Can we look upon entanglement as measurement?

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SUMMARY

The discussion centers on the interpretation of the state of entangled photons, specifically the global state |Phi> = (|H>|V> + |V>|H>)/sqrt2. Using density operator formalism, the reduced density operator for one photon is derived as rho_right = Tr_left(rho) = (1/2) (|H> PREREQUISITES

  • Quantum mechanics fundamentals, particularly entanglement and superposition.
  • Density operator formalism in quantum mechanics.
  • Understanding of polarization states of photons.
  • Familiarity with the concept of partial trace in quantum systems.
NEXT STEPS
  • Study the implications of the density operator formalism in quantum mechanics.
  • Explore the differences between statistical mixtures and superpositions in quantum states.
  • Learn about the measurement theory in quantum mechanics, focusing on entangled systems.
  • Review the paper referenced in the discussion: "http://arxiv.org/abs/1301.1673" for deeper insights into photon entanglement.
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Quantum physicists, researchers in quantum information science, and students studying quantum mechanics who seek to understand the nuances of photon entanglement and measurement interpretations.

Albert V
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Hi,

I have a question about how to interpret the state of an entangled photon

H = horisontal, V = vertical polarization



The global state is |Phi> = (|H>|V> + |V>|H>)/sqrt2.

By density operator formalism:

rho = |Phi><Phi|
= (1/2) ( |H>|V><H|<V| + |H>|V><V|<H| + |V>|H><H|<V| + |V>|H><V|<H| ).

in order to find the state on the right side, trace out the left side :

rho_right = Tr_left(rho) = (1/2) (|H><H|+|V><V|),

How should this state be interpreted? 1) as a photon EITHER in H OR V, or 2) a mixed state (superposition) containing components of both the left and the right side.

This would help me to understand this paper:

http://arxiv.org/abs/1301.1673
 
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First of all, you start with a two-photon state with entangled photons. It's a pure state given by a normalized state ket |\Phi \rangle. The corresponding statistical operator of the pure state is the projection operator \hat{\rho}_{2 \gamma}=|\Phi \rangle \langle \Phi|. This gives you the statistical properties on the polarization of both photons according to Borns rule.

Now you want to forget about the fact that you deal with a two-photon state and only know about the polarization state state of one photon. Thus you trace over the other photon's polarization states to end up with your reduced density operator \hat{\rho}_{\text{right}}=1/2 \mathbb{1}. This shows that an observer only looking at this photon's polarization measures an totally unpolarized beam of photons, i.e., he finds with probability 1/2 either a horizontally or a vertically polarized photon, and that's it.
 
Thanks for your answer, but when you say a "totally unpolarized beam of photons" does that imply a statistical mixture of states? Under the discussion: "What is the difference between entangled and "normal" photons?" another Sci Advisor said that:

"When you discard information about the other particle, you are left with a statistical mixture. (mathematically, this amounts to taking a partial trace)"

A statistical mixture of states is not equivalent to a linear superposition of states.
 
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