Mixed Quantum States: Definition, Uses & Homework

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SUMMARY

The discussion centers on mixed quantum states, defined as statistical ensembles of pure quantum states represented by a probability distribution. Mixed states are essential in quantum mechanics as they describe systems lacking complete information, such as unpolarized light, and are characterized by the density matrix ρ. The phenomenon of decoherence transforms pure states into mixed states, highlighting their role in quantum experiments. Understanding mixed states is crucial for solving various quantum mechanics problems, particularly those involving statistical properties and measurement outcomes.

PREREQUISITES
  • Quantum mechanics fundamentals
  • Density matrix formalism
  • Concept of decoherence
  • Statistical ensembles in quantum physics
NEXT STEPS
  • Explore the implications of decoherence in quantum systems
  • Study the mathematical formulation of density matrices
  • Investigate the differences between pure and mixed states in quantum experiments
  • Learn about applications of mixed states in quantum information theory
USEFUL FOR

Quantum physicists, students of quantum mechanics, and researchers in quantum information science will benefit from this discussion on mixed quantum states and their applications.

Tac-Tics
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I have a book on quantum computation that explains the concept of a mixed quantum state. The definition is pretty plain, you just have a boring probability distribution over a set of quantum states.

What I would like to know is why we need mixed states. How are they represented physically in nature. What kind of leverage do they give us over pure states in describing an experiment? What kinds of homework problems would you expect to solve using them ;-)
 
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Tac-Tics said:
I have a book on quantum computation that explains the concept of a mixed quantum state. The definition is pretty plain, you just have a boring probability distribution over a set of quantum states.

What I would like to know is why we need mixed states. How are they represented physically in nature. What kind of leverage do they give us over pure states in describing an experiment? What kinds of homework problems would you expect to solve using them ;-)

Mixed states are standard statistical ensembles of "pure" quantum states, and they appear whenever we don't have complete information of the quantum state, pretty much in the same way as in classical physics. For instance, if you have a beam of "unpolarized" light, then you represent this as a mixed state of "up" and "down" spins for the photons. This is entirely different from a superposition of "up" and "down", which would result in just another polarization state, and which would show "interference" effects.

Now, there can be a funny interplay between the statistical properties of mixed states, and the statistical properties of the measurement results of a pure quantum state.

In a way, you can see a mixed state as "a superposition without interference effects". In fact, quantum mechanics manifests itself as the possibility to come up with different results than that of a mixed state, in a true superposition (a pure state).
Decoherence is the phenomenon of turning superpositions in mixed states.
 
vanesch said:
In a way, you can see a mixed state as "a superposition without interference effects". In fact, quantum mechanics manifests itself as the possibility to come up with different results than that of a mixed state, in a true superposition (a pure state).
Decoherence is the phenomenon of turning superpositions in mixed states.

How would you go about preparing a particle in a mixed state?
 
Tac-Tics said:
How would you go about preparing a particle in a mixed state?

The same way you prepare a dice to be in a mixed state :smile:

Seriously, a mixed state is an ensemble description. In fact, one of the peculiar things about the interplay between mixed state statistics and quantum statistics is that considering particles in a "mixed state" is indistinguishable from considering them in a randomly drawn pure state if that random drawing gives a statistically equivalent description as the mixed state. Worse, there are *different* ensembles of *different* pure states which are all observationally indistinguishable from the "mixed state". What describes a mixed state, or all of these ensembles, is the density matrix rho.

Simple example:
the mixed state "unpolarized electron".

You can see it as 50% |x+> and 50% |x-> (an ensemble of pure states)
or you can see it as 50% |z+> and 50% |z-> (another ensemble of pure states)
or you can see it as 25% |x+>, 25%|x->, 25%|z+> and 25% |z-> (yet another ensemble of pure states)
etc...

they are all observationally indistinguishable. They are all described by one and the same density matrix rho:
1/2 0
0 1/2
 

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