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Saturday, May 30, 2015

Exploring Quantum Physics - Final Exam Part 2 Question 4

Question:

What is the Gaussian variational estimate of the ground state energy for the following potential:

ˆHΨ(r)=22μ2Ψ(r)+krΨ(r)=EΨ(r)

Solution:

I see this as the climax of the whole exam. The original problem statement has a lot of other hints, but I still get this wrong due to some inaccuracy.

First, we substitute the standard Gaussian to the kinetic energy term. I've got inaccuracy here so the whole problem is wrong. So let's do that here again.


22μ2Ψ(r)=22μ21π3/4d3/2exp(r22d2)=22μ21π3/4d3/2exp(r21+r22+r232d2)=22μπ3/4d3/22exp(r21+r22+r232d2)=22μπ3/4d3/2(r1d2,r2d2,r3d2)exp(r21+r22+r232d2)=22μπ3/4d3/2(r21d41d2+r22d41d2+r23d41d2)exp(r21+r22+r232d2)=22μπ3/4d3/2(r21d4+r22d4+r23d43d2)exp(r21+r22+r232d2)

To find the energy, we do an integration

T=1π3/4d3/2exp(r22d2)(22μπ3/4d3/2(r21d4+r22d4+r23d43d2)exp(r21+r22+r232d2))dV=1π3/4d3/2exp(r21+r22+r232d2)(22μπ3/4d3/2(r21d4+r22d4+r23d43d2)exp(r21+r22+r232d2))dV=1π3/4d3/222μπ3/4d3/2exp(r21+r22+r232d2)((r21d4+r22d4+r23d43d2)exp(r21+r22+r232d2))dV=22μπ3/2d3((r21d4+r22d4+r23d43d2)exp(r21+r22+r23d2))dV=22μπ3/2d5((r21d2+r22d2+r23d23)exp(r21+r22+r23d2))dV=22μπ3/2d5((r21d2+r22d2+r23d2)exp(r21+r22+r23d2))dV+22μπ3/2d5(3exp(r21+r22+r23d2))dV=22μπ3/2d7((r21+r22+r23)exp(r21+r22+r23d2))dV+22μπ3/2d5(3exp(r21+r22+r23d2))dV

In this form, we can see this is a Gaussian variance integral. We know that 12πσ2ex22σ2dx=1 and x212πσ2ex22σ2dx=σ2, so we can compute the basic integrals as follow:

exp(x2d2)dx=exp(x22(12)d2)dx=exp(x22(12)2d2)dx=exp(x22(d2)2)dx=2π(d2)212π(d2)2exp(x22(d2)2)dx=2π(d2)2=πd x2exp(x2d2)dx=x2exp(x22(12)d2)dx=x2exp(x22(12)2d2)dx=x2exp(x22(d2)2)dx=2π(d2)212π(d2)2x2exp(x22(d2)2)dx=2π(d2)2(d2)2=πd32


With these basic integral - computing T becomes a substitution exercise. The above are triple integrals and therefore we turn it into iterated integral and compute them.

T=22μπ3/2d7((r21+r22+r23)exp(r21+r22+r23d2))dV+22μπ3/2d5(3exp(r21+r22+r23d2))dV=22μπ3/2d7(3πd32πdπd)+22μπ3/2d5(3πdπdπd)=324μd2+322μd2=324μd2

Next we move on an compute V, another integral

V=ΨkrΨdV=1π3/4d3/2exp(r22d2)kr1π3/4d3/2exp(r22d2)dV=1π3/2d3exp(r22d2)krexp(r22d2)dV=1π3/2d3krexp(r2d2)dV

Despite the deceptive simplicity in the formula, it is a triple integral with r being the length of the vector. Now it make sense to convert this to spherical coordinates.

=1π3/2d34πkr3exp(r2d2)dr

Let we let s=r2d2, ds=2rd2dr, so we further simplify this to

=1π3/2d34πkr3exp(s)dr=1π3/2d34πkr3d22rexp(s)ds=1π3/2d34πkr2d22exp(s)ds=1π3/2d34πkr2d42d2exp(s)ds=1π3/2d34πkd42sexp(s)ds=2kdπ1/2sexp(s)ds=2kdπ1/2Γ(2)=2kdπ1/2

So the total energy is T+V=324μd2+2kdπ1/2. To estimate the ground state we would want to minimize it.

0=ddd(T+V)=ddd(324μd2+2kdπ1/2)=3(2)24μd3+2kπ1/23(2)24μd3=2kπ1/2d3=3(2)2π1/24(2k)μ=32π1/24kμ

Finally, we substitute this back into the energy expression

T+V=324μd2+2kdπ1/2=32d4μd3+2kdπ1/2=32d4μ(32π1/24kμ)+2kdπ1/2=kdπ1/2+2kdπ1/2=3kdπ1/2=3kπ1/2(32π1/24kμ)1/3=(81k32π1/24kμπ3/2)1/3=(81k224πμ)1/3=(814π)1/3(2k2μ)1/3

Phew - that's it! What a climax.

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