Lattice Effective Field Theory for Nuclear Physics - XQCD13

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Quartet neutron-deuteron scattering (pionless EFT at LO) Pine, D.L., Rupak, work in progress 52
Use coupled channels for capture reactions and break up processes. Lattice Green’s function methods for radiative capture tested for n + p d + g in pionless effective field theory at leading order. Elastic scattering amplitude ( 1 S 0 and 3 S 1 ) M1 radiative capture amplitude 1 S 3 S 1 0 1 S 3 0 S 1 Rupak, D.L., PRL 111 (2013) 032502 53
Page 1 and 2: Lattice Effective Field Theory for
Page 3 and 4: Elemental composition of the human
Page 5 and 6: Stellar nucleosynthesis 5
Page 7 and 8: Lattice quantum chromodynamics u p
Page 9 and 10: T [MeV] Accessible by Lattice QCD 1
Page 11 and 12: Nuclear Scattering Data Effective F
Page 13 and 14: Next-to-leading order on the lattic
Page 15 and 16: LO 3 : S waves 15
Page 17 and 18: Three nucleon forces Two unknown co
Page 19 and 20: Coulomb potential p p Charge symmet
Page 21 and 22: Euclidean time projection p p 21
Page 24: Schematic of lattice Monte Carlo ca
Page 27 and 28: Ground state of Helium-4 LO* (O(Q 0
Page 29 and 30: Ground state of Beryllium-8 LO* (O(
Page 31 and 32: Carbon-12 spectrum and the Hoyle st
Page 33 and 34: Ground state of Carbon-12 LO* (O(Q
Page 35 and 36: Shell model wavefunctions Alpha clu
Page 37 and 38: Structure of ground state and first
Page 39 and 40: Excited state spectrum of carbon-12
Page 41 and 42: Triple alpha reaction rate EM width
Page 43 and 44: Figure courtesy of U.-G. Meißner E
Page 45 and 46: Hoyle relative to Be-8-alpha Be-8 r
Page 47 and 48: “End of the world” plot Epelbau
Page 49 and 50: Use projection Monte Carlo to propa
Page 51: Example: Quartet neutron-deuteron s
Page 55: Summary A golden age for nuclear th

Lattice Effective Field Theory for Nuclear Physics - XQCD13

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