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Display information for equation id:math.3923.29 on revision:3923

* Page found: Zustände mit Bahn- und Spinvariablen (eq math.3923.29)

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Hash: 6834192831241825ab49d8397d399b29

TeX (original user input): 

\begin{align}
& {{{\hat{H}}}_{B}}{{\left| {{\Psi }_{\alpha }} \right\rangle }_{t}}=i\hbar \frac{\partial }{\partial t}{{\left| {{\Psi }_{\alpha }} \right\rangle }_{t}}\Leftrightarrow \left( {{{\hat{H}}}_{B}}\times 1 \right){{\left| \Psi \right\rangle }_{t}}=i\hbar \frac{\partial }{\partial t}{{\left| \Psi \right\rangle }_{t}} \\
& \alpha =1,2 \\
\end{align}

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MathML (19.499 KB / 2.331 KB) :

H ^ B ⁢ | Ψ α ⟩ t = i ⁢ ℏ ⁢ ∂ ∂ ⁡ t ⁢ | Ψ α ⟩ t ⇔ ( H ^ B × 1 ) ⁢ | Ψ ⟩ t = i ⁢ ℏ ⁢ ∂ ∂ ⁡ t ⁢ | Ψ ⟩ t α = 1 , 2 missing-subexpression ⇔ subscript ^ 𝐻 𝐵 subscript ket subscript Ψ 𝛼 𝑡 𝑖 Planck-constant-over-2-pi 𝑡 subscript ket subscript Ψ 𝛼 𝑡 subscript ^ 𝐻 𝐵 1 subscript ket Ψ 𝑡 𝑖 Planck-constant-over-2-pi 𝑡 subscript ket Ψ 𝑡 missing-subexpression 𝛼 1 2 {\displaystyle{\displaystyle\begin{aligned} &\displaystyle{{{\hat{H}}}_{B}}{{% \left|{{\Psi}_{\alpha}}\right\rangle}_{t}}=i\hbar\frac{\partial}{\partial t}{{% \left|{{\Psi}_{\alpha}}\right\rangle}_{t}}\Leftrightarrow\left({{{\hat{H}}}_{B% }}\times 1\right){{\left|\Psi\right\rangle}_{t}}=i\hbar\frac{\partial}{% \partial t}{{\left|\Psi\right\rangle}_{t}}\\ &\displaystyle\alpha=1,2\\ \end{aligned}}}

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H^B|Ψα⟩t=iℏ∂∂t|Ψα⟩t⇔(H^B×1)|Ψ⟩t=iℏ∂∂t|Ψ⟩tα=1,2

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