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<?xml version="1.0" encoding="UTF-8"?> <collection xmlns="http://www.loc.gov/MARC21/slim"> <record> <controlfield tag="001">2848401</controlfield> <controlfield tag="005">20231208043331.0</controlfield> <datafield tag="024" ind1="8" ind2=" "> <subfield code="a">oai:cds.cern.ch:2848401</subfield> <subfield code="p">cerncds:FULLTEXT</subfield> <subfield code="p">cerncds:CERN:FULLTEXT</subfield> <subfield code="p">cerncds:CERN</subfield> </datafield> <datafield tag="024" ind1="7" ind2=" "> <subfield code="2">DOI</subfield> <subfield code="9">APS</subfield> <subfield code="a">10.1103/PhysRevD.108.115002</subfield> <subfield code="q">publication</subfield> </datafield> <datafield tag="035" ind1=" " ind2=" "> <subfield code="9">arXiv</subfield> <subfield code="a">oai:arXiv.org:2206.01674</subfield> </datafield> <datafield tag="035" ind1=" " ind2=" "> <subfield code="a">oai:inspirehep.net:2091329</subfield> <subfield code="u">https://inspirehep.net/api/oai2d</subfield> <subfield code="9">Inspire</subfield> <subfield code="d">2023-12-07T15:42:08Z</subfield> <subfield code="h">2023-12-08T03:11:39Z</subfield> <subfield code="m">marcxml</subfield> <subfield code="t">true</subfield> </datafield> <datafield tag="035" ind1=" " ind2=" "> <subfield code="9">Inspire</subfield> <subfield code="a">2091329</subfield> </datafield> <datafield tag="037" ind1=" " ind2=" "> <subfield code="9">arXiv</subfield> <subfield code="a">arXiv:2206.01674</subfield> <subfield code="c">hep-ph</subfield> </datafield> <datafield tag="037" ind1=" " ind2=" "> <subfield code="9">arXiv:reportnumber</subfield> <subfield code="a">CERN-TH-2022-208</subfield> </datafield> <datafield tag="041" ind1=" " ind2=" "> <subfield code="a">eng</subfield> </datafield> <datafield tag="100" ind1=" " ind2=" "> <subfield code="a">Freitas, Felipe F.</subfield> <subfield code="m">felipefreitas@ua.pt</subfield> <subfield code="u">Aveiro U.</subfield> <subfield code="v">Departamento de Física, Universidade de Aveiro and CIDMA, Campus de Santiago, 3810-183 Aveiro, Portugal</subfield> </datafield> <datafield tag="245" ind1=" " ind2=" "> <subfield code="9">APS</subfield> <subfield code="a">Interplay between flavor anomalies and neutrino properties</subfield> </datafield> <datafield tag="246" ind1=" " ind2=" "> <subfield code="9">arXiv</subfield> <subfield code="a">On interplay between flavour anomalies and neutrino properties</subfield> </datafield> <datafield tag="260" ind1=" " ind2=" "> <subfield code="c">2023-12-01</subfield> </datafield> <datafield tag="269" ind1=" " ind2=" "> <subfield code="c">2022-06-03</subfield> </datafield> <datafield tag="300" ind1=" " ind2=" "> <subfield code="a">17 p</subfield> </datafield> <datafield tag="500" ind1=" " ind2=" "> <subfield code="9">arXiv</subfield> <subfield code="a">Accepted version</subfield> </datafield> <datafield tag="520" ind1=" " ind2=" "> <subfield code="9">APS</subfield> <subfield code="a">A minimal extension of the Standard Model (SM) featuring two scalar leptoquarks, an SU(2) doublet with hypercharge <math display="inline"><mrow><mn>1</mn><mo>/</mo><mn>6</mn></mrow></math> and a singlet with hypercharge <math display="inline"><mrow><mn>1</mn><mo>/</mo><mn>3</mn></mrow></math>, is proposed as an economical benchmark model for studies of an interplay between flavor physics and properties of the neutrino sector. The presence of such type of leptoquarks radiatively generates neutrino masses and offers a simultaneous explanation for the current <math display="inline"><mi>B</mi></math>-physics anomalies involving <math display="inline"><mi>b</mi><mo stretchy="false">→</mo><mi>c</mi><mo>ℓ</mo><msub><mi>ν</mi><mo>ℓ</mo></msub></math> decays. The model can also accommodate both the muon magnetic moment and the recently reported <math display="inline"><mi>W</mi></math>-mass anomalies, while complying with the most stringent lepton flavor-violating observables.</subfield> </datafield> <datafield tag="520" ind1=" " ind2=" "> <subfield code="9">arXiv</subfield> <subfield code="a">A minimal extension of the Standard Model (SM) featuring two scalar leptoquarks, an SU(2) doublet with hypercharge 1/6 and a singlet with hypercharge 1/3, is proposed as an economical benchmark model for studies of an interplay between flavour physics and properties of the neutrino sector. The presence of such type of leptoquarks radiatively generates neutrino masses and offers a simultaneous explanation for the current B-physics anomalies involving $b \to c \ell \nu_\ell$ decays. The model can also accommodate both the muon magnetic moment and the recently reported $W$ mass anomalies, while complying with the most stringent lepton flavour violating observables.</subfield> </datafield> <datafield tag="540" ind1=" " ind2=" "> <subfield code="3">preprint</subfield> <subfield code="a">CC BY 4.0</subfield> <subfield code="u">http://creativecommons.org/licenses/by/4.0/</subfield> </datafield> <datafield tag="540" ind1=" " ind2=" "> <subfield code="3">publication</subfield> <subfield code="a">CC BY 4.0</subfield> <subfield code="f">SCOAP3</subfield> <subfield code="u">https://creativecommons.org/licenses/by/4.0/</subfield> </datafield> <datafield tag="542" ind1=" " ind2=" "> <subfield code="3">publication</subfield> <subfield code="d">authors</subfield> <subfield code="g">2023</subfield> </datafield> <datafield tag="595" ind1=" " ind2="D"> <subfield code="a">3</subfield> <subfield code="d">2022-06-09</subfield> <subfield code="s">abs</subfield> </datafield> <datafield tag="595" ind1=" " ind2="D"> <subfield code="a">3</subfield> <subfield code="d">2022-06-13</subfield> <subfield code="s">printed</subfield> </datafield> <datafield tag="595" ind1=" " ind2=" "> <subfield code="a">CERN-TH</subfield> </datafield> <datafield tag="650" ind1="1" ind2="7"> <subfield code="2">arXiv</subfield> <subfield code="a">hep-ph</subfield> </datafield> <datafield tag="650" ind1="1" ind2="7"> <subfield code="2">SzGeCERN</subfield> <subfield code="a">Particle Physics - Phenomenology</subfield> </datafield> <datafield tag="690" ind1="C" ind2=" "> <subfield code="a">CERN</subfield> </datafield> <datafield tag="690" ind1="C" ind2=" "> <subfield code="a">ARTICLE</subfield> </datafield> <datafield tag="700" ind1=" " ind2=" "> <subfield code="a">Gonçalves, João</subfield> <subfield code="j">ORCID:0000-0002-9423-243X</subfield> <subfield code="m">jpedropino@ua.pt</subfield> <subfield code="u">Aveiro U.</subfield> <subfield code="v">Departamento de Física, Universidade de Aveiro and CIDMA, Campus de Santiago, 3810-183 Aveiro, Portugal</subfield> <subfield code="v">Department of Astronomy and Theoretical Physics, Lund University, 221 00 Lund, Sweden</subfield> </datafield> <datafield tag="700" ind1=" " ind2=" "> <subfield code="a">Morais, António P.</subfield> <subfield code="j">ORCID:0000-0001-7141-8162</subfield> <subfield code="m">aapmorais@ua.pt</subfield> <subfield code="u">Aveiro U.</subfield> <subfield code="u">CERN</subfield> <subfield code="v">Departamento de Física, Universidade de Aveiro and CIDMA, Campus de Santiago, 3810-183 Aveiro, Portugal</subfield> <subfield code="v">Theoretical Physics Department, CERN, 1211 Geneva 23, Switzerland</subfield> </datafield> <datafield tag="700" ind1=" " ind2=" "> <subfield code="a">Pasechnik, Roman</subfield> <subfield code="j">ORCID:0000-0003-4231-0149</subfield> <subfield code="m">Roman.Pasechnik@thep.lu.se</subfield> <subfield code="u">Lund U., Dept. 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