{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1361699994594950528.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1007/jhep06(2014)149"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/content/pdf/10.1007/JHEP06(2014)149"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1403.4775"}}],"dc:title":[{"@value":"Confronting Higgcision with electric dipole moments"}],"description":[{"notation":[{"@value":"Current data on the signal strengths and angular spectrum of the 125.5 GeV Higgs boson still allow a CP-mixed state, namely, the pseudoscalar coupling to the top quark can be as sizable as the scalar coupling: $C_u^S \\approx C_u^P =1/2$. CP violation can then arise and manifest in sizable electric dipole moments (EDMs). In the framework of two-Higgs-doublet models, we not only update the Higgs precision (Higgcision) study on the couplings with the most updated Higgs signal strength data, but also compute all the Higgs-mediated contributions from the 125.5 GeV Higgs boson to the EDMs, and confront the allowed parameter space against the existing constraints from the EDM measurements of Thallium, neutron, Mercury, and Thorium monoxide. We found that the combined EDM constraints restrict the pseudoscalar coupling to be less than about $10^{-2}$, unless there are contributions from other Higgs bosons, supersymmetric particles, or other exotic particles that delicately cancel the current Higgs-mediated contributions."}]},{"notation":[{"@value":"34 pages, 17 figures, to appear in JHEP"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381699994594950529","@type":"Researcher","foaf:name":[{"@value":"Kingman Cheung"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994594950528","@type":"Researcher","foaf:name":[{"@value":"Jae Sik Lee"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994594950531","@type":"Researcher","foaf:name":[{"@value":"Eibun Senaha"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994594950530","@type":"Researcher","foaf:name":[{"@value":"Po-Yan Tseng"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"10298479"}],"prism:publicationName":[{"@value":"Journal of High Energy Physics"}],"dc:publisher":[{"@value":"Springer Science and Business Media LLC"}],"prism:publicationDate":"2014-06","prism:volume":"2014","prism:number":"6","prism:startingPage":"149"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","url":[{"@id":"http://link.springer.com/content/pdf/10.1007/JHEP06(2014)149"}],"createdAt":"2014-06-28","modifiedAt":"2017-06-22","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20and%20High%20Energy%20Physics","dc:title":"Nuclear and High Energy Physics"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology","dc:title":"High Energy Physics - Phenomenology"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Experiment%20(hep-ex)","dc:title":"High Energy Physics - Experiment (hep-ex)"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology%20(hep-ph)","dc:title":"High Energy Physics - Phenomenology (hep-ph)"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Experiment","dc:title":"High Energy Physics - Experiment"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360002215251114624","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Linear programming analysis of the R-parity violation within EDM-constraints"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298754834809472","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Electroweak baryogenesis in aligned two Higgs doublet models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360565168516632832","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Probing exotic phenomena at the interface of nuclear and particle physics with the electric dipole moments of diamagnetic atoms: A unique window to hadronic and semi-leptonic CP violation"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184981155072","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Electric dipole moment of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>Hg</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>199</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>\n atom from \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>P</mml:mi></mml:math>\n, \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>C</mml:mi><mml:mi>P</mml:mi></mml:math>\n-odd electron-nucleon interaction"}]},{"@id":"https://cir.nii.ac.jp/crid/1360572092649172352","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Testing aligned CP-violating Higgs sector at future lepton colliders"}]},{"@id":"https://cir.nii.ac.jp/crid/1360853567625890432","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Aligned CP-violating Higgs sector canceling the electric dipole moment"}]},{"@id":"https://cir.nii.ac.jp/crid/1361694369820247040","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Nuclear electric dipole moment in the cluster model with a triton: \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi>Li</mml:mi><mml:mprescripts/><mml:none/><mml:mn>7</mml:mn></mml:mmultiscripts></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mmultiscripts><mml:mi mathvariant=\"normal\">B</mml:mi><mml:mprescripts/><mml:none/><mml:mn>11</mml:mn></mml:mmultiscripts></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/2051433317031842304","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Probing CP-violating Higgs sectors via the precision measurement of coupling constants"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1007/jhep06(2014)149"},{"@type":"OPENAIRE","@value":"doi_dedup___::abb9c77e76ceab986e05a6efab4e9b48"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2014)110_references_DOI_DJPrw9v7NNAS0H0la1IjJMvJv3u"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2022)104_references_DOI_DJPrw9v7NNAS0H0la1IjJMvJv3u"},{"@type":"CROSSREF","@value":"10.1140/epja/i2017-12237-2_references_DOI_DJPrw9v7NNAS0H0la1IjJMvJv3u"},{"@type":"CROSSREF","@value":"10.1103/physrevd.99.075021_references_DOI_DJPrw9v7NNAS0H0la1IjJMvJv3u"},{"@type":"CROSSREF","@value":"10.1007/jhep04(2021)144_references_DOI_DJPrw9v7NNAS0H0la1IjJMvJv3u"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz038_references_DOI_DJPrw9v7NNAS0H0la1IjJMvJv3u"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2020)026_references_DOI_DJPrw9v7NNAS0H0la1IjJMvJv3u"},{"@type":"CROSSREF","@value":"10.1103/physrevc.100.055501_references_DOI_DJPrw9v7NNAS0H0la1IjJMvJv3u"}]}