Symmetry of time-dependent Schrödinger equations. II. Exact solutions for the equation {∂<i>x</i> <i>x</i>+2<i>i</i>∂<i>t</i>−2<i>g</i>2(<i>t</i>)<i>x</i>2−2<i>g</i>1(<i>t</i>)<i>x</i> −2<i>g</i>0(<i>t</i>)}Ψ(<i>x</i>, <i>t</i>) = 0 (Q3957296)
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| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Symmetry of time-dependent Schrödinger equations. II. Exact solutions for the equation {∂<i>x</i> <i>x</i>+2<i>i</i>∂<i>t</i>−2<i>g</i>2(<i>t</i>)<i>x</i>2−2<i>g</i>1(<i>t</i>)<i>x</i> −2<i>g</i>0(<i>t</i>)}Ψ(<i>x</i>, <i>t</i>) = 0 |
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Symmetry of time-dependent Schrödinger equations. II. Exact solutions for the equation {∂<i>x</i> <i>x</i>+2<i>i</i>∂<i>t</i>−2<i>g</i>2(<i>t</i>)<i>x</i>2−2<i>g</i>1(<i>t</i>)<i>x</i> −2<i>g</i>0(<i>t</i>)}Ψ(<i>x</i>, <i>t</i>) = 0 (English)
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1982
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maximal kinematical algebra
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commuting observables
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irreducible representation space
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wave functions
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