some boundary condition for the SWD wavefunction. We would start with a Gaussian ansatz and see what type of wavefunction does it lead to when continued to a region $2a^2\frac{V_0} {M}<1$, where both gravity and the matter field are both quantum in nature. From the classical Einstein equation $$G_{\mu\nu}=R_{\mu\nu}-{1\over 2} g_{\mu\nu} R=kT_{\mu\nu}\,$$ we observe that “geometry and matter” get coupled through (43). It is also a well known fact that the matter field is quantized and for that reason in equation (43) one writes $<T_{\mu\nu}>$ on the right hand side and treats $g_{\mu\nu}$ as classical background. Keeping this in mind we argued that time is determined by the geometry itself. Let us be precise about the equation (42). The time that appears in (42) is the time that we use in quantum theory and is specified by the classical background $a(t)$ which in turn has been determined from the initial condition as if the many fingureness gets hidden in the $a(t)$ by the initial condition. The dynamicalness of $t$ has been transferred by demanding both $a(t)$ and $t$ complex and allowing $t$ to move both forward and backward direction. Whereas it is difficult to realize it in the framework of 