Why doesn't this FTL communication scheme work?

Click For Summary

Discussion Overview

The discussion revolves around the feasibility of using entangled particles for faster-than-light (FTL) communication, specifically examining whether Alice can send information to Bob by manipulating the states of entangled particles. The scope includes theoretical considerations of quantum mechanics and entanglement, as well as the implications of measurement on entangled states.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants propose that Alice could send information by selectively flipping the state of entangled particles, suggesting that a measurement could indicate a change in state.
  • Others argue that Alice cannot selectively flip the state of particles without breaking the entanglement, leading to a 50-50 mix of outcomes for Bob regardless of Alice's actions.
  • A later reply clarifies that while Alice can choose a measurement basis, this does not allow her to control the outcome of Bob's measurements, which remain random until correlated.
  • Some participants mention that measuring Alice's particle breaks the entanglement, making any subsequent state manipulation irrelevant to Bob's measurements.
  • One participant references a method involving Raman transitions, suggesting it could allow for state manipulation after measurement, but others challenge this by stating it does not enable FTL communication.
  • There is a discussion about whether specific operations could selectively break entanglement based on particle states, with some asserting that such operations are not possible.

Areas of Agreement / Disagreement

Participants generally disagree on the possibility of using entangled particles for FTL communication. While some explore the theoretical potential of manipulating states, others firmly state that the fundamental principles of quantum mechanics prevent such communication methods.

Contextual Notes

The discussion highlights limitations in understanding the implications of measurement on entangled states and the conditions under which entanglement can be manipulated. There are unresolved details regarding the specific operations that could affect entanglement and the assumptions underlying the proposed methods.

Christofer Br
Messages
51
Reaction score
0
If Alice and Bob had a large number of particles entangled together (with state of either 0 or 1), could Alice send information by breaking the entanglement of particles with state of 1 (by flipping the state for example) so that Bob measures 50% of particles to be in the state opposite of 0, that is 1, plus half of the remaining 50% to be in state of 1 (due to 50/50 chance for measurement of either state in the disentangled pairs) resulting in 75% of the states to be 1 - indicating that Alice has broke the entanglement, which would be the information (one bit)?
 
Physics news on Phys.org
Christofer Br said:
If Alice and Bob had a large number of particles entangled together (with state of either 0 or 1), could Alice send information by breaking the entanglement of particles with state of 1 (by flipping the state for example) so that Bob measures 50% of particles to be in the state opposite of 0, that is 1, plus half of the remaining 50% to be in state of 1 (due to 50/50 chance for measurement of either state in the disentangled pairs) resulting in 75% of the states to be 1 - indicating that Alice has broke the entanglement, which would be the information (one bit)?
It doesn't work because Alice can't selectively flip the state of the particles with spin 1 because she doesn't know which they are. Anything that Alice does to her particles is just as likely to turn a one into a zero at Bob's end as to turn a zero into one, so Bob end up with a 50-50 mix no matter what Alice does.

If there were a way of preparing entangled pairs so that up front Alice knew which particles she would measure to be in one state or the other (or even if on average Alice's partcles were more likely to be in one state than the other) it would be possible to send a signal as you describe. But such a preparation is impossible, and indeed this is baked into the mathematical definition of the entangled state.
 
Just to add to Nugatory's correct answer:

Alice can select a measurement basis for the particle she gets. That measurement basis *is* shared with Bob's particle. In other words, that is the only manner in which she affects Bob. There is no other transformation at Alice's end that Alice can control that would be shared with Bob's particle.

And as fate has it, there is no measurement possible on Bob's side alone that allows him to detect what measurement basis Alice has chosen. Every measurement he makes will yield a random outcome. (Only when Alice and Bob's measurements are brought together do any correlations appear.)
 
Nugatory said:
It doesn't work because Alice can't selectively flip the state of the particles with spin 1 because she doesn't know which they are. Anything that Alice does to her particles is just as likely to turn a one into a zero at Bob's end as to turn a zero into one, so Bob end up with a 50-50 mix no matter what Alice does.

If there were a way of preparing entangled pairs so that up front Alice knew which particles she would measure to be in one state or the other (or even if on average Alice's partcles were more likely to be in one state than the other) it would be possible to send a signal as you describe. But such a preparation is impossible, and indeed this is baked into the mathematical definition of the entangled state.
I've read about raman transition which is exactly what i described, a method to flip the state of a particle with laser AFTER it has been measured, so that the entaglement with bobs particles is broken and their state in upcoming measurment will be independent
 
Christofer Br said:
I've read about raman transition which is exactly what i described, a method to flip the state of a particle with laser AFTER it has been measured,
It's easy enough to flip the state of Alice's particle after it has been measured, but the act of measuring her particle breaks the entanglement so the subsequent flip doesn't affect Bob's measurement. Alice knows that if Bob had measures his particle he'll get the opposite of whatever she measured; Bob knows the same thing about Alice's particle, but has no way of knowing whether Alice has subsequently flipped it.

If that's not consistent with what you read, post up a link to it so we can find where the misunderstanding is.
 
Nugatory said:
It's easy enough to flip the state of Alice's particle after it has been measured, but the act of measuring her particle breaks the entanglement so the subsequent flip doesn't affect Bob's measurement. Alice knows that if Bob had measures his particle he'll get the opposite of whatever she measured; Bob knows the same thing about Alice's particle, but has no way of knowing whether Alice has subsequently flipped it.

If that's not consistent with what you read, post up a link to it so we can find where the misunderstanding is.

https://www.google.pl/amp/s/www.for...nt-allow-faster-than-light-communication/amp/

The part starts with "the answer is to"
Bob would know alice has" flipped" because he would get result of 75% of (1) state instead of 50% each.
 
No plan that Alice has for operations to perform on her half of an entangled pair can change Bob's expectation for measuring his half away from 50/50.

The reason your specific plan won't work is that there is no operation that "breaks the entanglement of particles with state of 1 [but not with state 0]". In order to determine that the particle has a state of 1 or not, you must have already broken the entanglement. (Alternatively you may have moved the entanglement into different qubits instead of breaking it. The specific problem depends on unstated details of your plan.)

For example, in the Forbes article you quoted in your latest post they say:

If you choose your states carefully, you can arrange it so that an atom in state 0 will absorb the laser and flip its state, but an atom in state 1 won't interact with the laser at all.

This is an example of an operation that moves the entanglement. The qubit that was being stored in the particle's 0-vs-1 state has been moved into the presence-vs-absence of a photon in the laser beam (or something like that). The entanglement wasn't destroyed, it was moved. Then Alice's equipment records a dip (or no dip) in the laser beam, completing the measurement process that happened to be started by moving the quantum information into something easier to work with.

(Actually, I don't know anything about trapped ions. Other sentences in the article imply that the 0 state is flipping some state of the photon, in which case the information is being copied instead of moved. Regardless of those details, this is not a selective destroy-entanglement-if-1 process.)
 
  • Like
Likes   Reactions: MichPod

Similar threads

  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 41 ·
2
Replies
41
Views
6K
  • · Replies 19 ·
Replies
19
Views
3K
  • · Replies 148 ·
5
Replies
148
Views
16K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 63 ·
3
Replies
63
Views
10K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 19 ·
Replies
19
Views
2K