INTEGRAIS QUÂNTICO RELATIVISTA DE GRACELI [43]

March 06, 2025

$G$ ${\nabla }^{2}\psi =\sum _{n=1}^{N}{\frac {\partial ^{2}\psi }{\partial x_{n}^{2}}}$

$G$ ${\hat {H}}$ ${\nabla }^{2}\psi =\sum _{n=1}^{N}{\frac {\partial ^{2}\psi }{\partial x_{n}^{2}}}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$T_{\mu \nu }$ ${\frac {h}{m_{e}c}}$ $T_{\mu \nu }$ ${\nabla }^{2}\psi =\sum _{n=1}^{N}{\frac {\partial ^{2}\psi }{\partial x_{n}^{2}}}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$\psi ^{*}$

$G$ $G$ ${\nabla }^{2}\psi =\sum _{n=1}^{N}{\frac {\partial ^{2}\psi }{\partial x_{n}^{2}}}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$G$ $G$ $\lambda$ $\psi ^{*}$ $T_{\mu \nu }$ $[$ ${\frac {h}{m_{e}c}}$ / $\lambda$ $\psi ^{*}$ ${\nabla }^{2}\psi =\sum _{n=1}^{N}{\frac {\partial ^{2}\psi }{\partial x_{n}^{2}}}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

March 06, 2025

$G$ $\lambda ={\frac {h}{p}}$

$G$ ${\hat {H}}$ $\lambda ={\frac {h}{p}}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$T_{\mu \nu }$ ${\frac {h}{m_{e}c}}$ $T_{\mu \nu }$ $\lambda ={\frac {h}{p}}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$\psi ^{*}$ $\lambda ={\frac {h}{p}}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

$G$ $G$ $\lambda ={\frac {h}{p}}$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

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

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INTEGRAIS QUÂNTICO RELATIVISTA DE GRACELI [43]

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