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and the Einstein's field equations can be made equivalent to square of energy by the product of a factor as the speed of light in vacuum.

[tex] c \left[ R_{\mu \nu} - \frac{1}{2} g_{\mu \nu} R \right] = - 8 \pi \frac{a^2 c^4}{h} T_{\mu \nu} [/tex]

In empty space at time=0, and considering vacuum fluctuation, the field equations become

[tex] cR_{\mu \nu} = \left(\psi_i \cdot \psi_j \right) \left(\phi_i \cdot \phi_j \right) \geq h^2 [/tex]