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Symbols in Expression \(\frac{\partial}{\partial t} \psi( \vec{r},t)=\psi_0 \frac{\partial}{\partial t}\exp\left(i\left(\frac{ \vec{p}\cdot\vec{r}}{\hbar} - \frac{E t}{\hbar} \right) \right)\)

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ID latex name description reference dimension: time dimension: length dimension: mass dimension: electric charge dimension: luminous intensity dimension: amount of substance dimension: temperature scope domain
0000006238 E
\(E\)		 electric field https://en.wikipedia.org/wiki/Electric_field 0 0 0 0 0 0 0 real any
0000001054 \hbar
\(\hbar\)		 Reduced Planck's constant https://en.wikipedia.org/wiki/Planck_constant#Value -1 2 1 0 0 0 0 real any
0000001467 t
\(t\)		 time https://en.wikipedia.org/wiki/Time_in_physics 1 0 0 0 0 0 0 real any
0000009489 \psi
\(\psi\)		 none 0 0 0 0 0 0 0 complex any
0000008330 \psi_0
\(\psi_0\)		 amplitude of wavefunction 0 0 0 0 0 0 0 complex any
0000004621 i
\(i\)		 imaginary unit https://en.wikipedia.org/wiki/Imaginary_unit 0 0 0 0 0 0 0 imaginary any
0000001134 p
\(p\)		 momentum https://en.wikipedia.org/wiki/Momentum -1 1 1 0 0 0 0 real any
0000002718 \exp
\(\exp\)		 e https://en.wikipedia.org/wiki/E_(mathematical_constant) 0 0 0 0 0 0 0 real any
0000009472 \vec{r}
\(\vec{r}\)		 radius vector 0 1 0 0 0 0 0 real any

Add Symbol to Expression \(\frac{\partial}{\partial t} \psi( \vec{r},t)=\psi_0 \frac{\partial}{\partial t}\exp\left(i\left(\frac{ \vec{p}\cdot\vec{r}}{\hbar} - \frac{E t}{\hbar} \right) \right)\)

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Remove Symbol used in Expression \(\frac{\partial}{\partial t} \psi( \vec{r},t)=\psi_0 \frac{\partial}{\partial t}\exp\left(i\left(\frac{ \vec{p}\cdot\vec{r}}{\hbar} - \frac{E t}{\hbar} \right) \right)\)

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Operations in Expression \(\frac{\partial}{\partial t} \psi( \vec{r},t)=\psi_0 \frac{\partial}{\partial t}\exp\left(i\left(\frac{ \vec{p}\cdot\vec{r}}{\hbar} - \frac{E t}{\hbar} \right) \right)\)

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Relation in Expression \(\frac{\partial}{\partial t} \psi( \vec{r},t)=\psi_0 \frac{\partial}{\partial t}\exp\left(i\left(\frac{ \vec{p}\cdot\vec{r}}{\hbar} - \frac{E t}{\hbar} \right) \right)\)

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