It is not that bosons are "encouraged" to occupy the same place, that is quite wrong. Here is an article on the spin-statistics theorem which describes the relationship between particle statistics and the transformation of the wave function under permutations of identical particles. This kind of thing requires more knowledge of quantum mechanics, so I recommend reading an introductory QM textbook.
In short, if you have two identical particles, and your wave function is $\psi(x_1,x_2)$, then
$$ \psi(x_1,x_2) = \pm \psi(x_2,x_1), $$
and this is the relation you should impose on the discretized wave function. You will get a vector of values $\psi_{jk}$ (where $x_j$ are the points in discretized space), and so when you write down the numerical method applied to $\psi_{jk}$, you also require that $\psi_{jk}=\pm \psi_{jk}$, and adjust the numerical method to take account of this (anti-)symmetry.
Also, bear in mind that for non-interacting particles, the PDE separates, and the solution will be of the form $$\frac12\big(\psi_1(x_1)\psi_2(x_2)\pm \psi_1(x_2)\psi_2(x_1)\big),$$
where each $\psi_{i}$ solves the one-particle Schrodinger equation.
What you are asking is more a question of physics than scientific computing.