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dc.contributor.authorSavage, Martin J.
dc.contributor.authorTiburzi, Brian C.
dc.contributor.authorWagman, Michael L.
dc.contributor.authorWinter, Frank
dc.contributor.authorBeane, Silas R.
dc.contributor.authorChang, Emmanuel
dc.contributor.authorOrginos, Kostas
dc.contributor.authorNPLQCD Collaboration
dc.contributor.authorShanahan, Phiala E
dc.contributor.authorDavoudi, Zohreh
dc.contributor.authorDetmold, William
dc.date.accessioned2017-08-14T13:55:31Z
dc.date.available2017-08-14T13:55:31Z
dc.date.issued2017-08
dc.date.submitted2017-01
dc.identifier.issn0031-9007
dc.identifier.issn1079-7114
dc.identifier.urihttp://hdl.handle.net/1721.1/110935
dc.description.abstractThe nuclear matrix element determining the pp→de⁺ν fusion cross section and the Gamow-Teller matrix element contributing to tritium β decay are calculated with lattice quantum chromodynamics for the first time. Using a new implementation of the background field method, these quantities are calculated at the SU(3) flavor–symmetric value of the quark masses, corresponding to a pion mass of m[subscript π]∼806  MeV. The Gamow-Teller matrix element in tritium is found to be 0.979(03)(10) at these quark masses, which is within 2σ of the experimental value. Assuming that the short-distance correlated two-nucleon contributions to the matrix element (meson-exchange currents) depend only mildly on the quark masses, as seen for the analogous magnetic interactions, the calculated pp→de⁺ν transition matrix element leads to a fusion cross section at the physical quark masses that is consistent with its currently accepted value. Moreover, the leading two-nucleon axial counterterm of pionless effective field theory is determined to be L[subscript 1,A]=3.9(0.2)(1.0)(0.4)(0.9)  fm³ at a renormalization scale set by the physical pion mass, also agreeing within the accepted phenomenological range. This work concretely demonstrates that weak transition amplitudes in few-nucleon systems can be studied directly from the fundamental quark and gluon degrees of freedom and opens the way for subsequent investigations of many important quantities in nuclear physics.en_US
dc.description.sponsorshipNational Science Foundation (U.S.) (PHY11-25915)en_US
dc.publisherAmerican Physical Societyen_US
dc.relation.isversionofhttp://dx.doi.org/10.1103/PhysRevLett.119.062002en_US
dc.rightsArticle is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.en_US
dc.sourceAmerican Physical Societyen_US
dc.titleProton-Proton Fusion and Tritium β Decay from Lattice Quantum Chromodynamicsen_US
dc.typeArticleen_US
dc.identifier.citationSavage, Martin J. et al. "Proton-Proton Fusion and Tritium β Decay from Lattice Quantum Chromodynamics." Physical Review Letters 119, 6: 062002 © 2017 American Physical Societyen_US
dc.contributor.departmentMassachusetts Institute of Technology. Center for Theoretical Physicsen_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physicsen_US
dc.contributor.departmentMassachusetts Institute of Technology. Laboratory for Nuclear Scienceen_US
dc.contributor.mitauthorShanahan, Phiala E
dc.contributor.mitauthorDavoudi, Zohreh
dc.contributor.mitauthorDetmold, William
dc.relation.journalPhysical Review Lettersen_US
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2017-08-10T22:00:02Z
dc.language.rfc3066en
dc.rights.holderAmerican Physical Society
dspace.orderedauthorsSavage, Martin J.; Shanahan, Phiala E.; Tiburzi, Brian C.; Wagman, Michael L.; Winter, Frank; Beane, Silas R.; Chang, Emmanuel; Davoudi, Zohreh; Detmold, William; Orginos, Kostasen_US
dspace.embargo.termsNen_US
dc.identifier.orcidhttps://orcid.org/0000-0002-1110-3633
dc.identifier.orcidhttps://orcid.org/0000-0002-0400-8363
mit.licensePUBLISHER_POLICYen_US


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