Lattice Effective Field Theory for Nuclear Physics - XQCD13

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Schematic of lattice Monte Carlo calculation Hybrid Monte Carlo sampling 24
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 26 and 27: Ground state of Helium-4 Epelbaum,
Page 28 and 29: Ground state of Beryllium-8 Epelbau
Page 30 and 31: Particle clustering included automa
Page 32 and 33: Ground state of Carbon-12 Epelbaum,
Page 34 and 35: Simulations using general initial/f
Page 36 and 37: Carbon-12 0 1 + 0 2 + Epelbaum, Kre
Page 38 and 39: Structure of Hoyle state and second
Page 40 and 41: Light quark mass dependence of heli
Page 42 and 43: Is nature fine-tuned? Less resonanc
Page 44 and 45: Lattice results for pion mass depen
Page 46 and 47: Evidence for correlation with alpha
Page 48 and 49: Scattering and reactions on the lat
Page 50 and 51: Compute the projected adiabatic mat
Page 52 and 53: Quartet neutron-deuteron scattering
Page 54 and 55: M1 transition amplitude n + p d +

Lattice Effective Field Theory for Nuclear Physics - XQCD13

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