Lattice Effective Field Theory for Nuclear Physics - XQCD13

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Compute the projected adiabatic matrix Projected adiabatic Hamiltonian is now an effective two-body Hamiltonian. Similar in spirit to no-core shell model with resonating group method. But some differences. Distortion of the nucleus wavefunctions is automatic due to projection in Euclidean time. Rupak, D.L., PRL 111 (2013) 032502; Pine, D.L., Rupak, work in progress 50
Example: Quartet neutron-deuteron scattering Pine, D.L., Rupak, work in progress 51
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: Use projection Monte Carlo to propa
Page 53 and 54: Use coupled channels for capture re
Page 55: Summary A golden age for nuclear th

Lattice Effective Field Theory for Nuclear Physics - XQCD13

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