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Variational Method and Energy Approximation

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Using the variational method, find the best possible wave function approximation for a given system where Ψ(λ)\Psi(\lambda) depends on the parameter λ\lambda. Calculate the expectation value of the energy and find the condition for minimum energy.

The variational method is a powerful tool in quantum mechanics used for approximating the ground state energy of a system. It relies on choosing a trial wave function that depends on one or more parameters and adjusting these parameters to minimize the expectation value of the energy. The central idea is that among all possible wave functions, the true ground state wave function will give the lowest possible expectation value for the energy of the system, according to the variational principle.

This problem involves selecting a parameter-dependent wave function and finding the condition under which the energy expectation value is minimized. The strategy involves calculating the expectation value of the Hamiltonian with respect to your trial wave function and varying the parameters to find a minimum. This often involves taking the derivative of the energy expectation with respect to the parameters and setting it to zero to find critical points, and then determining which of these yields the lowest energy. This method is particularly useful because it gives an upper bound on the true ground state energy even when an exact solution is unobtainable.

Understanding the variational method offers insights into the approximation techniques beyond exact solutions, demonstrating how assumptions and approximations can be used effectively in quantum mechanics. It illustrates how theoretical approaches can provide practical outcomes, such as predicting energy levels in complex quantum systems where solving the Schrödinger equation exactly is not feasible.

Posted by Gregory 5 hours ago

Related Problems

Use the variational method to find the upper bound for the ground state energy of the 1D infinite square well problem.

For a Hamiltonian partitioned as H=H0+λVH = H_0 + \lambda V, determine the first order correction to the energy E1E_1 using perturbation theory. Consider the zeroth order Hamiltonian H0Ψ0=E0Ψ0H_0 \Psi_0 = E_0 \Psi_0 to have a known solution.

In time-dependent perturbation theory, the first-order transition amplitude from an initial state m|m\rangle to a final state n|n\rangle is given by

cn(1)(t)=i0tnV(t)m,eiωnmt,dt,c_n^{(1)}(t) = -\frac{i}{\hbar} \int_0^t \langle n | V(t') | m \rangle , e^{i \omega_{nm} t'} , dt',

where ωnm=EnEm\omega_{nm} = \frac{E_n - E_m}{\hbar} and V(t)V(t) is the time-dependent perturbation.

a) Explain the physical meaning of the transition amplitude cn(1)(t)c_n^{(1)}(t).

b) Write down the expression for the transition probability from state m|m\rangle to n|n\rangle, and explain how it relates to the amplitude.

Given an unperturbed system with known exact eigenvalues and eigenfunctions, apply time-independent perturbation theory to find the first-order correction to the eigenvalue EnE_n and the eigenfunction ψn\psi_n.