INTEGRAIS QUÂNTICO DE GRACELI [40]

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ $\lambda ={h \over m_{e}v}$ ] $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ $[$ $\lambda ={h \over m_{e}v}$ $\psi ^{*}$

$G$ $\lambda ={h \over m_{e}v}$ $] /$ $G$ $G$ $\lambda$ $\psi ^{*}$

$G$ $\lambda ={h \over m_{e}v}$ $G$

$G$ $G$ $ψ [$ $\lambda ={h \over m_{e}v}$ ] $\psi ^{*}$

$G$ $G$ $\lambda$ $\psi ^{*}$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ ${\frac {h}{m_{e}c}}$ ] $G$ $\lambda$ $\psi ^{*}$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ $G$ $\lambda$ $[$ ${\frac {h}{m_{e}c}}$ / $\lambda$ $]$ $\psi ^{*}$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ ${\frac {h}{m_{e}c}}$ / $ψ$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ $[$ ${\frac {h}{m_{e}c}}$ / $\lambda$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ ${\frac {h}{m_{e}c}}$ / $T_{\mu \nu }$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ $[$ ${\frac {h}{m_{e}c}}$ / $\lambda$ $T_{\mu \nu }$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ $\lambda ={h \over m_{e}v}$ $G$

$G$ $G$ $\lambda ={h \over m_{e}v}$ ${\hat {H}}$ $G$ $\lambda ={h \over m_{e}v}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$