Nuclear Physics with Lattice QCD





Physics Results

Our lattice QCD calculations were performed with Chroma , the lattice software written by Robert Edwards and his team at the Jefferson Laboratory (JLab).  Chroma contains all of the necessary packages to perform lattice calculations.  We have written all of the contraction code required for two-particle interactions and single hadron ground-state spectroscopy.   We submitted a proposal for an exploratory study of two-hadron interactions and for a partially-quenched calculation of the nucleon mass (to extract the sigma-term and strong isospin breaking) to the SciDAC Lattice committee, and were awarded roughly 8% of the JLab computing resources for the funding period April 2005 to April 2006.  The LHP collaboration very kindly allowed us to use the domain-wall propagators they had computed on the MILC lattices as part of their program funded by SciDAC.

Pion-Pion Scattering in the I=2 Channel


The results of our calculation of pion-pion scattering in the I=2 channel are shown in the above figure.  The scattering length multiplied by the pion mass is plotted vs the pion mass dividied by the pion decay constant as measured on the lattices.
Both the quantities on the vertical and horizontal axes are independent of the scale-setting procedure.
The lattice data was computed with domain-wall valence quarks (Kaplan fermions) on the fully-dynamical gauge configurations with staggered sea-quarks.  The lattice spacing is b~0.125 fm, and the spatial extent L~2.5 fm.
The blue-point is the lowest mass datum computed by the CP-PACS collaboration with Wilson on Wilson quarks.

The dashed line corresponds to the parameter free tree-level prediction of chiral perturbation theory (Weinberg), and is seen to be very close to what is computed with lattice QCD.  The shaded region corresponds to our fit, and associated uncertainties, to chiral perturbation theory at the one-loop level.  Both the tree-level and loop-level extrapolations to the physical point agree with the experimental value, and have a smaller uncertainty.




Nucleon-Nucleon Scattering

We have calulated the energy shifts associated with two nucleons using domain wall valence quarks on the staggered MILC lattices with b~0.125 fm, and  spatial extent L~2.5 fm.  The ratio of the proton-proton correlator to the square of the single proton correlator is shown below.



The scattering lengths in the 1S0 channel extracted from the energy-splitting derived from the ratio of correlators  are shown in the figure below, along with the currently best theoretical understanding about how to extrapolate to the chiral limit.   In the extrapolation the experimental value of the scattering length at the physical pion mass has been included, as currently there is not enough lattice data in the regime where the theory is valid.



The scattering lengths in the 3S1-3D1 coupled-channel extracted from the energy-splitting derived from the ratio of correlators  are shown in the figure below, along with the currently best theoretical understanding about how to extrapolate to the chiral limit.   Again, in the extrapolation the experimental value of the scattering length at the physical pion mass has been included, as at this point in time there is not enough lattice data in the regime where the theory is valid.
The chiral extrapolations were performed with the effective field theories (EFT) that have been developed during the last 15 or so years, initiated by the pioneering work of Weinberg.  The advantage these theories have over traditional approaches to nuclear physics is that the dependence upon the light quark masses is explicit.   However,  the lowest pion mass data point is at the upper limits of applicability of the EFT's, and as such there is significant uncertainty in the extrapolations.   Clearly, a lattice QCD calculation at a pion mass of ~ 250 MeV will dramatically reduce the uncertainty.




The Gell-Mann--Okubo Mass-Relation

The Gell-Mann--Okubo mass relation among the baryons in the lowest-lying octet holds to high precision, much higher than one would naively expect  based on SU(3) breaking alone.  Deviations to the relation are from representations transforming as a 27 of SU(3).
In fact, in the large-Nc limit of QCD one finds a suppression factor of 1/Nc ontop of the SU(3) breaking suppresson.
It might have been the case that the smallness of the violation of the relation was small accidentally due to the values of the light quark masses, however, our lattice calculations showed that the violations are small at all values of the light-quark masses.







The Neutron-Proton Mass Difference

The mass difference between the neutron and proton is one of the basic properties of our universe.
We used partially-quenched lattice QCD calculations to compute the contribution to the neutron-proton mass difference from the mass difference between the up and down quarks.  We found that the light-quarks contribute
Mn - Mp = 2.26 +- 0.57 +- 0.42 +- 0.10 MeV
which agrees with the best estimate based on the experimental masses and best estimate of the electromagnetic contribution of
Mn - Mp = 2.05 +- 0.3 MeV.
In our calculation we used the most recent MILC determination of Mu/Md = 0.43 +- 0.01 +- 0.08.



 
Kaon-Pion Scattering

fK/fpi

YN Scattering