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[LECS/QM-11] TIme Dependent Sch\"{o}dinger equation

AK-47's picture 24-06-24 11:06:43

[NOTES/QM-12001] Free Particle Energy Eigen functions and Eigen values

The energy eigenvalues and eigenfunctions are obtained for a free particle in one dimension. Properties and delta function normalization are discussed. It is shown that the energy eigenvalue must be positive. The free particle solution in three dimension is briefly given.

kapoor's picture 24-06-24 09:06:03

[NOTES/QM-12004] Free Particle in Three Dimensions

The energy eigen functions of free particle are given. These are found to be eigen functions  momentum also. The energy eigen functions have infinite degeneracy. There an eigen function  corresponding to each momentum direction.

kapoor's picture 24-06-24 05:06:27

[NOTES/QM-11002] Probability Conservation

Starting from the time dependent Schr\"{o}dinger equation, an equation of continuity \[{\partial\rho\over\partial t} + \vec{\nabla}.\vec{j}=0\] is derived. Physical interpretation of the continuity equation is given in analogy with charge conservation in electromagnetic theory. The equation of continuity represents conservation of probability in quantum mechanics.

AK-47's picture 24-06-23 18:06:03

[NOTES/QM-11006] Optics Mechanics Analogy Road to Wave Mechanics

                  
Making use of analogy between optics ad mechanics we motivate the introduction of the Schrodinger equation.
Here Fermi's "Lectures on Quantum Mechanics" has been followed very closely..

AK-47's picture 24-06-23 18:06:17

[NOTES/QM-11004] Time Reversal Symmetry

Time reversal operation in quantum mechanics of one particle is discussed.

AK-47's picture 24-06-23 18:06:29

[NOTES/QM-11003] Schrodinger Equation for a Charged Particle

Using the classical Hamiltonian and the correspondence rule \(\vec p \to -i\hbar \nabla\), the expression for the Hamiltonian operator for a charged particle is written giving the time dependent Schr\"{o}dinger equation. The Schrodinger equation retains its form under gauge transformations if the wave function is assumed to transform as
\[ \psi(\vec{r},t) \to \psi^\prime (\vec{r},t) =  
e^{-i(q/c)\Lambda(\vec{r},t)}\psi(\vec{r},t). \]

AK-47's picture 24-06-23 18:06:54

[NOTES/QM-11001] Time Dependent Schrodinger Equation :Solution for Wave function at time \(t\)

For conservative systems, we show how solution of time dependent Schrodinger equation can be found by separation of variables. Explicit expression for the wave function at arbitrary time \(t\) is obtained in terms of energy eigenfunctions and eigenvalues. 

AK-47's picture 24-06-23 15:06:07

[NOTES/QM-11007] Time Variation of Average Values

Starting from the time dependent Schrodinger equation, it is proved that the average value a dynamical variable \(\hat F\)obeys the equation\begin{equation} {d\over dt}\, \langle \hat{F} \rangle = \,\langle{\partial\over \partial t} \hat{F} \rangle + {1\over i\hbar} \langle\, [\hat{F},\hat{H} ]\, \rangle.\end{equation}

AK-47's picture 24-06-23 05:06:24

[NOTES/QM-10004] Momentum Representation

The momentum representation is defined and its  connection with  the coordinate  representations is discussed. The transformation bewteen the two is effected by \(\innerproduct{x}{p}\) which are just the momentum eigenfunctions in the coordinate representation. Delta function normalization and the box normalization is discussed for the momentum eigenfunctions.

AK-47's picture 24-06-22 11:06:14

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