsGer	10.1051/epjconf/202329006003 doi (DE-627)DOAJ096359978 (DE-599)DOAJc7665b8662224ddb8501415577722ad7 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions. Physics Bosnar D. verfasserin aut Bragadireanu M. verfasserin aut Cargnelli M. verfasserin aut Carminati M. verfasserin aut Clozza A. verfasserin aut Deda G. verfasserin aut Del Grande R. verfasserin aut Dulski K. verfasserin aut Fiorini C. verfasserin aut Friščić I. verfasserin aut Guaraldo C. verfasserin aut Iliescu M. verfasserin aut Iwasaki M. verfasserin aut Khreptak A. verfasserin aut Manti S. verfasserin aut Marton J. verfasserin aut Miliucci M. verfasserin aut Moskal P. verfasserin aut Napolitano F. verfasserin aut Niedźwiecki S. verfasserin aut Ohnishi O. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Wycech S. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 06003(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 06003 year:2023 https://doi.org/10.1051/epjconf/202329006003 kostenfrei https://doaj.org/article/c7665b8662224ddb8501415577722ad7 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_06003.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 06003 2023
allfieldsSound	10.1051/epjconf/202329006003 doi (DE-627)DOAJ096359978 (DE-599)DOAJc7665b8662224ddb8501415577722ad7 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions. Physics Bosnar D. verfasserin aut Bragadireanu M. verfasserin aut Cargnelli M. verfasserin aut Carminati M. verfasserin aut Clozza A. verfasserin aut Deda G. verfasserin aut Del Grande R. verfasserin aut Dulski K. verfasserin aut Fiorini C. verfasserin aut Friščić I. verfasserin aut Guaraldo C. verfasserin aut Iliescu M. verfasserin aut Iwasaki M. verfasserin aut Khreptak A. verfasserin aut Manti S. verfasserin aut Marton J. verfasserin aut Miliucci M. verfasserin aut Moskal P. verfasserin aut Napolitano F. verfasserin aut Niedźwiecki S. verfasserin aut Ohnishi O. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Wycech S. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 290, p 06003(2023) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:290, p 06003 year:2023 https://doi.org/10.1051/epjconf/202329006003 kostenfrei https://doaj.org/article/c7665b8662224ddb8501415577722ad7 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_06003.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 06003 2023
language	English
source	In EPJ Web of Conferences 290, p 06003(2023) volume:290, p 06003 year:2023
sourceStr	In EPJ Web of Conferences 290, p 06003(2023) volume:290, p 06003 year:2023
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container_title	EPJ Web of Conferences
authorswithroles_txt_mv	De Paolis L. @@aut@@ Bosnar D. @@aut@@ Bragadireanu M. @@aut@@ Cargnelli M. @@aut@@ Carminati M. @@aut@@ Clozza A. @@aut@@ Deda G. @@aut@@ Del Grande R. @@aut@@ Dulski K. @@aut@@ Fiorini C. @@aut@@ Friščić I. @@aut@@ Guaraldo C. @@aut@@ Iliescu M. @@aut@@ Iwasaki M. @@aut@@ Khreptak A. @@aut@@ Manti S. @@aut@@ Marton J. @@aut@@ Miliucci M. @@aut@@ Moskal P. @@aut@@ Napolitano F. @@aut@@ Niedźwiecki S. @@aut@@ Ohnishi O. @@aut@@ Piscicchia K. @@aut@@ Sada Y. @@aut@@ Scordo A. @@aut@@ Sgaramella F. @@aut@@ Silarski M. @@aut@@ Sirghi D.L. @@aut@@ Sirghi F. @@aut@@ Skurzok M. @@aut@@ Wycech S. @@aut@@ Spallone A. @@aut@@ Toho K. @@aut@@ Tüchler M. @@aut@@ Yoshida C. @@aut@@ Zmeskal J. @@aut@@ Curceanu C. @@aut@@
publishDateDaySort_date	2023-01-01T00:00:00Z
hierarchy_top_id	647306611
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callnumber-first	Q - Science
author	De Paolis L.
spellingShingle	De Paolis L. misc QC1-999 misc Physics Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal
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topic_title	QC1-999 Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal
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title	Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal
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title_full	Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal
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author_browse	De Paolis L. Bosnar D. Bragadireanu M. Cargnelli M. Carminati M. Clozza A. Deda G. Del Grande R. Dulski K. Fiorini C. Friščić I. Guaraldo C. Iliescu M. Iwasaki M. Khreptak A. Manti S. Marton J. Miliucci M. Moskal P. Napolitano F. Niedźwiecki S. Ohnishi O. Piscicchia K. Sada Y. Scordo A. Sgaramella F. Silarski M. Sirghi D.L. Sirghi F. Skurzok M. Wycech S. Spallone A. Toho K. Tüchler M. Yoshida C. Zmeskal J. Curceanu C.
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title_sort	investigating the e2 nuclear resonance effects in kaonic atoms: the kameo proposal
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title_auth	Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal
abstract	The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions.
abstractGer	The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions.
abstract_unstemmed	The E2 nuclear resonance effect in kaonic atoms occurs when the energy of atomic de-excitation closely matches the energy of nuclear excitation, leading to the attenuation of some X-ray lines in the resonant isotope target. This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. In addition, a non-resonant 9242Mo isotope solid strip target will be used as a reference for standard non-resonant transitions.
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title_short	Investigating the E2 Nuclear Resonance Effects in Kaonic Atoms: The KAMEO Proposal
url	https://doi.org/10.1051/epjconf/202329006003 https://doaj.org/article/c7665b8662224ddb8501415577722ad7 https://www.epj-conferences.org/articles/epjconf/pdf/2023/16/epjconf_eunpc2023_06003.pdf https://doaj.org/toc/2100-014X
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author2	Bosnar D. Bragadireanu M. Cargnelli M. Carminati M. Clozza A. Deda G. Del Grande R. Dulski K. Fiorini C. Friščić I. Guaraldo C. Iliescu M. Iwasaki M. Khreptak A. Manti S. Marton J. Miliucci M. Moskal P. Napolitano F. Niedźwiecki S. Ohnishi O. Piscicchia K. Sada Y. Scordo A. Sgaramella F. Silarski M. Sirghi D.L. Sirghi F. Skurzok M. Wycech S. Spallone A. Toho K. Tüchler M. Yoshida C. Zmeskal J. Curceanu C.
author2Str	Bosnar D. Bragadireanu M. Cargnelli M. Carminati M. Clozza A. Deda G. Del Grande R. Dulski K. Fiorini C. Friščić I. Guaraldo C. Iliescu M. Iwasaki M. Khreptak A. Manti S. Marton J. Miliucci M. Moskal P. Napolitano F. Niedźwiecki S. Ohnishi O. Piscicchia K. Sada Y. Scordo A. Sgaramella F. Silarski M. Sirghi D.L. Sirghi F. Skurzok M. Wycech S. Spallone A. Toho K. Tüchler M. Yoshida C. Zmeskal J. Curceanu C.
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This phenomenon provides crucial information on the strong interaction between kaons and nuclei. The only nuclear E2 resonance effect observed so far was in the K− −9842Mo isotope, measured by G. L. Goldfrey, G-K. Lum, and C. E. Wiegand at Lawrence Berkeley Laboratory in 1975. However, the 25 hours of data taking were not sufficient to yield conclusive results. In four kaonic Molybdenum isotopes (9442Mo, 9642Mo, 9842and Mo, and 10042Mo), the nuclear E2 resonance effect is expected to occur at the same transition with similar energy values. To investigate this, the KAMEO (Kaonic Atoms Measuring Nuclear Resonance Effects Observables) experiment plans to conduct research on kaonic Molybdenum isotopes at the DAΦNE e+e− collider during the SIDDHARTA-2 experiment. The experimental strategy involves exposing four solid strip targets, each enriched with one Molybdenum isotope, to negatively charged kaons and using a germanium detector to measure X-ray transitions. 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