- Origin of Quantum Physics
- Wave function
- Collapse of Wave Function
- Physically Accepted Wave function
- Normalization Explained
- Method of Normalization
- Orthogonality & Orthonormality
- Hilbert Space
- Quantization Rules
- Operator Formalism
- Commutator Bracket
- Linear Operator
- Hermitian Operator
- Projection Operator
- Unitary Operator
- Parity Operator
- Expectation Value
- Schrodinger Equation
- Wave-Particle Duality Using Schrodinger Equation
- Superposition of States
- Various Representations of Wave Function
- Probability Current Density
- Uncertainty in Operators
- Shortcut for Calculating Momentum Expectation Value
Parity operator corresponds to space reflection about the origin i.e. $\hat{P}\psi(x)=\psi(-x)$ In general, $\hat{P}\psi(\overrightarrow{r})=\psi(-\overrightarrow{r});$ where $\overrightarrow{r}=x\hat{i}+y\hat{i}+z\hat{k}$ and $\overrightarrow{-r}=-x\hat{i}-y\hat{j}-z\hat{k}$ When parity operator acts on a wavefunction, the following changes take place in various coordinate systems: (i) Cartesian co-ordinate system: $x\rightarrow-x,y\rightarrow-y,z\rightarrow-z$ (ii) Spherical polar co-ordinate system: $r\rightarrow r,\,\theta\rightarrow\pi-\theta,\,\phi\rightarrow\pi+\phi$ (iii) Cyllindrical co-ordinate system: $p\rightarrow p,\phi\rightarrow\pi+\phi,z\rightarrow-z$ Properties: (1) Eigenvalues of the Parity Operator is 1, -1. $^{\Longleftrightarrow}$ $\hat{P}\psi(x)=\psi(-x)=\psi(x)\rightarrow$ even parity. $\hat{P}\psi(x)=\psi(-x)=-\psi(x)\rightarrow$ odd parity. (2) Parity operator is hermitian in nature. (3) Parity operator commutes with hamiltonian operator if the potential under which particle is moving i.e. $V\left(x\right)$ is symmetric in nature.