Current matrix element in HAL QCD’s wavefunction-equivalent potential method
Kai Watanabe (Research Center for Nuclear Physics, Osaka University, 10-1 Mihoga-oka, Ibaraki-shi, Osaka 567-0047, Japan); Noriyoshi Ishii (Research Center for Nuclear Physics, Osaka University, 10-1 Mihoga-oka, Ibaraki-shi, Osaka 567-0047, Japan)
We give a formula to calculate a matrix element of a conserved current in the effective quantum mechanics defined by the wavefunction-equivalent potentials proposed by the HAL QCD collaboration. As a first step, a non-relativistic field theory with two-channel coupling is considered as the original theory, with which a wavefunction-equivalent HAL QCD potential is obtained in a closed analytic form. The external field method is used to derive the formula by demanding that the result should agree with the original theory. With this formula, the matrix element is obtained by sandwiching the effective current operator between the left and right eigenfunctions of the effective Hamiltonian associated with the HAL QCD potential. In addition to the naive one-body current, the effective current operator contains an additional two-body term emerging from the degrees of freedom which has been integrated out.
