Quantum Mechanics Variational Method

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The discussion revolves around using a trial wavefunction to calculate the approximate energy of the first excited state for a particle in a box. The user initially derived an energy expression but encountered discontinuities at specific values of 'a'. After revising their integration, they found a new energy expression but still faced similar discontinuity issues. The user seeks clarification on the nature of these discontinuities and whether their setup is flawed. The conversation highlights the challenges in applying the variational method in quantum mechanics.
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Homework Statement


Consider a particle in a box in the interval [-a,a]. Use the trial wavefunction

ψT = x(a-x2)

to obtain an approximate energy for the first excited state of the box as a function of a.

Homework Equations



Schrodinger equation, Hamiltonian for atomic units is 1/2(d2/dx2)

Normalized energy E = ∫-aaψ*Hψdx/∫-aaψ*ψdx

The Attempt at a Solution



Right, so I just plugged in ψT to the energy equation, and after evaluating the integrals, got E = 1-(3/5)a2 / [a(a2/7-1/15)]. The problem is, this function is discontinuous. It is discontinuous at 0, which makes sense to me, and at a = √(7/15), which I don't understand. I'm pretty sure my integrations were done properly... can anyone either explain this discontinuity to me, or tell me why my set-up was flawed?

Thanks!
 
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Okay, I found one error in my integration. The revised function is E = 1-(3/5)a / [a(a^2/7-1/15)]. Still has the same discontinuity problems, though.
 

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