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               <dc:title>Ab initio Calculation of the np→dγ Radiative Capture Process</dc:title>
               <dc:creator>Beane, Silas R.</dc:creator>
               <dc:creator>Chang, Emmanuel</dc:creator>
               <dc:creator>Detmold, William</dc:creator>
               <dc:creator>Orginos, Kostas</dc:creator>
               <dc:creator>Parreño García, Assumpta</dc:creator>
               <dc:creator>Savage, Martin J.</dc:creator>
               <dc:creator>Tiburzi, Brian C.</dc:creator>
               <dc:creator>NPLQCD Collaboration</dc:creator>
               <dc:subject>Física de partícules</dc:subject>
               <dc:subject>Experiments</dc:subject>
               <dc:subject>Particle physics</dc:subject>
               <dc:subject>Experiments</dc:subject>
               <dc:description>Lattice QCD calculations of two-nucleon systems are used to isolate the short-distance two-body electromagnetic contributions to the radiative capture process n p → d γ , and the photo-disintegration processes γ ( * ) d → n p . In nuclear potential models, such contributions are described by phenomenological meson-exchange currents, while in the present work, they are determined directly from the quark and gluon interactions of QCD. Calculations of neutron-proton energy levels in multiple background magnetic fields are performed at two values of the quark masses, corresponding to pion masses of m π ∼ 450 and 806 MeV, and are combined with pionless nuclear effective field theory to determine the amplitudes for these low-energy inelastic processes. At m π ∼ 806     MeV , using only lattice QCD inputs, a cross section σ 806     MeV ∼ 17     mb is found at an incident neutron speed of v = 2 , 200     m / s . Extrapolating the short-distance contribution to the physical pion mass and combining the result with phenomenological scattering information and one-body couplings, a cross section of σ lqcd ( n p → d γ ) = 334.9 ( + 5.2 − 5.4 )     mb is obtained at the same incident neutron speed, consistent with the experimental value of σ expt ( n p → d γ ) = 334.2 ( 0.5 )     mb .</dc:description>
               <dc:date>2019-05-08T15:20:06Z</dc:date>
               <dc:date>2019-05-08T15:20:06Z</dc:date>
               <dc:date>2015-09-24</dc:date>
               <dc:date>2019-05-08T15:20:07Z</dc:date>
               <dc:type>info:eu-repo/semantics/article</dc:type>
               <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
               <dc:relation>Reproducció del document publicat a: https://doi.org/10.1103/PhysRevLett.115.132001</dc:relation>
               <dc:relation>Physical Review Letters, 2015, vol. 115, num. 13, p. 132001</dc:relation>
               <dc:relation>https://doi.org/10.1103/PhysRevLett.115.132001</dc:relation>
               <dc:rights>(c) American Physical Society, 2015</dc:rights>
               <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
               <dc:publisher>American Physical Society</dc:publisher>
               <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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