A question about "entanglement monogamy"

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Discussion Overview

The discussion revolves around the concept of "entanglement monogamy" in quantum mechanics, particularly focusing on the implications of a particle (A) becoming entangled with a macroscopic system and how this affects its entanglement with another particle (B). Participants explore theoretical implications, measurement processes, and the nature of entangled states.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants propose that if particle A becomes entangled with a macroscopic system, it may reduce the entanglement with particle B, suggesting that the degree of entanglement between A and B must be less than maximal.
  • Others argue that entangled particles A and B do not have separate existence until observed, implying that the act of measurement can break the entanglement.
  • A participant mentions that measuring one of an entangled pair without prior knowledge of their entanglement will not provide information about the other particle, as it will appear in a mixed state.
  • Another viewpoint is that to infer the spin of an entangled partner, one must know that the particles are entangled, and measurements must be performed on multiple pairs to establish correlations beyond random chance.
  • Some participants discuss the nature of the quantum system involving the environment, particle A, and particle B, suggesting that interactions with the environment can lead to a loss of entanglement between A and B.

Areas of Agreement / Disagreement

The discussion contains multiple competing views regarding the implications of entanglement monogamy and the nature of measurements in quantum mechanics. There is no consensus on whether the entanglement between A and B is reduced when A interacts with another system.

Contextual Notes

Participants express uncertainty about the interpretation of quantum mechanics, including the nature of measurement and the existence of particles prior to observation. There are unresolved questions regarding the implications of entanglement and the conditions under which it may be affected.

T S Bailey
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Suppose we have a particle pair (A, B) which are maximally entangled. Then A goes cavorting with some macroscopic system in a thermodynamically irreversible way, and becomes highly entangled with it. Does this entanglement with the new system reduce the entanglement between A and B? At first I want to say no, because if we were to measure a maximally entangled quanta and found it spinning one way (for example) we can immediately deduce the direction of spin for its partner. But since a measurement is just a process of sufficient interaction to produce entanglement with the measured quanta, and because only two systems may be maximally entangled with one another, I imagine that the degree of entanglement between A and B must now be something less than maximal. What am I missing?
 
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T S Bailey said:
Suppose we have a particle pair (A, B) which are maximally entangled. Then A goes cavorting with some macroscopic system in a thermodynamically irreversible way, and becomes highly entangled with it.

That's a mistake right off the bat.

For entangled particles A and B do not have separate existence.

Most certainly you can break the entanglement by observing just A or B - but prior to observation you can't say A or B have a separate existence.

Thanks
Bill
 
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T S Bailey said:
Suppose we have a particle pair (A, B) which are maximally entangled. Then A goes cavorting with some macroscopic system in a thermodynamically irreversible way, and becomes highly entangled with it. Does this entanglement with the new system reduce the entanglement between A and B?

Yes. That is what monogamy of entanglement means.

T S Bailey said:
At first I want to say no, because if we were to measure a maximally entangled quanta and found it spinning one way (for example) we can immediately deduce the direction of spin for its partner. But since a measurement is just a process of sufficient interaction to produce entanglement with the measured quanta, and because only two systems may be maximally entangled with one another, I imagine that the degree of entanglement between A and B must now be something less than maximal. What am I missing?

If you measure just one of an entangled pair without knowing that it was one of an entangled pair, measuring one will not tell you anything about the other particle. You will just think the particle you measured is in a mixed state.

Also, a measurement will break the entanglement between A and B.
 
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So if we were to perform an experiment like that described in the EPR paradox we could never infer the spin of the entangled partner? If that's the case then why is there confidence that entangled states exist at all?
 
T S Bailey said:
So if we were to perform an experiment like that described in the EPR paradox we could never infer the spin of the entangled partner?
You have to know in some other way (usually because you know how it was produced) that you have an entangled pair. If you know this, then when you measure the spin of one particle on a given axis you will know what the result would be if a measurement along the same axis is performed on the other particle.
then why is there confidence that entangled states exist at all?
Conversely, if you have a black box that is producing particle pairs and you want to know whether they are entangled, you have to perform measurements on both members of many pairs and then compare results. A single pair won't tell us anything - we'll get opposite results on the same axis 50% of the time just by random chance. But when we do many pairs and get correlations much higher than 50% we know that there is some sort of relationship between the two particles.
 
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T S Bailey said:
Does this entanglement with the new system reduce the entanglement between A and B? At first I want to say no, because if we were to measure a maximally entangled quanta and found it spinning one way (for example) we can immediately deduce the direction of spin for its partner. But since a measurement is just a process of sufficient interaction to produce entanglement with the measured quanta, and because only two systems may be maximally entangled with one another, I imagine that the degree of entanglement between A and B must now be something less than maximal. What am I missing?

We start with a quantum system consisting of the environment around A, the particle A, and the particle B. The initial state of this system is a superposition of "The environment is what it is; A is spin-up and B is spin-down" and "The environment is what it is; A is spin-down and B is spin-up"; in this state A and B are entangled. When A interacts with the environment around it, the system transitions (collapses? evolves? MWI branches? The interpretation doesn't matter) into one of two possible result states:
1) "A is spin-up and the environment is consistent with A being spin-up; B is spin-down"
2) "A is spin-down and the environment is consistent with A being spin-down; B is spin-up"
These are states in which A and the environment are entangled while A and B are not. If the environment happens to include some sort of readout (for example a dial with a needle that points up or down according to A's spin) then we will be able to know A's spin and what the result of a measurementof B's spin on that axis would be by examining that part of the environment and we'll call the interaction a measurement.

Thus, monogamy is respected and we get to know B's spin as well.
 
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T S Bailey said:
So if we were to perform an experiment like that described in the EPR paradox we could never infer the spin of the entangled partner? If that's the case then why is there confidence that entangled states exist at all?

Of course you can. What you can't do is say it has the property of spin, or even a separate existence, until you observe it.

Remember QM is a theory about observations. What's going on, and that includes if objects have an existence independent of other objects, when not observed, its silent about.

Thanks
Bill
 

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