CÁLCULO GRACELI SINTÉTICO [70]

a_0

,/ [

{\frac {\omega }{2\pi }}

.] φ =

a_n

cos

A(z)=\sum _{{n=-\infty }}^{\infty }a_{n}z^{n}\,

[

\mathrm {\phi (p)=\int \psi (q)e^{2\pi ipq \over h}dq.}

.] φ [ + ]

b_n

sen

B(z)=\sum _{{n=-\infty }}^{\infty }b_{n}z^{n}

[-

\mathrm {\phi (p)=\int \psi (q)e^{2\pi ipq \over h}dq.}

.] φ =

a_0

,/ [

{\frac {\omega }{2\pi }}

.] φ =

a_n

cos

A(z)=\sum _{{n=-\infty }}^{\infty }a_{n}z^{n}\,

[

{\partial ^{2} \over \partial x^{2}}\psi (x,t)=\mathrm {i} \hbar {\partial  \over \partial t}\psi (x,t).

.] φ [ + ]

b_n

sen

B(z)=\sum _{{n=-\infty }}^{\infty }b_{n}z^{n}

[-

{\partial ^{2} \over \partial x^{2}}\psi (x,t)=\mathrm {i} \hbar {\partial  \over \partial t}\psi (x,t).

.] φ =

a_0

,/ [

{\frac {\omega }{2\pi }}

.] φ =

a_n

cos

A(z)=\sum _{{n=-\infty }}^{\infty }a_{n}z^{n}\,

[

{\partial ^{2} \over \partial x^{2}}\psi (x,t)+V(x)\psi (x,t)=\mathrm {i} \hbar {\partial  \over \partial t}\psi (x,t).

.] φ [ + ]

b_n

sen

B(z)=\sum _{{n=-\infty }}^{\infty }b_{n}z^{n}

[-

{\partial ^{2} \over \partial x^{2}}\psi (x,t)+V(x)\psi (x,t)=\mathrm {i} \hbar {\partial  \over \partial t}\psi (x,t).

.] φ =

a_0

,/ [

{\frac {\omega }{2\pi }}

.] φ =

a_n

cos

A(z)=\sum _{{n=-\infty }}^{\infty }a_{n}z^{n}\,

[

\left({\partial ^{2} \over \partial x^{2}}+1\right)\psi (x,t)={\partial ^{2} \over \partial t^{2}}\psi (x,t).

.] φ [ + ]

b_n

sen

B(z)=\sum _{{n=-\infty }}^{\infty }b_{n}z^{n}

[-

\left({\partial ^{2} \over \partial x^{2}}+1\right)\psi (x,t)={\partial ^{2} \over \partial t^{2}}\psi (x,t).

a_0

,/ [

{\frac {\omega }{2\pi }}

.] φ =

a_n

cos

A(z)=\sum _{{n=-\infty }}^{\infty }a_{n}z^{n}\,

[

f_{1}(t)={\frac {1}{T}}\sum _{-\infty }^{\infty }f(t)e^{iwnt}

..] φ [ + ]

b_n

sen

B(z)=\sum _{{n=-\infty }}^{\infty }b_{n}z^{n}

[-

f_{1}(t)={\frac {1}{T}}\sum _{-\infty }^{\infty }f(t)e^{iwnt}

.]] φ =.] φ =

a_0

,/ [

{\frac {\omega }{2\pi }}

.] φ =

a_n

cos

A(z)=\sum _{{n=-\infty }}^{\infty }a_{n}z^{n}\,

[

f(t)={\frac {1}{2\pi }}\int \limits _{-\infty }^{\infty }F(w)e^{iwt}dw

.] φ [ + ]

b_n

sen

B(z)=\sum _{{n=-\infty }}^{\infty }b_{n}z^{n}

[-

f(t)={\frac {1}{2\pi }}\int \limits _{-\infty }^{\infty }F(w)e^{iwt}dw

]] φ =

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