FÓTON-ELETRODINÂMICA GRACELI - QUÂNTICA QUÍMICA RELATIVISITA

TEORIA GRACELI QUÂNTICA QUÍMICA RELATIVISTA DE CAMPOS.

1 / $\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / ${\sqrt {(-i\mathbf {\nabla } )^{2}+m^{2}}}\psi =i{\frac {\partial }{\partial t}}\psi$ $c={\frac {\lambda }{T}}=\lambda \,f$ $\left|\psi ({\vec {r}},t)\right\rangle$ [-1]

1 / $\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / $c={\frac {\lambda }{T}}=\lambda \,f$ $i\hbar {\frac {\partial \psi }{\partial t}}={\frac {\hbar c}{i}}\left(\alpha _{0}mc\psi +\alpha _{1}{\frac {\partial \psi }{\partial x^{1}}}+\alpha _{2}{\frac {\partial \psi }{\partial x^{2}}}+\alpha _{3}{\frac {\partial \psi }{\partial x^{3}}}\right)$ $\left|\psi ({\vec {r}},t)\right\rangle$ [-1]

1 / $\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / $c={\frac {\lambda }{T}}=\lambda \,f$ ${\vec {v}}\cdot {\vec {u}}=\sum _{i=1}^{N}v^{i}u^{i}\equiv v^{i}u^{i}$ . $\left|\psi ({\vec {r}},t)\right\rangle$ [-1]

1 / $\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / $c={\frac {\lambda }{T}}=\lambda \,f$ $S=\int dtL(\phi ,\partial _{\mu }\phi )$ . $\left|\psi ({\vec {r}},t)\right\rangle$ [-1]

1 / $\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / $c={\frac {\lambda }{T}}=\lambda \,f$ $L=\int dx{\frac {1}{2}}\left[\mu {\dot {\phi (t,x)}}^{2}-\nu \left({\frac {d\phi (t,x)}{dx}}\right)^{2}\right]$ ,. $\left|\psi ({\vec {r}},t)\right\rangle$ [-1]

1 / $\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / $c={\frac {\lambda }{T}}=\lambda \,f$ $-{\frac {\hbar ^{2}}{2m_{e}}}{{\nabla }^{2}}\psi +V\psi =E\psi$ ,. $\left|\psi ({\vec {r}},t)\right\rangle$ [-1]

/ $\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / $c={\frac {\lambda }{T}}=\lambda \,f$ ${1 \over \Phi }{d^{2}\Phi \over d\phi ^{2}}=-m^{2}$ ,. $\left|\psi ({\vec {r}},t)\right\rangle$ [-1]

$\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / $c={\frac {\lambda }{T}}=\lambda \,f$ $\Phi ''={\frac {d^{2}\Phi }{d\phi ^{2}}}$ , ,. $\left|\psi ({\vec {r}},t)\right\rangle$

$\left|\psi ({\vec {r}},t)\right\rangle$ [EG = E = M μ] / $c={\frac {\lambda }{T}}=\lambda \,f$ $E=-{\frac {m\,e^{4}\,Z^{2}}{8\,\varepsilon _{0}^{2}\,n^{2}\,h^{2}}}$ , ,. $\left|\psi ({\vec {r}},t)\right\rangle$

Pesquisar este blog

FÓTON-ELETRODINÂMICA GRACELI - QUÂNTICA QUÍMICA RELATIVISITA

Comentários

Postar um comentário