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Display information for equation id:math.1777.6 on revision:1777

* Page found: Lippmann- Schwinger- Gleichung (eq math.1777.6)

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Hash: 2d91ba08ee5a66bcdb12d2a9a66ef6b4

TeX (original user input): 

\begin{align}

& \left| \Psi  \right\rangle =\left| \Phi  \right\rangle +\frac{1}{\left( E-{{{\hat{H}}}_{0}} \right)}{{{\hat{H}}}^{(1)}}\left| \Psi  \right\rangle  \\

& \frac{1}{\left( E-{{{\hat{H}}}_{0}} \right)}:={{\left( E-{{{\hat{H}}}_{0}} \right)}^{-1}} \\

\end{align}

LaTeXML (experimentell; verwendet MathML) rendering

MathML (15.718 KB / 2.073 KB) :

| Ψ ⟩ = | Φ ⟩ + 1 ( E - H ^ 0 ) ⁢ H ^ ( 1 ) ⁢ | Ψ ⟩ 1 ( E - H ^ 0 ) := ( E - H ^ 0 ) - 1 absent ket Ψ ket Φ 1 𝐸 subscript ^ 𝐻 0 superscript ^ 𝐻 1 ket Ψ absent assign 1 𝐸 subscript ^ 𝐻 0 superscript 𝐸 subscript ^ 𝐻 0 1 {\displaystyle{\displaystyle\begin{aligned} \par&\displaystyle\left|\Psi\right% \rangle=\left|\Phi\right\rangle+\frac{1}{\left(E-{{{\hat{H}}}_{0}}\right)}{{{% \hat{H}}}^{(1)}}\left|\Psi\right\rangle\\ \par&\displaystyle\frac{1}{\left(E-{{{\hat{H}}}_{0}}\right)}:={{\left(E-{{{% \hat{H}}}_{0}}\right)}^{-1}}\\ \par\end{aligned}}}

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MathML (experimentell; keine Bilder) rendering

MathML (2.499 KB / 451 B) :

|Ψ⟩=|Φ⟩+1(E−H^0)H^(1)|Ψ⟩1(E−H^0):=(E−H^0)−1

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