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\[ \vec{A}  = 5\hat{x} + 4\hat{y}   \]

One-dimensional time-dependent Schrodinger equation of a particle of mass \(m\) is  \[ i\hbar \frac{d \Psi(x,t)}{dt} = - \frac{\hbar^{2}}{2m} \nabla^{2} \Psi(x,t) + V(x) \Psi(x,t)\] where \(\Psi(x,t)\) is the wave-function representing the particle and \(V(x)\) is assumed to be a real function representing the potential energy of the particle.

\[ \Ket{ p } \]

\( \bra{math}\)

\[ \ket{math}\]

\[ \braket{math}\]

\[ \set{math}\]

\[ \Bra{math}\)

\[ \Ket{math}\]

\[ \Braket{math}\]

\[ \Set{math}\]

Take an example : \[ \bra{\Psi}\]

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