Superposition & Mixture : Preparation and Representation of

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Discussion Overview

The discussion revolves around the concepts of superposition and mixtures in quantum mechanics, specifically focusing on the preparation and representation of mixtures using Gaussian wavefunctions and density matrices. Participants explore the implications of these concepts in theoretical contexts.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • One participant questions how to prepare a mixture similar to the example of two non-overlapping Gaussian wavefunctions discussed in an article.
  • Another participant challenges the assertion that a mixture cannot be represented by a wavefunction, suggesting that mixed states can be expressed using orthogonal states and providing a specific formulation.
  • A participant seeks clarification on the specific nature of the states ##|+\rangle## and ##|-\rangle## mentioned in the context of the mixed state representation.
  • One participant responds that ##|+\rangle## and ##|-\rangle## are simply two states from an auxiliary space.

Areas of Agreement / Disagreement

Participants express differing views on the representation of mixtures and superpositions, with no consensus reached on the correctness of the initial claim regarding wavefunction representation.

Contextual Notes

The discussion includes assumptions about the nature of states and their orthogonality, as well as the implications for symmetry breaking, which are not fully resolved.

Swamp Thing
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I have been reading this explanation about superpositions and mixtures. The author takes the example of two non-overlapping regions in space, each covered by a gaussian wavefunction. He goes on to compare the superposition and the mixture made up of those two gaussian functions, based on their different representations in terms of their density matrices.

My question is, how would one actually prepare a mixture exactly like the example discussed there?
 
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The article states that a mixture cannot be represented by a wavefunction. This isn't completely correct. E.g. introducing additional states ##|+\rangle## and ##|-\rangle##, which are supposed to be orthogonal, you can write the mixed state as ## p_1|\psi_1\rangle |+\rangle+p_2 |\psi_2\rangle |-\rangle##.
This is especially important in symmetry breaking, where (sub)spaces with different symmetry become orthogonal.
 
What would ##|+\rangle## and ##|-\rangle## be in the example that he talks about?
 
Just two states from an auxillary space.
 

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