Charged lepton flavor-violating transitions in color octet model

Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transit...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Li, Bin [verfasserIn] Liao, Yi [verfasserIn] Ma, Xiao-Dong [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2016

Schlagwörter:	Yukawa Coupling Neutrino Mass Matrix Inverted Hierarchy Color Octet Future Sensitivity

Übergeordnetes Werk:	Enthalten in: The European physical journal - Berlin : Springer, 1998, 76(2016), 11 vom: 09. Nov.
Übergeordnetes Werk:	volume:76 ; year:2016 ; number:11 ; day:09 ; month:11

Links:	Volltext

DOI / URN:	10.1140/epjc/s10052-016-4462-5

Katalog-ID:	SPR008348871

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matchkey_str	article:14346052:2016----::hrelpofaovoaigrniinic
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allfields	10.1140/epjc/s10052-016-4462-5 doi (DE-627)SPR008348871 (SPR)s10052-016-4462-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Li, Bin verfasserin aut Charged lepton flavor-violating transitions in color octet model 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transitions in current and future experiments. We find that for general values of parameters the branching ratios for LFV decays of the Higgs and Z bosons are far below current and even future experimental bounds. For LFV transitions of the muon, the present bounds can be satisfied generally, while future sensitivities could distinguish between the singlet and triplet color-octet fermions. The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles. Yukawa Coupling (dpeaa)DE-He213 Neutrino Mass Matrix (dpeaa)DE-He213 Inverted Hierarchy (dpeaa)DE-He213 Color Octet (dpeaa)DE-He213 Future Sensitivity (dpeaa)DE-He213 Liao, Yi verfasserin aut Ma, Xiao-Dong verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 76(2016), 11 vom: 09. Nov. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:76 year:2016 number:11 day:09 month:11 https://dx.doi.org/10.1140/epjc/s10052-016-4462-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 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 33.50 ASE AR 76 2016 11 09 11
spelling	10.1140/epjc/s10052-016-4462-5 doi (DE-627)SPR008348871 (SPR)s10052-016-4462-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Li, Bin verfasserin aut Charged lepton flavor-violating transitions in color octet model 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transitions in current and future experiments. We find that for general values of parameters the branching ratios for LFV decays of the Higgs and Z bosons are far below current and even future experimental bounds. For LFV transitions of the muon, the present bounds can be satisfied generally, while future sensitivities could distinguish between the singlet and triplet color-octet fermions. The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles. Yukawa Coupling (dpeaa)DE-He213 Neutrino Mass Matrix (dpeaa)DE-He213 Inverted Hierarchy (dpeaa)DE-He213 Color Octet (dpeaa)DE-He213 Future Sensitivity (dpeaa)DE-He213 Liao, Yi verfasserin aut Ma, Xiao-Dong verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 76(2016), 11 vom: 09. Nov. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:76 year:2016 number:11 day:09 month:11 https://dx.doi.org/10.1140/epjc/s10052-016-4462-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 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 33.50 ASE AR 76 2016 11 09 11
allfields_unstemmed	10.1140/epjc/s10052-016-4462-5 doi (DE-627)SPR008348871 (SPR)s10052-016-4462-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Li, Bin verfasserin aut Charged lepton flavor-violating transitions in color octet model 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transitions in current and future experiments. We find that for general values of parameters the branching ratios for LFV decays of the Higgs and Z bosons are far below current and even future experimental bounds. For LFV transitions of the muon, the present bounds can be satisfied generally, while future sensitivities could distinguish between the singlet and triplet color-octet fermions. The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles. Yukawa Coupling (dpeaa)DE-He213 Neutrino Mass Matrix (dpeaa)DE-He213 Inverted Hierarchy (dpeaa)DE-He213 Color Octet (dpeaa)DE-He213 Future Sensitivity (dpeaa)DE-He213 Liao, Yi verfasserin aut Ma, Xiao-Dong verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 76(2016), 11 vom: 09. Nov. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:76 year:2016 number:11 day:09 month:11 https://dx.doi.org/10.1140/epjc/s10052-016-4462-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 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 33.50 ASE AR 76 2016 11 09 11
allfieldsGer	10.1140/epjc/s10052-016-4462-5 doi (DE-627)SPR008348871 (SPR)s10052-016-4462-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Li, Bin verfasserin aut Charged lepton flavor-violating transitions in color octet model 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transitions in current and future experiments. We find that for general values of parameters the branching ratios for LFV decays of the Higgs and Z bosons are far below current and even future experimental bounds. For LFV transitions of the muon, the present bounds can be satisfied generally, while future sensitivities could distinguish between the singlet and triplet color-octet fermions. The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles. Yukawa Coupling (dpeaa)DE-He213 Neutrino Mass Matrix (dpeaa)DE-He213 Inverted Hierarchy (dpeaa)DE-He213 Color Octet (dpeaa)DE-He213 Future Sensitivity (dpeaa)DE-He213 Liao, Yi verfasserin aut Ma, Xiao-Dong verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 76(2016), 11 vom: 09. Nov. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:76 year:2016 number:11 day:09 month:11 https://dx.doi.org/10.1140/epjc/s10052-016-4462-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 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 33.50 ASE AR 76 2016 11 09 11
allfieldsSound	10.1140/epjc/s10052-016-4462-5 doi (DE-627)SPR008348871 (SPR)s10052-016-4462-5-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Li, Bin verfasserin aut Charged lepton flavor-violating transitions in color octet model 2016 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transitions in current and future experiments. We find that for general values of parameters the branching ratios for LFV decays of the Higgs and Z bosons are far below current and even future experimental bounds. For LFV transitions of the muon, the present bounds can be satisfied generally, while future sensitivities could distinguish between the singlet and triplet color-octet fermions. The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles. Yukawa Coupling (dpeaa)DE-He213 Neutrino Mass Matrix (dpeaa)DE-He213 Inverted Hierarchy (dpeaa)DE-He213 Color Octet (dpeaa)DE-He213 Future Sensitivity (dpeaa)DE-He213 Liao, Yi verfasserin aut Ma, Xiao-Dong verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 76(2016), 11 vom: 09. Nov. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:76 year:2016 number:11 day:09 month:11 https://dx.doi.org/10.1140/epjc/s10052-016-4462-5 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 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 33.50 ASE AR 76 2016 11 09 11
language	English
source	Enthalten in The European physical journal 76(2016), 11 vom: 09. Nov. volume:76 year:2016 number:11 day:09 month:11
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topic_facet	Yukawa Coupling Neutrino Mass Matrix Inverted Hierarchy Color Octet Future Sensitivity
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author	Li, Bin
spellingShingle	Li, Bin ddc 530 bkl 33.50 misc Yukawa Coupling misc Neutrino Mass Matrix misc Inverted Hierarchy misc Color Octet misc Future Sensitivity Charged lepton flavor-violating transitions in color octet model
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topic_title	530 ASE 33.50 bkl Charged lepton flavor-violating transitions in color octet model Yukawa Coupling (dpeaa)DE-He213 Neutrino Mass Matrix (dpeaa)DE-He213 Inverted Hierarchy (dpeaa)DE-He213 Color Octet (dpeaa)DE-He213 Future Sensitivity (dpeaa)DE-He213
topic	ddc 530 bkl 33.50 misc Yukawa Coupling misc Neutrino Mass Matrix misc Inverted Hierarchy misc Color Octet misc Future Sensitivity
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title	Charged lepton flavor-violating transitions in color octet model
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title_full	Charged lepton flavor-violating transitions in color octet model
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title_sort	charged lepton flavor-violating transitions in color octet model
title_auth	Charged lepton flavor-violating transitions in color octet model
abstract	Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transitions in current and future experiments. We find that for general values of parameters the branching ratios for LFV decays of the Higgs and Z bosons are far below current and even future experimental bounds. For LFV transitions of the muon, the present bounds can be satisfied generally, while future sensitivities could distinguish between the singlet and triplet color-octet fermions. The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles.
abstractGer	Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transitions in current and future experiments. We find that for general values of parameters the branching ratios for LFV decays of the Higgs and Z bosons are far below current and even future experimental bounds. For LFV transitions of the muon, the present bounds can be satisfied generally, while future sensitivities could distinguish between the singlet and triplet color-octet fermions. The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles.
abstract_unstemmed	Abstract We study charged lepton flavor-violating (LFV) transitions in the color octet model that generates neutrino mass and lepton mixing at one loop. By taking into account neutrino oscillation data and assuming octet particles of TeV scale mass, we examine the feasibility to detect these transitions in current and future experiments. We find that for general values of parameters the branching ratios for LFV decays of the Higgs and Z bosons are far below current and even future experimental bounds. For LFV transitions of the muon, the present bounds can be satisfied generally, while future sensitivities could distinguish between the singlet and triplet color-octet fermions. The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles.
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title_short	Charged lepton flavor-violating transitions in color octet model
url	https://dx.doi.org/10.1140/epjc/s10052-016-4462-5
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up_date	2024-07-03T19:36:27.551Z
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The triplet case could be ruled out by future %$\mu -e%$ conversion in nuclei, and for the singlet case the conversion and the decays %$\mu \rightarrow 3e,~e\gamma %$ play complementary roles in excluding relatively low-mass regions of the octet particles.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Yukawa Coupling</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Neutrino Mass Matrix</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Inverted Hierarchy</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Color Octet</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Future Sensitivity</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Liao, Yi</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ma, Xiao-Dong</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">The European physical journal</subfield><subfield code="d">Berlin : Springer, 1998</subfield><subfield code="g">76(2016), 11 vom: 09. 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Charged lepton flavor-violating transitions in color octet model

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