Find the possible total energies (Quantum Physics)

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Homework Help Overview

The discussion revolves around a quantum physics problem involving two particles connected by a spring, with a focus on determining the possible total energies for different cases: one with different particles and another with identical fermions. The context includes classical and quantum mechanical interpretations of the system.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the concept of total energy as a sum of potential and kinetic energy, considering classical and quantum perspectives. There is an attempt to apply the harmonic oscillator model, but some participants express uncertainty about the appropriateness of this model for fermions. Questions arise regarding the interpretation of the problem and the feasibility of connecting fermions to a spring.

Discussion Status

The discussion is ongoing, with some participants attempting to solve the first part of the problem while others express confusion about the setup. Guidance has been offered regarding variable transformations to simplify the two-particle system, indicating a productive direction in the exploration of the problem.

Contextual Notes

Some participants note the potential relevance of the natural length of the spring and question the assumptions about particle interactions. There is also mention of the need to translate classical potential into a quantum context, highlighting the complexity of the problem.

BookWei
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Homework Statement


I'm doing problems for practice in quantum physics.
Consider two particles of the mass m in one dimension with coordinates being denoted by x and they are
connected by a spring with spring constant k. Suppose that the total momentum of the system is p.
Find all possible total energies for the following cases :
(1)two particles are different (2)two particles are identical fermions.

2. The attempt at a solution
(1) I try to guess the answer...
Total energy is the sum of potential and kinetic energy. Now our particles have the same mass and they are one-dimensional. Moreover, they are non-identical. Now potential energy is based on spring constant K therefore V=1/2*K*x^2 . Now considering the harmonic oscillator in classic sense total energy E= T +V
Therefore E = P^2/2m + 1/2*mω^2*x^2.

considering energy from quantum mechanical point of view, we know P= -iℏ d/dx =p' and x=x' hamiltonian becomes, H= 1/2 p'^2/2m + 1/2*mω'^2*x^2
now considering the particles time independent
H'ψ(x) = Eψ(x)
the eigenvalues of this Hamiltonian is based on En = (n+ 1/2)ℏω where ground state has non-zero energy.

(2) I have no idea how to start this problem.

Thank you for your help.
 
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BookWei said:
Thank you for your help.

I'm not sure at all how to interpret this problem. My first thought was that you have two particles in a harmonic oscillator, but I suspect that is not what is intended.

I'm not sure how you can have two fermions connected by a spring. How could you attach a fermion to a spring?

Perhaps what is meant is simply to calculate the potential for a classical system of this type and then translate that to a quantum potential - based on particle repulsion and attraction, rather than a spring! - and solve the resulting Schrödinger equation.

In any case, your solution to 1), which appears to be simply a solution to a single particle SHO, cannot be correct.
 
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Thanks a lot.
I upload the original problem file.

I will try to solve the problem (1).
 

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BookWei said:
Thanks a lot.
I upload the original problem file.

I will try to solve the problem (1).

Okay, so the question setter does believe you can attach fermions and bosons to a spring. On the face of it, the natural length of the spring should be relevant, but I think you'll just have to do the maths and see what happens.
 
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BookWei said:
H'ψ(x) = Eψ(x)
You have a two-particle system. So, you can consider the wavefunction to be a function of two position coordinates: ψ(x1, x2).

Do you know how to do a coordinate transformation which separates out the center-of-mass motion and the motion relative to the center of mass (with a reduced mass μ)?
 
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I tried to solve this problem for two days.
But I still do not know how to solve it...
 
I suggest that you change variables from ##x_1## and ##x_2## to ##X_c## and ##x##, where ##X_c## is the coordinate of the center of mass and ##x = x_2 - x_1##. This is a standard method for reducing the two-body problem to two independent one-body problems.

Hopefully you've seen this before. See the first 3 or 4 pages here: http://physics.oregonstate.edu/~corinne/COURSES/ph426/notes2.pdf
 
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TSny said:
I suggest that you change variables from ##x_1## and ##x_2## to ##X_c## and ##x##, where ##X_c## is the coordinate of the center of mass and ##x = x_2 - x_1##. This is a standard method for reducing the two-body problem to two independent one-body problems.

Hopefully you've seen this before. See the first 3 or 4 pages here: http://physics.oregonstate.edu/~corinne/COURSES/ph426/notes2.pdf
Thank you so much !
 

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