Bell State of two non-orthogonal modes

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Discussion Overview

The discussion revolves around the possibility of creating a Bell state using two non-orthogonal polarizations of a photon, specifically examining the state represented as |10⟩ + |01⟩. Participants explore the implications of non-orthogonality on the properties of such a state, including its entanglement characteristics and measurement outcomes.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants question whether a Bell state can be defined using non-orthogonal states, noting that they would not yield the typical anticorrelation statistics associated with Bell states.
  • Others argue that while a state like |10⟩ + |01⟩ can be constructed, it does not possess the properties of a maximally entangled Bell state due to the non-orthogonality of the basis states.
  • A participant expresses a desire to understand the conceptual implications of the state without converting it to an orthogonal basis, despite acknowledging that calling it a Bell state may be incorrect.
  • There is a discussion about the linear independence of the non-orthogonal states, with some participants asserting that they can still span a space despite not being orthogonal.
  • One participant points out that measurement must be analyzed in the context of orthogonal eigenstates, suggesting that the original non-orthogonal representation may lead to incorrect conclusions about measurement outcomes.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether a Bell state can be appropriately defined with non-orthogonal states. There are competing views on the implications of non-orthogonality for entanglement and measurement outcomes, and the discussion remains unresolved.

Contextual Notes

Participants highlight limitations in their understanding of the notation and the implications of non-orthogonality, indicating that some foundational concepts may be under discussion without full clarity.

McLaren Rulez
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Is this possible? If I have, say a photon and two non-orthogonal polarizations [itex]\mid0\rangle[/itex] and [itex]\mid1\rangle[/itex], can I create a Bell state [itex]\mid10\rangle+\mid 01\rangle[/itex]

If not, what is the reason?

Thank you :)
 
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Anyone?

I understand that I won't get the anticorrelation statistics but does it makes sense to describe a Bell state of non-orthogonal subsystems? That is, can the object [itex]\mid10\rangle+\mid 01\rangle[/itex] exist regardless of what statistics it gives under measurement?
 
McLaren Rulez said:
Anyone?

I understand that I won't get the anticorrelation statistics but does it makes sense to describe a Bell state of non-orthogonal subsystems? That is, can the object [itex]\mid10\rangle+\mid 01\rangle[/itex] exist regardless of what statistics it gives under measurement?

I must confess that I don't understand your notation. If [itex]\mid0\rangle[/itex] and [itex]\mid1\rangle[/itex] are possible states of a single photon, I'd understand what was meant by something like [itex]\frac{\mid0\rangle+\mid1\rangle}{\sqrt{2}}[/itex], but I'm not sure what to make of [itex]\mid10\rangle[/itex] or a "Bell state".
 
McLaren Rulez said:
I understand that I won't get the anticorrelation statistics but does it makes sense to describe a Bell state of non-orthogonal subsystems?
I don't think it makes sense to write it that way, but you can construct such a state. However, it won't have the properties of a Bell state because [itex]\mid10\rangle+\mid 01\rangle[/itex] is not maximally entangled if the two "basis" states are not orthogonal.

To see how such a state would look like in the usual basis, you can simply decompose one of the "basis" states and calculate the resulting state. For example |1>=a|0>+b|1'> where |1'> is orthogonal to |0>.
 
kith said:
I don't think it makes sense to write it that way, but you can construct such a state. However, it won't have the properties of a Bell state because [itex]\mid10\rangle+\mid 01\rangle[/itex] is not maximally entangled if the two "basis" states are not orthogonal.

To see how such a state would look like in the usual basis, you can simply decompose one of the "basis" states and calculate the resulting state. For example |1>=a|0>+b|1'> where |1'> is orthogonal to |0>.

Thank you for your reply. I don't want to look at it in the usual basis; I want to stay in this non orthogonal basis. Just to understand this from a conceptual point of view.

I see that calling it a Bell state is probably wrong. But the idea is that we have two non orthogonal polarizations [itex]0[/itex] and [itex]1[/itex].

Now, the state [itex]\mid10\rangle+\mid 01\rangle[/itex] is a state such that if Alice measures and finds the first photon is polarized along [itex]0[/itex] and Bob sends his photon through a polarizer in direction [itex]1[/itex] and puts a detector after that, then Bob's detector will always register a click.

Is this correct?
 
McLaren Rulez said:
Now, the state [itex]\mid10\rangle+\mid 01\rangle[/itex] is a state such that if Alice measures and finds the first photon is polarized along [itex]0[/itex] and Bob sends his photon through a polarizer in direction [itex]1[/itex] and puts a detector after that, then Bob's detector will always register a click.

Is this correct?
No. If you make a measurement, you have to decompose your state into the (orthogonal) eigenstates of the measurement operator. To analyze your situation, you have to write the state in Alice's basis (0, 1') first. If you don't do this, you get incorrect results. For example, Alice's probability to measure 0 is bigger than 1/2, because the second term contains an additional part a|0>.

Having written the state in Alice's basis, you can do the state reduction and you will see that the final state is not equal to |01>.

McLaren Rulez said:
I don't want to look at it in the usual basis; I want to stay in this non orthogonal basis.
You probably know this, but just to be clear: your "basis" is not really a basis because its elements are not linearly independent.
 
Last edited:
Okay I wrote out [itex]\frac{1}{\sqrt{2}}(\mid0,+\rangle\ +\mid +,0\rangle)[/itex] and it turns out to be [itex]\frac{1}{2}(2\mid0,0\rangle\ +\mid 1,0\rangle\ +\mid 0,1\rangle)[/itex]. I see what you mean about the statistics being not so trivial.

A final query though: I thought that my vectors are indeed linearly independent, though not orthogonal? I can get any state vector I want with combinations of [itex]\mid0\rangle[/itex] and [itex]\mid+\rangle[/itex]. I thought that them being non orthogonal is the problem. Or is there something basic that I am missing?

Thank you for your replies!
 
McLaren Rulez said:
A final query though: I thought that my vectors are indeed linearly independent, though not orthogonal? I can get any state vector I want with combinations of [itex]\mid0\rangle[/itex] and [itex]\mid+\rangle[/itex]. I thought that them being non orthogonal is the problem. Or is there something basic that I am missing?
Sorry, I have missed something basic. ;-) You are of course right about this.
 
Thank you kith! I appreciate your help very much :)
 
  • #10
You're welcome. :smile:
 

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