The ballooning theory of the second kind anticipates the spontaneous radial symmetry breaking of unstable toroidal local modes in tokamak such as drift waves owing to toroidicity. Taking the fluid model equation of ion temperature gradient driven mode to be an instance, the two-dimensional local mode structure associated with the symmetry breaking is solved. When the sideband is neglected, it is reduced to the modified slab wave function by the radial shift. The modified slab wave function is used to yield the seed parallel Reynolds stress, which would otherwise (as in the traditional slab wave function) be zero.