Must ensembles be homogeneous?

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Discussion Overview

The discussion revolves around the concept of ensembles in quantum mechanics, specifically whether ensembles must be homogeneous or if they can include mixed states. Participants explore the definitions and implications of pure and mixed states, as well as the conditions under which different types of ensembles can be considered valid.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that an ensemble consists of systems prepared in the same way, questioning if this implies all systems must be in the same state.
  • One participant mentions that a pure state can be prepared, but expresses uncertainty about preparing a statistical mixture.
  • Another participant explains that a mixed state can be represented by a density matrix and can be prepared through measurements without sorting outcomes.
  • It is noted that a mixed state can arise from entangled systems, where the reduced density matrix of a subsystem may be mixed.
  • Concerns are raised about the validity of using an ensemble with specific proportions of states (30% in state s and 70% in state t) to represent a mixed state, questioning whether this constitutes a proper or improper mixture.
  • One participant argues that a proper mixture can be created by randomly mixing pure ensembles, while another emphasizes that the state described can be a proper mixture if the states are pure and the weights sum to one.

Areas of Agreement / Disagreement

Participants express differing views on the nature of mixed states and the validity of certain ensembles. There is no consensus on whether the ensemble described in the original post is a proper or improper mixture, indicating ongoing debate and uncertainty.

Contextual Notes

Participants highlight the importance of the definitions of proper and improper mixtures, as well as the conditions under which ensembles can be considered valid. The discussion reflects a range of assumptions and interpretations regarding quantum states and measurements.

normvcr
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An ensemble is a collection of systems, all prepared in the same way. Does this mean that all the systems are in the same state? I have seen some authors create ensembles where 30% of the systems are in a state, s, and 70% of the systems are in a state, t . As far as measurements go, this ensemble represents the mixed state 0.3 s + 0.7 t . Is this accepted as a valid ensemble for this mixed state?
 
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Yes, the same pure state per individual system. It's one of the underlying (i.e. not explicit) assumptions in QM: the ability to prepare a system in a certain state.
 
What about the mixed (non-pure) state example that is in the original post?
 
I honestly don't know how to physically prepare a statistical mixture. A pure one can be done through a Stern-Gerlach type of experimental setup. So, sorry for not helping more, I'm rather into the mathematical delopments of QM than to the their connection with real-life experiments.
 
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Thanks for the info. Perhaps, someone else will know about ensembles of mixed states.
 
Yes, the ensemble can be mixed - it can be any ensemble that is represented by a density matrix. One way to prepare a mixed state is to perform a measurement, but don't sort according to the outcome. The ensemble will be a statistical mixture of all possible measurement outcomes. The mixed density matrix prepared by ignorance of a measurement outcome is called a "proper mixture".

A mixed state can also be prepared by preparing a system that is in a pure state. If the subsystems are entangled, then the reduced density matrix of a subsystem will be mixed. As an example of a mixed state preparation, take a Bell state of a pair of spins. The Bell state is a pure state. If you make observations on only one spin in the entangled pair, the reduced density matrix describing the state of that spin is mixed. The mixed density matrix prepared by ignorance of some degrees of freedom in a total pure state is called an "improper mixture".

There is a relationship between the two ways of preparing a mixed state. Take the Bell state again. If we always measure on spin A first, we will cause the wave function to collapse. However, the person measuring spin B, if performing his measurement locally and not sorting according to the outcome of the measurement on spin A, will basically be doing a measurement on a mixed state prepared by measurement followed by not sorting. This is an example of local measurements being completely unable to distinguish between proper and improper mixtures. Nonlocal measurements can distinguish between them.
 
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Thank you for the detailed response. From the question in the original post, the mixed state 0.3 s + 0.7 t is represented by the ensemble having 30% of the systems in state s and 70% of the systems in state t, but this is not a proper mixture unless the states s and t happen to be the two eigen states of a measurement operator, with eigenvalues 0.3 and 0.7, respectively. Do you see any problem with using this ensemble, which is neither proper nor improper, to represent the mixed state?
 
normvcr said:
Thank you for the detailed response. From the question in the original post, the mixed state 0.3 s + 0.7 t is represented by the ensemble having 30% of the systems in state s and 70% of the systems in state t, but this is not a proper mixture unless the states s and t happen to be the two eigen states of a measurement operator, with eigenvalues 0.3 and 0.7, respectively. Do you see any problem with using this ensemble, which is neither proper nor improper, to represent the mixed state?

You understand about proper and improper mixtures :D:D:D:D:D:D:D.

Improper ones happen all the time due to decoherence.

Proper ones are easily done simply by randomly mixing up pure ensembles. Say for axample you want 1/6th in a certain pure state and 5/6th in another pure state simply take a dice, throw it, and every time you get a 1 select it from one state otherwise from another. Do that a large number of times.

I will leave you to think about the implications of the fact it can conceptually be made as large as you like, but not infinite. Its the same issue you get in stochastic models used in applied math all the time.

Thanks
Bill
 
normvcr said:
Thank you for the detailed response. From the question in the original post, the mixed state 0.3 s + 0.7 t is represented by the ensemble having 30% of the systems in state s and 70% of the systems in state t, but this is not a proper mixture unless the states s and t happen to be the two eigen states of a measurement operator, with eigenvalues 0.3 and 0.7, respectively. Do you see any problem with using this ensemble, which is neither proper nor improper, to represent the mixed state?

The state you describe is a proper mixture for any s and t that are pure states. A proper mixture is just a statistically weighted mixture of any pure states, so as long as the relative weights add up to 1, it's ok. http://en.wikipedia.org/wiki/Density_matrix
 

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