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Display information for equation id:math.1599.24 on revision:1599

* Page found: Zeitunabhängige Schrödinger- Gleichung und stationäre Zustände (eq math.1599.24)

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Hash: 838a7b191dac3f422ffeb7b65eba18ac

TeX (original user input):

\int\limits_{{{R}^{3}}}^{{}}{{}}\left( \hat{H}\Psi  \right)*\Psi {{d}^{3}}r=\int\limits_{{{R}^{3}}}^{{}}{{}}\left( E\Psi  \right)*\Psi {{d}^{3}}r=E*

TeX (checked):

\int \limits _{{R}^{3}}^{}{}\left({\hat {H}}\Psi \right)*\Psi {{d}^{3}}r=\int \limits _{{R}^{3}}^{}{}\left(E\Psi \right)*\Psi {{d}^{3}}r=E*

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MathML (1.279 KB / 329 B) :

R3(H^Ψ)*Ψd3r=R3(EΨ)*Ψd3r=E*
<math class="mwe-math-element" xmlns="http://www.w3.org/1998/Math/MathML"><mrow data-mjx-texclass="ORD"><mstyle displaystyle="true" scriptlevel="0"><munderover><mo form="prefix" texclass="OP">&#x222B;</mo><mrow data-mjx-texclass="ORD"><msup><mi>R</mi><mrow data-mjx-texclass="ORD"><mn>3</mn></mrow></msup></mrow><mrow data-mjx-texclass="ORD"></mrow></munderover><mrow data-mjx-texclass="INNER"><mo data-mjx-texclass="OPEN">(</mo><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>H</mi><mo>^</mo></mover></mrow></mrow><mi mathvariant="normal">&#x03A8;</mi><mo data-mjx-texclass="CLOSE">)</mo></mrow><mo>*</mo><mi mathvariant="normal">&#x03A8;</mi><msup><mi>d</mi><mrow data-mjx-texclass="ORD"><mn>3</mn></mrow></msup><mi>r</mi><mo>=</mo><munderover><mo form="prefix" texclass="OP">&#x222B;</mo><mrow data-mjx-texclass="ORD"><msup><mi>R</mi><mrow data-mjx-texclass="ORD"><mn>3</mn></mrow></msup></mrow><mrow data-mjx-texclass="ORD"></mrow></munderover><mrow data-mjx-texclass="INNER"><mo data-mjx-texclass="OPEN">(</mo><mi>E</mi><mi mathvariant="normal">&#x03A8;</mi><mo data-mjx-texclass="CLOSE">)</mo></mrow><mo>*</mo><mi mathvariant="normal">&#x03A8;</mi><msup><mi>d</mi><mrow data-mjx-texclass="ORD"><mn>3</mn></mrow></msup><mi>r</mi><mo>=</mo><mi>E</mi><mo>*</mo></mstyle></mrow></math>

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Calculated based on the variables occurring on the entire Zeitunabhängige Schrödinger- Gleichung und stationäre Zustände page

Identifiers

  • R
  • H^
  • Ψ
  • Ψ
  • r
  • R
  • E
  • Ψ
  • Ψ
  • r
  • E

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