Jump to navigation
Jump to search
General
Display information for equation id:math.2663.12 on revision:2663
* Page found: Klein Gordon im (Vektor)Potential, Eichinvarianz (eq math.2663.12)
(force rerendering)Occurrences on the following pages:
Hash: 314904d9a89155dff9f04f61f6b7bdde
TeX (original user input):
\mathfrak{i} \hbar {{\partial }_{t}}\Psi =\frac{{{p}^{2}}}{2m}\Psi
TeX (checked):
{\mathfrak {i}}\hbar {{\partial }_{t}}\Psi ={\frac {{p}^{2}}{2m}}\Psi
LaTeXML (experimental; uses MathML) rendering
MathML (4.279 KB / 960 B) :
<math xmlns="http://www.w3.org/1998/Math/MathML" id="p1.1.m1.1" class="ltx_Math" alttext="{\displaystyle{\displaystyle\mathfrak{i}\hbar{{\partial}_{t}}\Psi=\frac{{{p}^{% 2}}}{2m}\Psi}}" display="inline">
<semantics id="p1.1.m1.1a">
<mrow id="p1.1.m1.1.9" xref="p1.1.m1.1.9.cmml">
<mrow id="p1.1.m1.1.9.1" xref="p1.1.m1.1.9.1.cmml">
<mi id="p1.1.m1.1.1" xref="p1.1.m1.1.1.cmml">𝔦</mi>
<mo id="p1.1.m1.1.9.1.1" xref="p1.1.m1.1.9.1.1.cmml"></mo>
<mi mathvariant="normal" id="p1.1.m1.1.2" xref="p1.1.m1.1.2.cmml">ℏ</mi>
<mo id="p1.1.m1.1.9.1.1a" xref="p1.1.m1.1.9.1.1.cmml"></mo>
<mrow id="p1.1.m1.1.9.1.2" xref="p1.1.m1.1.9.1.2.cmml">
<msub id="p1.1.m1.1.9.1.2.1" xref="p1.1.m1.1.9.1.2.1.cmml">
<mo id="p1.1.m1.1.3" xref="p1.1.m1.1.3.cmml">∂</mo>
<mi id="p1.1.m1.1.4.1" xref="p1.1.m1.1.4.1.cmml">t</mi>
</msub>
<mo id="p1.1.m1.1.9.1.2a" xref="p1.1.m1.1.9.1.2.cmml"></mo>
<mi mathvariant="normal" id="p1.1.m1.1.5" xref="p1.1.m1.1.5.cmml">Ψ</mi>
</mrow>
</mrow>
<mo id="p1.1.m1.1.6" xref="p1.1.m1.1.6.cmml">=</mo>
<mrow id="p1.1.m1.1.9.2" xref="p1.1.m1.1.9.2.cmml">
<mstyle displaystyle="true" id="p1.1.m1.1.7" xref="p1.1.m1.1.7.cmml">
<mfrac id="p1.1.m1.1.7a" xref="p1.1.m1.1.7.cmml">
<msup id="p1.1.m1.1.7.2" xref="p1.1.m1.1.7.2.cmml">
<mi id="p1.1.m1.1.7.2.1" xref="p1.1.m1.1.7.2.1.cmml">p</mi>
<mn id="p1.1.m1.1.7.2.2.1" xref="p1.1.m1.1.7.2.2.1.cmml">2</mn>
</msup>
<mrow id="p1.1.m1.1.7.3" xref="p1.1.m1.1.7.3.cmml">
<mn id="p1.1.m1.1.7.3.1" xref="p1.1.m1.1.7.3.1.cmml">2</mn>
<mo id="p1.1.m1.1.7.3.3" xref="p1.1.m1.1.7.3.3.cmml"></mo>
<mi id="p1.1.m1.1.7.3.2" xref="p1.1.m1.1.7.3.2.cmml">m</mi>
</mrow>
</mfrac>
</mstyle>
<mo id="p1.1.m1.1.9.2.1" xref="p1.1.m1.1.9.2.1.cmml"></mo>
<mi mathvariant="normal" id="p1.1.m1.1.8" xref="p1.1.m1.1.8.cmml">Ψ</mi>
</mrow>
</mrow>
<annotation-xml encoding="MathML-Content" id="p1.1.m1.1b">
<apply id="p1.1.m1.1.9.cmml" xref="p1.1.m1.1.9">
<eq id="p1.1.m1.1.6.cmml" xref="p1.1.m1.1.6"/>
<apply id="p1.1.m1.1.9.1.cmml" xref="p1.1.m1.1.9.1">
<times id="p1.1.m1.1.9.1.1.cmml" xref="p1.1.m1.1.9.1.1"/>
<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.m1.1.9.1.2.cmml" xref="p1.1.m1.1.9.1.2">
<apply id="p1.1.m1.1.9.1.2.1.cmml" xref="p1.1.m1.1.9.1.2.1">
<csymbol cd="ambiguous" id="p1.1.m1.1.9.1.2.1.1.cmml" xref="p1.1.m1.1.9.1.2.1">subscript</csymbol>
<partialdiff id="p1.1.m1.1.3.cmml" xref="p1.1.m1.1.3"/>
<ci id="p1.1.m1.1.4.1.cmml" xref="p1.1.m1.1.4.1">𝑡</ci>
</apply>
<ci id="p1.1.m1.1.5.cmml" xref="p1.1.m1.1.5">Ψ</ci>
</apply>
</apply>
<apply id="p1.1.m1.1.9.2.cmml" xref="p1.1.m1.1.9.2">
<times id="p1.1.m1.1.9.2.1.cmml" xref="p1.1.m1.1.9.2.1"/>
<apply id="p1.1.m1.1.7.cmml" xref="p1.1.m1.1.7">
<divide id="p1.1.m1.1.7.1.cmml" xref="p1.1.m1.1.7"/>
<apply id="p1.1.m1.1.7.2.cmml" xref="p1.1.m1.1.7.2">
<csymbol cd="ambiguous" id="p1.1.m1.1.7.2.3.cmml" xref="p1.1.m1.1.7.2">superscript</csymbol>
<ci id="p1.1.m1.1.7.2.1.cmml" xref="p1.1.m1.1.7.2.1">𝑝</ci>
<cn type="integer" id="p1.1.m1.1.7.2.2.1.cmml" xref="p1.1.m1.1.7.2.2.1">2</cn>
</apply>
<apply id="p1.1.m1.1.7.3.cmml" xref="p1.1.m1.1.7.3">
<times id="p1.1.m1.1.7.3.3.cmml" xref="p1.1.m1.1.7.3.3"/>
<cn type="integer" id="p1.1.m1.1.7.3.1.cmml" xref="p1.1.m1.1.7.3.1">2</cn>
<ci id="p1.1.m1.1.7.3.2.cmml" xref="p1.1.m1.1.7.3.2">𝑚</ci>
</apply>
</apply>
<ci id="p1.1.m1.1.8.cmml" xref="p1.1.m1.1.8">Ψ</ci>
</apply>
</apply>
</annotation-xml>
<annotation encoding="application/x-tex" id="p1.1.m1.1c">{\displaystyle{\displaystyle\mathfrak{i}\hbar{{\partial}_{t}}\Psi=\frac{{{p}^{%
2}}}{2m}\Psi}}</annotation>
</semantics>
</math>
SVG image empty. Force Re-Rendering
SVG (0 B / 8 B) :
MathML (experimental; no images) rendering
MathML (733 B / 277 B) :
<math class="mwe-math-element" xmlns="http://www.w3.org/1998/Math/MathML"><mrow data-mjx-texclass="ORD"><mstyle displaystyle="true" scriptlevel="0"><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mi mathvariant="fraktur">i</mi></mrow></mrow><mi data-mjx-alternate="1">ℏ</mi><msub><mi>∂</mi><mrow data-mjx-texclass="ORD"><mi>t</mi></mrow></msub><mi mathvariant="normal">Ψ</mi><mo>=</mo><mrow data-mjx-texclass="ORD"><mfrac><mrow data-mjx-texclass="ORD"><msup><mi>p</mi><mrow data-mjx-texclass="ORD"><mn>2</mn></mrow></msup></mrow><mrow data-mjx-texclass="ORD"><mrow data-mjx-texclass="ORD"><mn>2</mn><mi>m</mi></mrow></mrow></mfrac></mrow><mi mathvariant="normal">Ψ</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 Klein Gordon im (Vektor)Potential, Eichinvarianz page
Identifiers
MathML observations
0results
0results
no statistics present please run the maintenance script ExtractFeatures.php
0 results
0 results