GRACELI - DELTA TENSOR QUANTUM FUNÇÃO

${\mathcal {L}}\left\{\delta (t-a)\right\}=e^{-as}$ / $[$ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ] =

$\delta (x-\alpha )={\frac {1}{2\pi }}\int _{-\infty }^{\infty }e^{ip(x-\alpha )}\ dp\ .$ / $[$ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ] =

${\mathcal {F}}(\delta (t-a))=\int _{-\infty }^{\infty }\delta (t-a)e^{-i\omega t}dt=e^{-i\omega a}$ . $[$ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ] =

$m{\operatorname {d^{2}} \!x \over \operatorname {d} \!t^{2}}+kx=I\delta (t)$ / $[$ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ] =

$f(x)=\sum p(x_{i})\delta (x-x_{i})$ / $[$ $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ] =

${\mathcal {L}}\left\{\delta (t-a)\right\}=e^{-as}$ / $g_{ij}(x)=\delta _{ij}-{\frac {1}{3}}R_{iklj}x^{k}x^{l}+O(|x|^{3})$ [ ${T^{\lambda }}_{\mu \nu }$ ] [

[

R_{\rho \sigma \mu \nu }=g_{\rho \zeta }{R^{\zeta }}_{\sigma \mu \nu }.

]

[

\lambda

{\mathcal {T}}

\sigma

\psi

-i\hbar {\frac {\partial }{\partial x_{n}}}

[x,t] ] =

$\delta (x-\alpha )={\frac {1}{2\pi }}\int _{-\infty }^{\infty }e^{ip(x-\alpha )}\ dp\ .$ / / $g_{ij}(x)=\delta _{ij}-{\frac {1}{3}}R_{iklj}x^{k}x^{l}+O(|x|^{3})$ [ ${T^{\lambda }}_{\mu \nu }$ ] [

[

R_{\rho \sigma \mu \nu }=g_{\rho \zeta }{R^{\zeta }}_{\sigma \mu \nu }.

]

[

\lambda

{\mathcal {T}}

\sigma

\psi

-i\hbar {\frac {\partial }{\partial x_{n}}}

[x,t] ] =

${\mathcal {F}}(\delta (t-a))=\int _{-\infty }^{\infty }\delta (t-a)e^{-i\omega t}dt=e^{-i\omega a}$ . /

g_{ij}(x)=\delta _{ij}-{\frac {1}{3}}R_{iklj}x^{k}x^{l}+O(|x|^{3})

[

{T^{\lambda }}_{\mu \nu }

] [

[

R_{\rho \sigma \mu \nu }=g_{\rho \zeta }{R^{\zeta }}_{\sigma \mu \nu }.

]

[

\lambda

{\mathcal {T}}

\sigma

\psi

-i\hbar {\frac {\partial }{\partial x_{n}}}

[x,t] ] =

$m{\operatorname {d^{2}} \!x \over \operatorname {d} \!t^{2}}+kx=I\delta (t)$ / / $g_{ij}(x)=\delta _{ij}-{\frac {1}{3}}R_{iklj}x^{k}x^{l}+O(|x|^{3})$ [ ${T^{\lambda }}_{\mu \nu }$ ] [

[

R_{\rho \sigma \mu \nu }=g_{\rho \zeta }{R^{\zeta }}_{\sigma \mu \nu }.

]

[

\lambda

{\mathcal {T}}

\sigma

\psi

-i\hbar {\frac {\partial }{\partial x_{n}}}

[x,t] ] =

$f(x)=\sum p(x_{i})\delta (x-x_{i})$ / / $g_{ij}(x)=\delta _{ij}-{\frac {1}{3}}R_{iklj}x^{k}x^{l}+O(|x|^{3})$ [ ${T^{\lambda }}_{\mu \nu }$ ] [

[

R_{\rho \sigma \mu \nu }=g_{\rho \zeta }{R^{\zeta }}_{\sigma \mu \nu }.

]

[

\lambda

{\mathcal {T}}

\sigma

\psi

-i\hbar {\frac {\partial }{\partial x_{n}}}

[x,t] ] =

${\mathcal {L}}\left\{\delta (t-a)\right\}=e^{-as}$ / $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ [DR] = ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$

$\delta (x-\alpha )={\frac {1}{2\pi }}\int _{-\infty }^{\infty }e^{ip(x-\alpha )}\ dp\ .$ / $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ [DR] = ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$

${\mathcal {F}}(\delta (t-a))=\int _{-\infty }^{\infty }\delta (t-a)e^{-i\omega t}dt=e^{-i\omega a}$ . / $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ [DR] = ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$

$m{\operatorname {d^{2}} \!x \over \operatorname {d} \!t^{2}}+kx=I\delta (t)$ / $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ [DR] = ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$

$f(x)=\sum p(x_{i})\delta (x-x_{i})$ / $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ [DR] = ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$

Pesquisar este blog

GRACELI - DELTA TENSOR QUANTUM FUNÇÃO

Comentários

Postar um comentário