Jump to navigation Jump to search

General

Display information for equation id:math.1598.0 on revision:1598

* Page found: Zeitunabhängige Schrödinger- Gleichung und stationäre Zustände (eq math.1598.0)

(force rerendering)

Occurrences on the following pages:

Hash: 2b780f1cce6d8d78fe92866d0fab1784

TeX (original user input):

i\hbar \dot{\Psi }(\bar{r},t)=\hat{H}\Psi

TeX (checked):

i\hbar {\dot {\Psi }}({\bar {r}},t)={\hat {H}}\Psi

LaTeXML (experimental; uses MathML) rendering

MathML (3.788 KB / 853 B) :

i Ψ ˙ ( r ¯ , t ) = H ^ Ψ 𝑖 Planck-constant-over-2-pi ˙ Ψ ¯ 𝑟 𝑡 ^ 𝐻 Ψ {\displaystyle{\displaystyle i\hbar\dot{\Psi}(\bar{r},t)=\hat{H}\Psi}}
<math xmlns="http://www.w3.org/1998/Math/MathML" id="p1.1.m1.1" class="ltx_Math" alttext="{\displaystyle{\displaystyle i\hbar\dot{\Psi}(\bar{r},t)=\hat{H}\Psi}}" display="inline">
  <semantics id="p1.1.m1.1a">
    <mrow id="p1.1.m1.1.12" xref="p1.1.m1.1.12.cmml">
      <mrow id="p1.1.m1.1.12.1" xref="p1.1.m1.1.12.1.cmml">
        <mi id="p1.1.m1.1.1" xref="p1.1.m1.1.1.cmml">i</mi>
        <mo id="p1.1.m1.1.12.1.1" xref="p1.1.m1.1.12.1.1.cmml"></mo>
        <mi mathvariant="normal" id="p1.1.m1.1.2" xref="p1.1.m1.1.2.cmml"></mi>
        <mo id="p1.1.m1.1.12.1.1a" xref="p1.1.m1.1.12.1.1.cmml"></mo>
        <mover accent="true" id="p1.1.m1.1.3" xref="p1.1.m1.1.3.cmml">
          <mi mathvariant="normal" id="p1.1.m1.1.3.2" xref="p1.1.m1.1.3.2.cmml">Ψ</mi>
          <mo id="p1.1.m1.1.3.1" xref="p1.1.m1.1.3.1.cmml">˙</mo>
        </mover>
        <mo id="p1.1.m1.1.12.1.1b" xref="p1.1.m1.1.12.1.1.cmml"></mo>
        <mrow id="p1.1.m1.1.12.1.2" xref="p1.1.m1.1.12.1.2.1.cmml">
          <mo stretchy="false" id="p1.1.m1.1.4" xref="p1.1.m1.1.12.1.2.1.cmml">(</mo>
          <mover accent="true" id="p1.1.m1.1.5" xref="p1.1.m1.1.5.cmml">
            <mi id="p1.1.m1.1.5.2" xref="p1.1.m1.1.5.2.cmml">r</mi>
            <mo stretchy="false" id="p1.1.m1.1.5.1" xref="p1.1.m1.1.5.1.cmml">¯</mo>
          </mover>
          <mo id="p1.1.m1.1.6" xref="p1.1.m1.1.12.1.2.1.cmml">,</mo>
          <mi id="p1.1.m1.1.7" xref="p1.1.m1.1.7.cmml">t</mi>
          <mo stretchy="false" id="p1.1.m1.1.8" xref="p1.1.m1.1.12.1.2.1.cmml">)</mo>
        </mrow>
      </mrow>
      <mo id="p1.1.m1.1.9" xref="p1.1.m1.1.9.cmml">=</mo>
      <mrow id="p1.1.m1.1.12.2" xref="p1.1.m1.1.12.2.cmml">
        <mover accent="true" id="p1.1.m1.1.10" xref="p1.1.m1.1.10.cmml">
          <mi id="p1.1.m1.1.10.2" xref="p1.1.m1.1.10.2.cmml">H</mi>
          <mo stretchy="false" id="p1.1.m1.1.10.1" xref="p1.1.m1.1.10.1.cmml">^</mo>
        </mover>
        <mo id="p1.1.m1.1.12.2.1" xref="p1.1.m1.1.12.2.1.cmml"></mo>
        <mi mathvariant="normal" id="p1.1.m1.1.11" xref="p1.1.m1.1.11.cmml">Ψ</mi>
      </mrow>
    </mrow>
    <annotation-xml encoding="MathML-Content" id="p1.1.m1.1b">
      <apply id="p1.1.m1.1.12.cmml" xref="p1.1.m1.1.12">
        <eq id="p1.1.m1.1.9.cmml" xref="p1.1.m1.1.9"/>
        <apply id="p1.1.m1.1.12.1.cmml" xref="p1.1.m1.1.12.1">
          <times id="p1.1.m1.1.12.1.1.cmml" xref="p1.1.m1.1.12.1.1"/>
          <ci id="p1.1.m1.1.1.cmml" xref="p1.1.m1.1.1">𝑖</ci>
          <csymbol cd="latexml" id="p1.1.m1.1.2.cmml" xref="p1.1.m1.1.2">Planck-constant-over-2-pi</csymbol>
          <apply id="p1.1.m1.1.3.cmml" xref="p1.1.m1.1.3">
            <ci id="p1.1.m1.1.3.1.cmml" xref="p1.1.m1.1.3.1">˙</ci>
            <ci id="p1.1.m1.1.3.2.cmml" xref="p1.1.m1.1.3.2">Ψ</ci>
          </apply>
          <interval closure="open" id="p1.1.m1.1.12.1.2.1.cmml" xref="p1.1.m1.1.12.1.2">
            <apply id="p1.1.m1.1.5.cmml" xref="p1.1.m1.1.5">
              <ci id="p1.1.m1.1.5.1.cmml" xref="p1.1.m1.1.5.1">¯</ci>
              <ci id="p1.1.m1.1.5.2.cmml" xref="p1.1.m1.1.5.2">𝑟</ci>
            </apply>
            <ci id="p1.1.m1.1.7.cmml" xref="p1.1.m1.1.7">𝑡</ci>
          </interval>
        </apply>
        <apply id="p1.1.m1.1.12.2.cmml" xref="p1.1.m1.1.12.2">
          <times id="p1.1.m1.1.12.2.1.cmml" xref="p1.1.m1.1.12.2.1"/>
          <apply id="p1.1.m1.1.10.cmml" xref="p1.1.m1.1.10">
            <ci id="p1.1.m1.1.10.1.cmml" xref="p1.1.m1.1.10.1">^</ci>
            <ci id="p1.1.m1.1.10.2.cmml" xref="p1.1.m1.1.10.2">𝐻</ci>
          </apply>
          <ci id="p1.1.m1.1.11.cmml" xref="p1.1.m1.1.11">Ψ</ci>
        </apply>
      </apply>
    </annotation-xml>
    <annotation encoding="application/x-tex" id="p1.1.m1.1c">{\displaystyle{\displaystyle i\hbar\dot{\Psi}(\bar{r},t)=\hat{H}\Psi}}</annotation>
  </semantics>
</math>

SVG image empty. Force Re-Rendering

SVG (0 B / 8 B) :


MathML (experimental; no images) rendering

MathML (700 B / 277 B) :

iΨ˙(r¯,t)=H^Ψ
<math class="mwe-math-element" xmlns="http://www.w3.org/1998/Math/MathML"><mrow data-mjx-texclass="ORD"><mstyle displaystyle="true" scriptlevel="0"><mi>i</mi><mi data-mjx-alternate="1">&#x210F;</mi><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi mathvariant="normal">&#x03A8;</mi><mo>˙</mo></mover></mrow></mrow><mo stretchy="false">(</mo><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mover><mi>r</mi><mo>¯</mo></mover></mrow></mrow><mo>,</mo><mi>t</mi><mo stretchy="false">)</mo><mo>=</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></mstyle></mrow></math>

Translations to Computer Algebra Systems

Translation to Maple

In Maple:

Translation to Mathematica

In Mathematica:

Similar pages

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

Identifiers

  • i
  • Ψ˙
  • r¯
  • t
  • H^
  • Ψ

MathML observations

0results

0results

no statistics present please run the maintenance script ExtractFeatures.php

0 results

0 results