MECÂNICA GRACELI GENERALIZADA - QUÂNTICA TENSORIAL DIMENSIONAL RELATIVISTA DE CAMPOS [1.160]

o tensor energia-momento $T_{\mu \nu }$ é aquele de um campo eletromagnético, i.e. se o tensor momento-energia eletromagnético

UNIDADES DE GRACELI

M = MOMENTUM.

M = $t_{P}={\sqrt {\frac {\hbar G}{c^{5}}}}\approx 5.391247(60)\times 10^{-44}{\mbox{ s}}$ ] / [ [ / $\psi ^{*}$ $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$t_{P}={\sqrt {\frac {\hbar G}{c^{5}}}}\approx 5.391247(60)\times 10^{-44}{\mbox{ s}}$ ] / [ [ / $\psi ^{*}$ $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$E_{p}={\sqrt {\frac {\hbar c^{5}}{G}}}\approx$ / [ / $\psi ^{*}$ [ $\psi ^{*}$ $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$E_{p}={\frac {\hbar }{t_{P}}},$ / [ / $\psi ^{*}$ $/$ $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$m_{P}={\sqrt {\frac {\hbar c}{G}}}$ [ [ / $\psi ^{*}$ $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$\rho _{P}={\frac {m_{P}}{l_{P}^{3}}}={\frac {c^{5}}{\hbar G^{2}}}$ / [ / $\psi ^{*}$ $/$ $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$