{"@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/1361131421065970176.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1140/epjc/s10052-020-7723-2"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/content/pdf/10.1140/epjc/s10052-020-7723-2.pdf"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/article/10.1140/epjc/s10052-020-7723-2/fulltext.html"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1911.11507"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"Leading two-loop corrections to the Higgs boson self-couplings in models with extended scalar sectors"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:title>Abstract</jats:title><jats:p>We compute the dominant two-loop corrections to the Higgs trilinear coupling <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\lambda _{hhh}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi>λ</mml:mi><mml:mrow><mml:mi>hhh</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula> and to the Higgs quartic coupling <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\lambda _{hhhh}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi>λ</mml:mi><mml:mrow><mml:mi>hhhh</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula> in models with extended Higgs sectors, using the effective-potential approximation. We provide in this paper all necessary details about our calculations, and present general <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\overline{{\\mathrm{MS}}}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mover><mml:mi>MS</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math></jats:alternatives></jats:inline-formula> expressions for derivatives of the integrals appearing in the effective potential at two loops. We also consider three particular Beyond-the-Standard-Model (BSM) scenarios – namely a typical scenario of an Inert Doublet Model (IDM), and scenarios of a Two-Higgs-Doublet Model (2HDM) and of a Higgs Singlet Model (HSM) without scalar mixing – and we include all the necessary finite counterterms to obtain (in addition to <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\overline{{\\mathrm{MS}}}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mover><mml:mi>MS</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math></jats:alternatives></jats:inline-formula> results) on-shell scheme expressions for the corrections to the Higgs self-couplings. With these analytic results, we investigate the possible magnitude of two-loop BSM contributions to the Higgs self-couplings and the fate of the non-decoupling effects that are known to appear at one loop. We find that, at least as long as pertubative unitarity conditions are fulfilled, the size of two-loop corrections remains well below that of one-loop corrections. Typically, two-loop contributions to <jats:inline-formula><jats:alternatives><jats:tex-math>$$\\lambda _{hhh}$$</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi>λ</mml:mi><mml:mrow><mml:mi>hhh</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula> amount to approximately 20% of those at one loop, implying that the non-decoupling effects observed at one loop are not significantly modified, but also meaning that higher-order corrections need to be taken into account for the future perspective of precise measurements of the Higgs trilinear coupling.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381131421065971712","@type":"Researcher","foaf:name":[{"@value":"Johannes Braathen"}]},{"@id":"https://cir.nii.ac.jp/crid/1381131421065971970","@type":"Researcher","foaf:name":[{"@value":"Shinya Kanemura"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"14346044"},{"@type":"EISSN","@value":"14346052"}],"prism:publicationName":[{"@value":"The European Physical Journal C"}],"dc:publisher":[{"@value":"Springer Science and Business Media LLC"}],"prism:publicationDate":"2020-03","prism:volume":"80","prism:number":"3","prism:startingPage":"227"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://creativecommons.org/licenses/by/4.0","https://creativecommons.org/licenses/by/4.0"],"url":[{"@id":"http://link.springer.com/content/pdf/10.1140/epjc/s10052-020-7723-2.pdf"},{"@id":"http://link.springer.com/article/10.1140/epjc/s10052-020-7723-2/fulltext.html"}],"createdAt":"2020-03-10","modifiedAt":"2021-03-10","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=QB460-466","dc:title":"QB460-466"},{"@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-%20Phenomenology%20(hep-ph)","dc:title":"High Energy Physics - Phenomenology (hep-ph)"},{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20and%20particle%20physics.%20Atomic%20energy.%20Radioactivity","dc:title":"Nuclear and particle physics. 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