MECÂNICA GRACELI GENERALIZADA - QUÃNTICA TENSORIAL DIMENSIONAL RELATIVISTA DE CAMPOS [1.007]

- [ $\hbar$ $\lambda ={\frac {h}{p}}$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ $\left[-{\frac {\hbar ^{2}\nabla ^{2}}{2m}}+V\left(\mathbf {r} ,t\right)\right]\Psi \left(\mathbf {r} ,t\right)=i\hbar {\frac {\partial \Psi \left(\mathbf {r} ,t\right)}{\partial t}}$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ $\left[-{\frac {\hbar ^{2}\nabla ^{2}}{2m}}+V\left(\mathbf {r} \right)\right]\psi \left(\mathbf {r} \right)=E\psi \left(\mathbf {r} \right)$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ ${\sqrt {(-i\mathbf {\nabla } )^{2}+m^{2}}}\psi =i{\frac {\partial }{\partial t}}\psi$

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$

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)

G { f [dd]} ´[d] $\hbar$ $\psi$

- [ $\hbar$ ${\mathcal {L}}=\psi ^{*}(i\gamma ^{\mu }D_{\mu }-m)\psi -{\frac {1}{4}}F_{\mu \nu }F^{\mu \nu }$

G { f [dd]} ´[d] $\hbar$ $\psi$

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