Identical particles and separating the Schrodinger equation

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Homework Help Overview

The discussion revolves around the Schrödinger equation for two identical particles in a one-dimensional potential. The potential is expressed in terms of the positions of the particles and involves constants A and B. Participants are tasked with demonstrating the separability of the Schrödinger equation in the variables related to the sum and difference of the particle positions.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the method of variable separation by introducing new variables R and r. There are questions about the correctness of the Hamiltonian after rewriting it in terms of these new variables and concerns about the appearance of certain terms.

Discussion Status

Some participants have successfully rewritten the Hamiltonian and are exploring the implications of their transformations. There is ongoing clarification regarding the application of the multivariable chain rule to the second derivative terms. The discussion is productive, with participants actively engaging in checking assumptions and reasoning through their approaches.

Contextual Notes

Participants are navigating the complexities of rewriting the Hamiltonian and ensuring the correct application of mathematical principles, particularly in the context of identical particles and the implications of their exchange symmetry.

mangojuice14
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Homework Statement


Two identical particles, each of mass m, move in one dimension in the potential
$$V = \frac{1}{2}A(x_1^2+x_2^2)+ \frac{1}{2}B(x_1-x_2)^2$$
where A and B are positive constants and ##x_1## and ##x_2## denote the positions of the particles.
a) Show that the Schrödinger equation is separable in the variables ##x_1+x_2## and ##x_1-x_2##. Find the eigenvalues and the corresponding eigenfunctions.
b)Discuss the symmetry of the eigenfunctions with respect to particle exchange.

Homework Equations


Schrödinger equation:
$$HΨ = EΨ$$
Hamiltonian for identical particles
$$H = \frac{-ħ}{2m}\frac{d^2}{dx_1^2}-\frac{-ħ}{2m}\frac{d^2}{dx_2^2}+\frac{1}{2}A(x_1^2+x_2^2)+ \frac{1}{2}B(x_1-x_2)^2$$

The Attempt at a Solution


I plugged in the Hamiltonian into the Schrödinger equation, and separated variables by setting ##Ψ=X(x_1+x_2)Y(x_1-x_2)##, replaced Ψ with the product and divided by ##XY##. I end up with something I can't really solve. I'm mostly not sure if my separation method is correct, I'm confused on what it means by 'separable in the variables ##x_1+x_2## and ##x_1-x_2##' rather than just ##x_1## and ##x_2## for example. Thanks
 
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Define two new variables, say ##R \equiv x_1+x_2## and ##r \equiv x_1-x_2## and try and rewrite the Hamiltonian in terms of ##R## and ##r##.
 
DrClaude said:
Define two new variables, say ##R \equiv x_1+x_2## and ##r \equiv x_1-x_2## and try and rewrite the Hamiltonian in terms of ##R## and ##r##.
Thanks for the reply
Rewriting the Hamiltonian in terms of those new variables, I get
$$H = \frac{-ħ^2}{2m}\frac{d^2}{dx_1^2}-\frac{-ħ^2}{2m}\frac{d^2}{dx_2^2}+\frac{1}{2}A(R^2-2x_1x_2)+ \frac{1}{2}Br^2$$
This seems incorrect though because of the factor of ##-2x_1x_2## which is due to ##R^2 = x_1^2 + x_2^2+2x_1x_2##. Also, how would I go about changing the terms ##\frac{d^2}{dx_1^2}## and ##\frac{d^2}{dx_2^2}## in terms of R and r?
 
mangojuice14 said:
This seems incorrect though because of the factor of ##-2x_1x_2## which is due to ##R^2 = x_1^2 + x_2^2+2x_1x_2##.
There is also a factor ##x_1x_2## that can appear from ##r^2##.

mangojuice14 said:
Also, how would I go about changing the terms ##\frac{d^2}{dx_1^2}## and ##\frac{d^2}{dx_2^2}## in terms of R and r?
You have to use the multivariable chain rule.
 
Oh right! So I got
$$H = \frac{-ħ^2}{2m}\frac{d^2}{dx_1^2}-\frac{-ħ^2}{2m}\frac{d^2}{dx_2^2}+\frac{1}{2}A(\frac{R^2}{2}+\frac{r^2}{2})+ \frac{1}{2}Br^2$$
for the Hamiltonian.
For the ##\frac{d^2}{dx_1^2}## part I get that:
$$ \frac{d^2}{dx_1^2}=\frac{d^2}{dR^2}(\frac{dR}{dx_1})^2=\frac{d^2}{dR^2}$$
but I could have also used ##r## so am I just allowed to pick one thereby combining the two derivative terms (since the answer is the same for ##\frac{d^2}{dx_2^2}##) or am I doing something wrong?
 
mangojuice14 said:
For the ##\frac{d^2}{dx_1^2}## part I get that:
$$ \frac{d^2}{dx_1^2}=\frac{d^2}{dR^2}(\frac{dR}{dx_1})^2=\frac{d^2}{dR^2}$$
but I could have also used ##r## so am I just allowed to pick one thereby combining the two derivative terms (since the answer is the same for ##\frac{d^2}{dx_2^2}##) or am I doing something wrong?
The ##\frac{d^2}{dx_1^2}## operator will act on a function of ##R## and ##r##, which both depend on ##x_1##.

Have a look at https://www.math.hmc.edu/calculus/tutorials/multichainrule/
 
Oh I see, I think I got it. Thanks!
 

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