Three particles in a one-dimensional box of length L.

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Homework Help Overview

The problem involves three particles of mass m in a one-dimensional box of length L, focusing on finding a complete set of wavefunctions for the system. The original poster attempts to navigate the complexities of many-body quantum mechanics without specific details on particle interactions or boundary conditions.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the nature of the particles (interacting or non-interacting) and their statistical properties (bosons or fermions). The original poster explores methods like mean-field theory and second quantization but expresses uncertainty about the most efficient approach. Questions arise about general methods for expressing wavefunctions and the implications of completeness.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem. Some guidance has been offered regarding the treatment of non-interacting particles and references to external resources for further clarification. There is no explicit consensus on the best approach yet.

Contextual Notes

The problem lacks specific details about particle interactions and boundary conditions, which are critical for determining the appropriate methods for solving it. The open-ended nature of the question contributes to the complexity of the discussion.

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Homework Statement


Three particles, each of mass m, reside in a 1D "box" of length L. Find a complete set of wavefunctions,\phi_{k}(x) for the system. In this sense, "complete" means that any state of the system,\psi(x) can be written as a superposition of the wavefunctions, \phi_{k}(x).

Homework Equations


The TISE and TDSE, as well as other standard QM expressions.

The Attempt at a Solution


Well, there are no applied fields/forces, so I think I'm correct in saying that the Hamiltonian is time-independent (please correct me if this is not the case). This is a many-body problem, so I've attempted to use methods such as mean-field theory (Hartree-Fock), and second quantization, but run into trouble because the question doesn't give any clues as to which particles are being considered, or any boundary conditions.
I'm not sure if this is the most elegant way to complete the problem. Am I missing something simple? I know that each particle will be described by a separate wavefunction, and each linear combination of wavefunctions will also be a solution to the TDSE. I suppose I'm having trouble knowing which method will be the most efficient way to solve this.
Any help would be massively appreciated!
 
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Are the particles interacting or not? And are they bosons or fermions?
 
I'm not sure, this is all the question gives me. I think the question is somewhat open-ended. This is the reason I suspected there was some sort of "simple" reasoning behind the answer. Is there a method of writing out the wavelengths in a general way?
 
If the particle are non-interacting, then \psi can be written as a product of three one-particle wave functions. The latter are just the solution to the particle in a box. Care has to be taken to ensure that the final wave function has the proper (bosonic/fermionic) symmetry.

If the particles are interacting, then the problem gets much more complicated...
 
Yeah, I figured as much. What do you think would be the best way to proceed if I work under the assumption that the particles are interacting?
 
I think you should take a look at example no 5.1 page 217 of introduction to quantum mechanics 2nd ed by david.j.griffiths
 
That's brilliant, it's pretty much the exact question I had! Unfortunately there doesn't seem to be an answer in the book? It just sort of states the problem...
 
If you are asking about completeness then you can use dirichlet's theorem see page
46 of the same book
 

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