MECÂNICA GRACELI GENERALIZADA - QUÃNTICA TENSORIAL DIMENSIONAL RELATIVISTA DE CAMPOS [1.003]

- [ $\hbar$ $L(t)={\frac {1}{2}}mv^{2}-(V+Q),$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ $Q=-{\frac {\hbar ^{2}}{2m}}{\frac {\nabla ^{2}{\sqrt {\rho }}}{\sqrt {\rho }}}.$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ $K^{Q}(X_{1},t_{1};X_{0},t_{0})={\frac {1}{J(t)^{\frac {1}{2}}}}\exp \left[{\frac {i}{\hbar }}\int _{t_{0}}^{t_{1}}L(t)\,dt\right].$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ $i\hbar {\frac {\partial \psi }{\partial t}}=\left(-{\frac {\hbar ^{2}}{2m}}\nabla ^{2}+V\right)\psi \quad .$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ $\psi ={\sqrt {\rho }}\;\exp \left({\frac {i\,S}{\hbar }}\right),$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ ${\vec {v}}({\vec {r}},t)={\frac {\nabla S({\vec {r}},t)}{m}}\;.$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ $-{\frac {\partial S}{\partial t}}={\frac {\left(\nabla S\right)^{2}}{2m}}+V+Q\;,$

G { f [dd]} ´[d] $\hbar$ $\psi$