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Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Chatterjee, S.; Dragicevic, M.; Del Valle, A. Escalante; Fruhwirth, R.; Jeitler, M.; Krammer, N.; Lechner, L.; Liko, D.; Mikulec, I; Paulitsch, P.; Pitters, F. M.; Schieck, J.; Schofbeck, R.; Spanring, M.; Templ, S.; Waltenberger, W.; Waltenberger, W.
<?xml version='1.0' encoding='utf-8'?> <resource xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns="http://datacite.org/schema/kernel-4" xsi:schemaLocation="http://datacite.org/schema/kernel-4 http://schema.datacite.org/meta/kernel-4.1/metadata.xsd"> <identifier identifierType="URL">https://aperta.ulakbim.gov.tr/record/232768</identifier> <creators> <creator> <creatorName>Tumasyan, A.</creatorName> <givenName>A.</givenName> <familyName>Tumasyan</familyName> <affiliation>Yerevan Phys Inst, Yerevan, Armenia</affiliation> </creator> <creator> <creatorName>Adam, W.</creatorName> <givenName>W.</givenName> <familyName>Adam</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Andrejkovic, J. W.</creatorName> <givenName>J. W.</givenName> <familyName>Andrejkovic</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Bergauer, T.</creatorName> <givenName>T.</givenName> <familyName>Bergauer</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Chatterjee, S.</creatorName> <givenName>S.</givenName> <familyName>Chatterjee</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Dragicevic, M.</creatorName> <givenName>M.</givenName> <familyName>Dragicevic</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Del Valle, A. Escalante</creatorName> <givenName>A. Escalante</givenName> <familyName>Del Valle</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Fruhwirth, R.</creatorName> <givenName>R.</givenName> <familyName>Fruhwirth</familyName> </creator> <creator> <creatorName>Jeitler, M.</creatorName> <givenName>M.</givenName> <familyName>Jeitler</familyName> </creator> <creator> <creatorName>Krammer, N.</creatorName> <givenName>N.</givenName> <familyName>Krammer</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Lechner, L.</creatorName> <givenName>L.</givenName> <familyName>Lechner</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Liko, D.</creatorName> <givenName>D.</givenName> <familyName>Liko</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Mikulec, I</creatorName> <givenName>I</givenName> <familyName>Mikulec</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Paulitsch, P.</creatorName> <givenName>P.</givenName> <familyName>Paulitsch</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Pitters, F. M.</creatorName> <givenName>F. M.</givenName> <familyName>Pitters</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Schieck, J.</creatorName> <givenName>J.</givenName> <familyName>Schieck</familyName> </creator> <creator> <creatorName>Schofbeck, R.</creatorName> <givenName>R.</givenName> <familyName>Schofbeck</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Spanring, M.</creatorName> <givenName>M.</givenName> <familyName>Spanring</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Templ, S.</creatorName> <givenName>S.</givenName> <familyName>Templ</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Waltenberger, W.</creatorName> <givenName>W.</givenName> <familyName>Waltenberger</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> <creator> <creatorName>Waltenberger, W.</creatorName> <givenName>W.</givenName> <familyName>Waltenberger</familyName> <affiliation>Inst Hochenergiephys, Vienna, Austria</affiliation> </creator> </creators> <titles> <title>Search For A Heavy Higgs Boson Decaying Into Two Lighter Higgs Bosons In The Tau Tau Bb Final State At 13Tev</title> </titles> <publisher>Aperta</publisher> <publicationYear>2021</publicationYear> <dates> <date dateType="Issued">2021-01-01</date> </dates> <resourceType resourceTypeGeneral="Text">Journal article</resourceType> <alternateIdentifiers> <alternateIdentifier alternateIdentifierType="url">https://aperta.ulakbim.gov.tr/record/232768</alternateIdentifier> </alternateIdentifiers> <relatedIdentifiers> <relatedIdentifier relatedIdentifierType="DOI" relationType="IsIdenticalTo">10.1007/JHEP11(2021)057</relatedIdentifier> </relatedIdentifiers> <rightsList> <rights rightsURI="http://www.opendefinition.org/licenses/cc-by">Creative Commons Attribution</rights> <rights rightsURI="info:eu-repo/semantics/openAccess">Open Access</rights> </rightsList> <descriptions> <description descriptionType="Abstract">A search for a heavy Higgs boson H decaying into the observed Higgs boson h with a mass of 125 GeV and another Higgs boson h(S) is presented. The h and h(S) bosons are required to decay into a pair of tau leptons and a pair of b quarks, respectively. The search uses a sample of proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13TeV, corresponding to an integrated luminosity of 137 fb(-1). Mass ranges of 240-3000 GeV for m(H) and 60-2800 GeV for m(hS) are explored in the search. No signal has been observed. Model independent 95% confidence level upper limits on the product of the production cross section and the branching fractions of the signal process are set with a sensitivity ranging from 125 fb (for m(H) = 240 GeV) to 2.7 fb (for m(H) = 1000 GeV). These limits are compared to maximally allowed products of the production cross section and the branching fractions of the signal process in the next-to-minimal supersymmetric extension of the standard model.</description> </descriptions> </resource>
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