Difference between Mixed State and Superposition

In summary: A mixed state is a statistical ensemble of pure states, and cannot be represented by a single ket. So, using vectors to represent a mixed state is not possible.In summary, a mixed state and a superposition are essentially the same in structure, but the difference lies in their physical meaning and context in which they are used. A mixed state is a classical probability distribution of pure states, while a superposition is a quantum state that can exist in multiple states at the same time. Mathematically, a mixed state can be expressed using a density operator, while a superposition can be expressed using state vectors. However, a mixed state cannot be represented by a single vector.
  • #1
Dragonfall
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What is the difference between a mixed state and a superposition?
 
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  • #2
From my modest experience, there is no real technical difference. Perhaps when you're talking about the net effects / measurables etc - you refer to it as a superposition; while you're talking about the constituent states etc - you refer to it as a mixed state?
 
  • #3
If I understand you correctly, by superposition, you mean a pure state (which is the opposite of mixed). A mixed state is sometimes also called a classical superposition.

For example, consider a photon which could be either right-handed or left-handed (equiv. circularly polarized in either clockwise or anticlockwise direction).

A superposition of these states would give you a photon with maybe a 50/50 chance of either polarization being measured, and would be linearly polarized, so it would pass through a polarizing filter at the correct orientation with high probability.

A mixed state might also have 50/50 chance of being either left or right handed, but this is a classical probability, so it is definitely in one state or the other, and would consequently have about a 50/50 chance of passing through a polarizer of any orientation.

Alternatively, with the double slit experiment, you need a superposition of the states of passing through each slit to get the standard interference pattern. If you measure which slit the electron goes through, but ignore the result, then you still have a 50/50 chance of going through either slit. However, this will be a classical probability not a quantum superposition, so it is a mixed state and you won't see the interference pattern.

You can get a mixed state from a pure one simply by looking at a part of a larger system. For the double slit experiment above, if you include the state of the measuring equipment and anything it has interacted with, it will still be in a pure state.
 
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  • #4
I understand them to basically be the same in structure, but the difference is the context in which they are used. I always see the term mixed state associated with the idea of a linear combination of projectors where as a superposition is a term that is used for any linear combination in ANY Hilbert space.

As an example, let [tex]\psi_1, \psi_2[/tex] be elements in a Hilbert space.
[tex]\psi=\lambda_1\psi_1+\lambda_2\psi_2[/tex] is a superposition of two vectors but is generally still regarded as a pure state. Technically the density operator
[tex]|\psi\rangle\langle\psi|[/tex] is a pure state.
Where as the density operator
[tex]\lambda_1|\psi_1\rangle\langle\psi_1|+\lambda_2|\psi_2\rangle\langle\psi_2|[/tex]
is a mixed state.
 
  • #5
comote said:
[tex]\psi=\lambda_1\psi_1+\lambda_2\psi_2[/tex] is a superposition of two vectors but is generally still regarded as a pure state. Technically the density operator
[tex]|\psi\rangle\langle\psi|[/tex] is a pure state.
Where as the density operator
[tex]\lambda_1|\psi_1\rangle\langle\psi_1|+\lambda_2|\psi_2\rangle\langle\psi_2|[/tex]
is a mixed state.

Those expressions agree with what I was saying. Taking linear combinations of state vectors is quantum superposition, but taking combinations of density operators is the same of classical superposition.

Also, if the two vectors are normalized, you must have [itex]|\lambda_1|^2+|\lambda_2|^2=1[/itex] in the first expression, but [itex]\lambda_1+\lambda_2=1[/itex], and [itex]\lambda_1,\lambda_2\ge 0[/itex] in the second one.

In the second case, there is no way to distinguish between that state and the case where it is either in the definite state [itex]\psi_1[/itex] or in state [itex]\psi_2[/itex], and where you just don't know which one due to lack of knowledge. So, no quantum interference between the states occurs.
Mathematically, they are both just different types of linear combinations, but they have a very different meaning physically.
 
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  • #6
How do you express a mixed state using vectors?
 
  • #7
Dragonfall said:
How do you express a mixed state using vectors?

In general a mixed state (or statistical mixture) writes with the density matrix as follows :
[tex] \hat{\rho}=\sum_{\alpha} p_{\alpha} \left| \psi_p \rangle \langle \psi_p \right| [/tex]
Where [tex] p_{\alpha} [/tex] is the probability for the system to be in the state [tex] \left| \psi_{\alpha} \rangle [/tex] (that is not necessarily an eigen state). These [tex] p_{\alpha}[/tex] can be derived from expermimental data or by a priori assumptions.

The only cases for which a mixed state is equivalent to a superposition is when there exist a state [tex] \left|\psi_{\alpha_0} \rangle[/tex] whose [tex] p_{\alpha_0} =1 [/tex] (therefore we have [tex] p_{\alpha} =0 [/tex] for [tex] \alpha \: \neq \: \alpha_0 [/tex] ).

In this case you get a pure state and the density matrix writes :

[tex] \hat{\rho} = \left| \psi_{\alpha_0} \rangle \langle \psi_{\alpha_0} \right| [/tex]

EDIT : To answer straight forwardly to the question asked, you can't express a mixed state using only the ket notation.
 
1)

What is the difference between mixed state and superposition?

A mixed state refers to a quantum system that is described by a probabilistic combination of multiple pure states. In contrast, superposition refers to a quantum system that exists in a combination of two or more pure states simultaneously.

2)

Can a system be in both a mixed state and superposition at the same time?

No, a system can only be in either a mixed state or superposition at a given time. The two concepts are mutually exclusive and describe different types of quantum systems.

3)

How is a mixed state different from a classical probability distribution?

A classical probability distribution describes the uncertainty of a classical system, while a mixed state describes the uncertainty of a quantum system. In a classical probability distribution, the uncertainty arises from a lack of knowledge about the system, while in a mixed state, the uncertainty is inherent in the quantum nature of the system.

4)

What is the role of measurement in determining the state of a system in superposition?

Measurement plays a crucial role in determining the state of a system in superposition. When a measurement is made, the superposition collapses into one of the possible pure states, and the outcome of the measurement is one of the possible values associated with that state.

5)

Can superposition exist in macroscopic objects?

While superposition is a fundamental concept in quantum mechanics, its effects are usually only observed at the microscopic level. Macroscopic objects are typically described by classical mechanics and do not exhibit the same quantum behaviors as subatomic particles.

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