V.V. Vien , H.N. Long , A.E. Cárcamo Hernández , Juan Marchant González
{"title":"Q6 味 2HDM 中的费米子质量和混合以及 g - 2 μ介子反常现象","authors":"V.V. Vien , H.N. Long , A.E. Cárcamo Hernández , Juan Marchant González","doi":"10.1016/j.nuclphysb.2024.116722","DOIUrl":null,"url":null,"abstract":"<div><div>We propose an extended 2HDM with <span><math><msub><mrow><mi>Q</mi></mrow><mrow><mn>6</mn></mrow></msub><mo>×</mo><msub><mrow><mi>Z</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>×</mo><msub><mrow><mi>Z</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> symmetry that can successfully accommodate the SM fermion mass and mixing hierarchy. The tiny masses of the active neutrinos are generated from a type-I seesaw mechanism mediated by very heavy right-handed Majorana neutrinos. The model gives a natural explanation of the charged lepton mass hierarchy. Besides that, the experimental values of the physical observables of the neutrino sector: the neutrino mass squared splittings, the leptonic mixing angles and the leptonic Dirac CP violating phase, are also successfully reproduced for both normal and inverted neutrino mass hierarchies. We find a feasible range of values for the leptonic Dirac CP phase to be in the ranges <span><math><msub><mrow><mi>δ</mi></mrow><mrow><mi>C</mi><mi>P</mi></mrow></msub><mo>∈</mo><msup><mrow><mo>(</mo><mn>305.90</mn><mo>,</mo><mn>348.70</mn><mo>)</mo></mrow><mrow><mo>∘</mo></mrow></msup></math></span> for normal ordering and <span><math><msub><mrow><mi>δ</mi></mrow><mrow><mi>C</mi><mi>P</mi></mrow></msub><mo>∈</mo><msup><mrow><mo>(</mo><mn>308.00</mn><mo>,</mo><mn>348.00</mn><mo>)</mo></mrow><mrow><mo>∘</mo></mrow></msup></math></span> for inverted ordering, which is consistent with the 3<em>σ</em> experimentally allowed limits. The sum of neutrino masses is obtained as <span><math><mo>∑</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>∈</mo><mo>(</mo><mn>58.03</mn><mo>,</mo><mn>60.51</mn><mo>)</mo></math></span> meV for normal ordering and <span><math><mo>∑</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>∈</mo><mo>(</mo><mn>98.07</mn><mo>,</mo><mn>101.40</mn><mo>)</mo></math></span> meV for inverted ordering which are well consistent with all the recent limits. In addition, the obtained ranges for the effective neutrino masses are <span><math><mo>〈</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>e</mi><mi>e</mi></mrow></msub><mo>〉</mo><mo>∈</mo><mo>(</mo><mn>3.80</mn><mo>,</mo><mn>4.38</mn><mo>)</mo></math></span> meV, <span><math><msub><mrow><mi>m</mi></mrow><mrow><mi>β</mi></mrow></msub><mo>∈</mo><mo>(</mo><mn>8.53</mn><mo>,</mo><mn>9.34</mn><mo>)</mo><mspace></mspace><mtext>meV</mtext></math></span> for normal ordering and <span><math><mo>〈</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>e</mi><mi>e</mi></mrow></msub><mo>〉</mo><mo>∈</mo><mo>(</mo><mn>47.85</mn><mo>,</mo><mn>49.58</mn><mo>)</mo></math></span> meV, <span><math><msub><mrow><mi>m</mi></mrow><mrow><mi>β</mi></mrow></msub><mo>∈</mo><mo>(</mo><mn>48.39</mn><mo>,</mo><mn>50.09</mn><mo>)</mo><mspace></mspace><mtext>meV</mtext></math></span> for inverted ordering which are in agreement with the recent experimental bounds. For the quark sector, the derived results are also in agreement with the recent data on the quark masses and mixing angles. The model under consideration can also accommodate the muon anomalous magnetic moment.</div></div>","PeriodicalId":54712,"journal":{"name":"Nuclear Physics B","volume":"1008 ","pages":"Article 116722"},"PeriodicalIF":2.5000,"publicationDate":"2024-10-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Fermion masses and mixings and g − 2 muon anomaly in a Q6 flavored 2HDM\",\"authors\":\"V.V. Vien , H.N. Long , A.E. Cárcamo Hernández , Juan Marchant González\",\"doi\":\"10.1016/j.nuclphysb.2024.116722\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We propose an extended 2HDM with <span><math><msub><mrow><mi>Q</mi></mrow><mrow><mn>6</mn></mrow></msub><mo>×</mo><msub><mrow><mi>Z</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>×</mo><msub><mrow><mi>Z</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span> symmetry that can successfully accommodate the SM fermion mass and mixing hierarchy. The tiny masses of the active neutrinos are generated from a type-I seesaw mechanism mediated by very heavy right-handed Majorana neutrinos. The model gives a natural explanation of the charged lepton mass hierarchy. Besides that, the experimental values of the physical observables of the neutrino sector: the neutrino mass squared splittings, the leptonic mixing angles and the leptonic Dirac CP violating phase, are also successfully reproduced for both normal and inverted neutrino mass hierarchies. We find a feasible range of values for the leptonic Dirac CP phase to be in the ranges <span><math><msub><mrow><mi>δ</mi></mrow><mrow><mi>C</mi><mi>P</mi></mrow></msub><mo>∈</mo><msup><mrow><mo>(</mo><mn>305.90</mn><mo>,</mo><mn>348.70</mn><mo>)</mo></mrow><mrow><mo>∘</mo></mrow></msup></math></span> for normal ordering and <span><math><msub><mrow><mi>δ</mi></mrow><mrow><mi>C</mi><mi>P</mi></mrow></msub><mo>∈</mo><msup><mrow><mo>(</mo><mn>308.00</mn><mo>,</mo><mn>348.00</mn><mo>)</mo></mrow><mrow><mo>∘</mo></mrow></msup></math></span> for inverted ordering, which is consistent with the 3<em>σ</em> experimentally allowed limits. The sum of neutrino masses is obtained as <span><math><mo>∑</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>∈</mo><mo>(</mo><mn>58.03</mn><mo>,</mo><mn>60.51</mn><mo>)</mo></math></span> meV for normal ordering and <span><math><mo>∑</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>∈</mo><mo>(</mo><mn>98.07</mn><mo>,</mo><mn>101.40</mn><mo>)</mo></math></span> meV for inverted ordering which are well consistent with all the recent limits. In addition, the obtained ranges for the effective neutrino masses are <span><math><mo>〈</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>e</mi><mi>e</mi></mrow></msub><mo>〉</mo><mo>∈</mo><mo>(</mo><mn>3.80</mn><mo>,</mo><mn>4.38</mn><mo>)</mo></math></span> meV, <span><math><msub><mrow><mi>m</mi></mrow><mrow><mi>β</mi></mrow></msub><mo>∈</mo><mo>(</mo><mn>8.53</mn><mo>,</mo><mn>9.34</mn><mo>)</mo><mspace></mspace><mtext>meV</mtext></math></span> for normal ordering and <span><math><mo>〈</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>e</mi><mi>e</mi></mrow></msub><mo>〉</mo><mo>∈</mo><mo>(</mo><mn>47.85</mn><mo>,</mo><mn>49.58</mn><mo>)</mo></math></span> meV, <span><math><msub><mrow><mi>m</mi></mrow><mrow><mi>β</mi></mrow></msub><mo>∈</mo><mo>(</mo><mn>48.39</mn><mo>,</mo><mn>50.09</mn><mo>)</mo><mspace></mspace><mtext>meV</mtext></math></span> for inverted ordering which are in agreement with the recent experimental bounds. For the quark sector, the derived results are also in agreement with the recent data on the quark masses and mixing angles. The model under consideration can also accommodate the muon anomalous magnetic moment.</div></div>\",\"PeriodicalId\":54712,\"journal\":{\"name\":\"Nuclear Physics B\",\"volume\":\"1008 \",\"pages\":\"Article 116722\"},\"PeriodicalIF\":2.5000,\"publicationDate\":\"2024-10-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Physics B\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0550321324002888\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Physics B","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0550321324002888","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
Fermion masses and mixings and g − 2 muon anomaly in a Q6 flavored 2HDM
We propose an extended 2HDM with symmetry that can successfully accommodate the SM fermion mass and mixing hierarchy. The tiny masses of the active neutrinos are generated from a type-I seesaw mechanism mediated by very heavy right-handed Majorana neutrinos. The model gives a natural explanation of the charged lepton mass hierarchy. Besides that, the experimental values of the physical observables of the neutrino sector: the neutrino mass squared splittings, the leptonic mixing angles and the leptonic Dirac CP violating phase, are also successfully reproduced for both normal and inverted neutrino mass hierarchies. We find a feasible range of values for the leptonic Dirac CP phase to be in the ranges for normal ordering and for inverted ordering, which is consistent with the 3σ experimentally allowed limits. The sum of neutrino masses is obtained as meV for normal ordering and meV for inverted ordering which are well consistent with all the recent limits. In addition, the obtained ranges for the effective neutrino masses are meV, for normal ordering and meV, for inverted ordering which are in agreement with the recent experimental bounds. For the quark sector, the derived results are also in agreement with the recent data on the quark masses and mixing angles. The model under consideration can also accommodate the muon anomalous magnetic moment.
期刊介绍:
Nuclear Physics B focuses on the domain of high energy physics, quantum field theory, statistical systems, and mathematical physics, and includes four main sections: high energy physics - phenomenology, high energy physics - theory, high energy physics - experiment, and quantum field theory, statistical systems, and mathematical physics. The emphasis is on original research papers (Frontiers Articles or Full Length Articles), but Review Articles are also welcome.