抄録
The uniaxially compressional and tilt moduli of the fluxoid lattice obtained from the recent nonlocal theory have remarkable dispersion with respect to the wave number of deformation. However, the Lorentz force originating from the distorsion of these kinds in the fluxoid lattice is not dispersive, which implies that these elastic moduli have no dispersion as derived from the local theory. In order to examine this discrepancy, the relation between the displacement of the magnetic flux and that of the normal core of the fluxoid is investigated by using the quantization condition of the magnetic flux which has been disregarded in the nonlocal theory. The present result shows that the two displacements are the same. The resultant moduli have no dispersion and agree with the expressions of the local theory.
