Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup

The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon...
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Autor*in:	De Paolis L. [verfasserIn] Bazzi M. [verfasserIn] Bosnar D. [verfasserIn] Bragadireanu M. [verfasserIn] Cargnelli M. [verfasserIn] Carminati M. [verfasserIn] Clozza A. [verfasserIn] Deda G. [verfasserIn] Del Grande R. [verfasserIn] Fabbietti L. [verfasserIn] Fiorini C. [verfasserIn] Friščić I. [verfasserIn] Guaraldo C. [verfasserIn] Iliescu M. [verfasserIn] Iwasaki M. [verfasserIn] Khreptak A. [verfasserIn] King P. [verfasserIn] Sandri P. Levi [verfasserIn] Manti S. [verfasserIn] Marton J. [verfasserIn] Miliucci M. [verfasserIn] Moskal P. [verfasserIn] Napolitano F. [verfasserIn] Niedźwiecki S. [verfasserIn] Ohnishi H. [verfasserIn] Piscicchia K. [verfasserIn] Sada Y. [verfasserIn] Scordo A. [verfasserIn] Sgaramella F. [verfasserIn] Shi H. [verfasserIn] Silarski M. [verfasserIn] Sirghi D.L. [verfasserIn] Sirghi F. [verfasserIn] Skurzok M. [verfasserIn] Spallone A. [verfasserIn] Toho K. [verfasserIn] Tüchler M. [verfasserIn] Doce O. Vazquez [verfasserIn] Yoshida C. [verfasserIn] Zmeskal J. [verfasserIn] Curceanu C. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Übergeordnetes Werk:	In: EPJ Web of Conferences - EDP Sciences, 2010, 270, p 00028(2022)
Übergeordnetes Werk:	volume:270, p 00028 ; year:2022

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc

DOI / URN:	10.1051/epjconf/202227000028

Katalog-ID:	DOAJ026020505

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allfields	10.1051/epjconf/202227000028 doi (DE-627)DOAJ026020505 (DE-599)DOAJ9faa32ae0bee4873bc084276ceee2b36 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. The result of this measurement is presented in this paper, with a specific focus on the background rejection performed by the kaon trigger system. Physics Bazzi M. verfasserin aut 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 Fabbietti L. 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 King P. verfasserin aut Sandri P. Levi 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 H. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Shi H. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Doce O. Vazquez verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 270, p 00028(2022) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:270, p 00028 year:2022 https://doi.org/10.1051/epjconf/202227000028 kostenfrei https://doaj.org/article/9faa32ae0bee4873bc084276ceee2b36 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2022/14/epjconf_qcd@work2022_00028.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA 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 270, p 00028 2022
spelling	10.1051/epjconf/202227000028 doi (DE-627)DOAJ026020505 (DE-599)DOAJ9faa32ae0bee4873bc084276ceee2b36 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. The result of this measurement is presented in this paper, with a specific focus on the background rejection performed by the kaon trigger system. Physics Bazzi M. verfasserin aut 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 Fabbietti L. 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 King P. verfasserin aut Sandri P. Levi 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 H. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Shi H. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Doce O. Vazquez verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 270, p 00028(2022) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:270, p 00028 year:2022 https://doi.org/10.1051/epjconf/202227000028 kostenfrei https://doaj.org/article/9faa32ae0bee4873bc084276ceee2b36 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2022/14/epjconf_qcd@work2022_00028.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA 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 270, p 00028 2022
allfields_unstemmed	10.1051/epjconf/202227000028 doi (DE-627)DOAJ026020505 (DE-599)DOAJ9faa32ae0bee4873bc084276ceee2b36 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. The result of this measurement is presented in this paper, with a specific focus on the background rejection performed by the kaon trigger system. Physics Bazzi M. verfasserin aut 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 Fabbietti L. 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 King P. verfasserin aut Sandri P. Levi 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 H. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Shi H. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Doce O. Vazquez verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 270, p 00028(2022) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:270, p 00028 year:2022 https://doi.org/10.1051/epjconf/202227000028 kostenfrei https://doaj.org/article/9faa32ae0bee4873bc084276ceee2b36 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2022/14/epjconf_qcd@work2022_00028.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA 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 270, p 00028 2022
allfieldsGer	10.1051/epjconf/202227000028 doi (DE-627)DOAJ026020505 (DE-599)DOAJ9faa32ae0bee4873bc084276ceee2b36 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. The result of this measurement is presented in this paper, with a specific focus on the background rejection performed by the kaon trigger system. Physics Bazzi M. verfasserin aut 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 Fabbietti L. 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 King P. verfasserin aut Sandri P. Levi 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 H. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Shi H. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Doce O. Vazquez verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 270, p 00028(2022) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:270, p 00028 year:2022 https://doi.org/10.1051/epjconf/202227000028 kostenfrei https://doaj.org/article/9faa32ae0bee4873bc084276ceee2b36 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2022/14/epjconf_qcd@work2022_00028.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA 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 270, p 00028 2022
allfieldsSound	10.1051/epjconf/202227000028 doi (DE-627)DOAJ026020505 (DE-599)DOAJ9faa32ae0bee4873bc084276ceee2b36 DE-627 ger DE-627 rakwb eng QC1-999 De Paolis L. verfasserin aut Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. The result of this measurement is presented in this paper, with a specific focus on the background rejection performed by the kaon trigger system. Physics Bazzi M. verfasserin aut 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 Fabbietti L. 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 King P. verfasserin aut Sandri P. Levi 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 H. verfasserin aut Piscicchia K. verfasserin aut Sada Y. verfasserin aut Scordo A. verfasserin aut Sgaramella F. verfasserin aut Shi H. verfasserin aut Silarski M. verfasserin aut Sirghi D.L. verfasserin aut Sirghi F. verfasserin aut Skurzok M. verfasserin aut Spallone A. verfasserin aut Toho K. verfasserin aut Tüchler M. verfasserin aut Doce O. Vazquez verfasserin aut Yoshida C. verfasserin aut Zmeskal J. verfasserin aut Curceanu C. verfasserin aut In EPJ Web of Conferences EDP Sciences, 2010 270, p 00028(2022) (DE-627)647306611 (DE-600)2595425-8 2100014X nnns volume:270, p 00028 year:2022 https://doi.org/10.1051/epjconf/202227000028 kostenfrei https://doaj.org/article/9faa32ae0bee4873bc084276ceee2b36 kostenfrei https://www.epj-conferences.org/articles/epjconf/pdf/2022/14/epjconf_qcd@work2022_00028.pdf kostenfrei https://doaj.org/toc/2100-014X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA 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 270, p 00028 2022
language	English
source	In EPJ Web of Conferences 270, p 00028(2022) volume:270, p 00028 year:2022
sourceStr	In EPJ Web of Conferences 270, p 00028(2022) volume:270, p 00028 year:2022
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Physics
isfreeaccess_bool	true
container_title	EPJ Web of Conferences
authorswithroles_txt_mv	De Paolis L. @@aut@@ Bazzi M. @@aut@@ Bosnar D. @@aut@@ Bragadireanu M. @@aut@@ Cargnelli M. @@aut@@ Carminati M. @@aut@@ Clozza A. @@aut@@ Deda G. @@aut@@ Del Grande R. @@aut@@ Fabbietti L. @@aut@@ Fiorini C. @@aut@@ Friščić I. @@aut@@ Guaraldo C. @@aut@@ Iliescu M. @@aut@@ Iwasaki M. @@aut@@ Khreptak A. @@aut@@ King P. @@aut@@ Sandri P. Levi @@aut@@ Manti S. @@aut@@ Marton J. @@aut@@ Miliucci M. @@aut@@ Moskal P. @@aut@@ Napolitano F. @@aut@@ Niedźwiecki S. @@aut@@ Ohnishi H. @@aut@@ Piscicchia K. @@aut@@ Sada Y. @@aut@@ Scordo A. @@aut@@ Sgaramella F. @@aut@@ Shi H. @@aut@@ Silarski M. @@aut@@ Sirghi D.L. @@aut@@ Sirghi F. @@aut@@ Skurzok M. @@aut@@ Spallone A. @@aut@@ Toho K. @@aut@@ Tüchler M. @@aut@@ Doce O. Vazquez @@aut@@ Yoshida C. @@aut@@ Zmeskal J. @@aut@@ Curceanu C. @@aut@@
publishDateDaySort_date	2022-01-01T00:00:00Z
hierarchy_top_id	647306611
id	DOAJ026020505
language_de	englisch
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callnumber-first	Q - Science
author	De Paolis L.
spellingShingle	De Paolis L. misc QC1-999 misc Physics Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup
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topic_title	QC1-999 Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup
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title	Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup
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title_full	Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup
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author_browse	De Paolis L. Bazzi M. Bosnar D. Bragadireanu M. Cargnelli M. Carminati M. Clozza A. Deda G. Del Grande R. Fabbietti L. Fiorini C. Friščić I. Guaraldo C. Iliescu M. Iwasaki M. Khreptak A. King P. Sandri P. Levi Manti S. Marton J. Miliucci M. Moskal P. Napolitano F. Niedźwiecki S. Ohnishi H. Piscicchia K. Sada Y. Scordo A. Sgaramella F. Shi H. Silarski M. Sirghi D.L. Sirghi F. Skurzok M. Spallone A. Toho K. Tüchler M. Doce O. Vazquez Yoshida C. Zmeskal J. Curceanu C.
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title_sort	trigger rejection factor in the first kaonic helium run with the complete siddharta-2 setup
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title_auth	Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup
abstract	The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. The result of this measurement is presented in this paper, with a specific focus on the background rejection performed by the kaon trigger system.
abstractGer	The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. The result of this measurement is presented in this paper, with a specific focus on the background rejection performed by the kaon trigger system.
abstract_unstemmed	The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. The result of this measurement is presented in this paper, with a specific focus on the background rejection performed by the kaon trigger system.
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title_short	Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup
url	https://doi.org/10.1051/epjconf/202227000028 https://doaj.org/article/9faa32ae0bee4873bc084276ceee2b36 https://www.epj-conferences.org/articles/epjconf/pdf/2022/14/epjconf_qcd@work2022_00028.pdf https://doaj.org/toc/2100-014X
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up_date	2024-07-03T18:33:26.380Z
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fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">DOAJ026020505</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230502073658.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230226s2022 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1051/epjconf/202227000028</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ026020505</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ9faa32ae0bee4873bc084276ceee2b36</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">QC1-999</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">De Paolis L.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">The SIDDHARTA-2 experiment aims to perform the first measurement of the kaonic deuterium 2p → 1s x-ray transition energy. Such measurement, together with the measurement of kaonic hydrogen 2p → 1s x-ray energy transition performed by the SIDDHARTA experiment in 2011, allows the determination of kaon proton and kaon neutron scattering lengths and represents a fundamental input for the low energies QCD in the strangeness sector theory. The SIDDHARTA-2 experiment is presently installed at the DAΦNE electronpositron collider at the National Laboratories of Frascati, in Italy. In May 2022, the kaonic 4He x-ray transitions measurement was performed by the complete SIDDHARTA-2 setup, by using a gaseous target. 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Trigger rejection factor in the first kaonic helium run with the complete SIDDHARTA-2 setup

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