MECÂNICA GENERALIZADA GRACELI - QUÂNTICA QUÍMICA RELATIVISTA [140]

novembro 22, 2022

EQUAÇÃO DE ONDA REATIVISTA QUÃNTICA QUÍMICA EM MECÃNICA GENRALIZADA GRACELI :

G ψ = E ψ = IGFF $\psi ^{*}$ E [tG+] $\lambda$ ψ ω ${\mathcal {T}}$ /c] = $\,N_{A}$ $\,M$ $\,z^{+}$ $\,z^{-}$ $\,e$ [/ $\,\epsilon _{o}$ ] / $\,r_{0}$ / = $\lambda$ ħω $q\ \$ [Ϡ ] [ξ ] [,ς] $g_{s}$ $\epsilon _{s}$ [ $\epsilon _{s}$ q G*] ${\begin{pmatrix}\psi _{0}\\\psi _{1}\end{pmatrix}}$ ψ μ / h/c ψ(x, t) $-i\hbar {\frac {\partial }{\partial x_{n}}}$ x t ]..

[1/ ψ[1/ μ / mh/c [G ψ = E ψ = IGFF

\psi ^{*}

E [tG+]

\lambda

ψ ω

{\mathcal {T}}

] ψ

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

[-1]

[1/ ψ[1/ μ / m h/c [G ψ = E ψ = IGFF

\psi ^{*}

E [tG+]

\lambda

ψ ω

{\mathcal {T}}

\mu

,

\sigma

,

\psi

, ] ψ

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

{\hat {H}}

\hbar

i

{\boldsymbol {\mu }}=-g_{s}\mu _{B}({\boldsymbol {s}}/\hbar )

[1/ ψ[1/ μ / m h/c [G ψ = E ψ = IGFF

\psi ^{*}

E [tG+]

\lambda

ψ ω

{\mathcal {T}}

\mu

,

\sigma

,

\psi

, ] ψ

{\boldsymbol {\mu }}=-g_{s}\mu _{B}({\boldsymbol {s}}/\hbar )

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

{\hat {H}}

\hbar

i

E={\frac {hc}{\lambda }}

[1/ ψ[1/ μ / m h/c [G ψ = E ψ = IGFF

\psi ^{*}

E [tG+]

\lambda

ψ ω

{\mathcal {T}}

\mu

,

\sigma

,

\psi

, ] ψ

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

/ [

\lambda _{0}

] / m.

E={\frac {hc}{\lambda }}

\gamma _{ij}(x,t)=\sum _{k=1}^{N}\sigma _{ik}(x,t)\sigma _{jk}(x,t),

\lambda _{0}

é o comprimento de onda do fóton antes do espalhamento,

{\frac {\partial w}{\partial t}}={\frac {1}{2}}{\frac {\partial ^{2}w}{\partial x^{2}}}-uV(x)w

{\boldsymbol {\mu }}=-g_{s}\mu _{B}({\boldsymbol {s}}/\hbar )

E={\frac {hc}{\lambda }}

[G ψ = E ψ = IGFF

\psi ^{*}

E [tG+ =

{\hat {H}}

\hbar

i

[1/ ψ[1/ μ / m h/c [G ψ = E ψ = IGFF

\psi ^{*}

E [tG+]

\lambda

ψ ω

{\mathcal {T}}

\mu

,

\sigma

,

\psi

, ] ψ

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

/ [

\lambda _{0}

] / m.

{\boldsymbol {\mu }}=-g_{s}\mu _{B}({\boldsymbol {s}}/\hbar )

E={\frac {hc}{\lambda }}

\gamma _{ij}(x,t)=\sum _{k=1}^{N}\sigma _{ik}(x,t)\sigma _{jk}(x,t),

.

[G ψ = E ψ = IGFF

\psi ^{*}

E [tG+]

\lambda

ψ ω

{\mathcal {T}}

\mu

,

\sigma

,

\psi

, ]

/ [1- cos

θ ]

EFEITO FOTOELETRICO NO SISTEMA DE GRACELI COM ÂNGULOS;

hf=\phi +E_{c_{max}}\,

θ ]

\psi ^{*}

$E_{c_{max}}={\frac {1}{2}}mv_{m}^{2}$ /

[1- cos

θ ].

\psi ^{*}

TUNELAMENTO QUÂNTICO COM ÂNGULOS.

$T=e^{-2bL}$ $b={\sqrt {\frac {8\pi ^{2}m(Ub-E)}{h^{2}}}}$ / /

[1- cos

θ ].

\psi ^{*}

$T=e^{-2bL}$ $b={\sqrt {\frac {8\pi ^{2}m(Ub-E)}{h^{2}}}}$ $\lambda -\lambda _{0}={\frac {h}{m_{e}c}}(1-\cos {\theta })$ .

\psi ^{*}

TRIALIDADE MOMENTUM MAGNÉTICO - ONDAS - PARTÍCULAS.

E=hf

${\boldsymbol {\mu }}$ .

\psi ^{*}

$\lambda ={\frac {h}{p}}$ ${\boldsymbol {\mu }}$

\psi ^{*}

$p={\frac {E}{c}}$ , ${\boldsymbol {\mu }}$

\psi ^{*}

$p={\frac {E}{c}}$

\psi ^{*}

$\mathrm {Energia} =\mathrm {Massa} \,\times \,(\mathrm {velocidade\ da\ luz\ no\ vacuo} )^{2}$ ${\boldsymbol {\mu }}$

\psi ^{*}

\mathrm {E} =\mathrm {m} \,\times \,\mathrm {c} ^{2}

/ ${\boldsymbol {\mu }}$

\psi ^{*}

\psi ^{*}

= INTERAÇÕES DE FORÇAS FUNDAMENTAIS

E=mc2 ${\boldsymbol {\mu }}$

E=mc2 ${\boldsymbol {\mu }}$ $\psi ^{*}$

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