- #1
msumm21
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- TL;DR Summary
- Trying to better understand the measurement problem in the context of a simple experiment
I’m trying to understand the measurement problem using the simplest experiment I can think of--passing a particle P through a 50/50 beam splitter S, sending it down “path A” or “path B” with equal probability. Each path has a detector that can tell us if P was in that path. The detectors “amplify the signal” to eventually reach our "brain" through a series of interactions. Consider path A. P first interacts with some particle A1, which then interacts with A2, then A3, … until something AN reaches our "brain" to tell us the particle was detected in path A. Likewise in path B: B1,B2,...,BN.
Simple Analysis
P passes S and enters the state A+B before encountering any part of a detector. Upon encountering A1/B1 it becomes entangled in the state ##A\otimes A1 + B\otimes B1## (abusing notation here so that A1 here represents P interacting with the 1st part of the detector in path A). At this point entanglement destroys the pure state of P itself (P itself is in a mixed state, disallowing interference), but the pure state of the larger system remains: interference is possible using the bigger system of P, A1 and B1.
After the next interaction with A2/B2 the state becomes ##A \otimes A1 \otimes A2 + B \otimes B1 \otimes B2 ##. Now P with the first portion of the detectors decohered, but by including the 2nd part of the detectors we could still produce interference between the two alternatives A/B.
Above repeats to A3/B3, A4/B4, ... until we "see a flash" from detector A or B (via AN or BN).
Interpretations / Questions
Decoherence
Some people reportedly believe decoherence solves the measurement problem. In the context of this experiment, do some believe that decoherence of P after interacting with the first portion of the measuring device constitutes collapse? If so, how do they explain the interference that can occur in the larger system P,A1,B1? If not, how do they mark a particular step where collapse occurred?
Pilot-wave theory
If, at any time in this experiment, interference between the two paths can be created, then when & how do you reveal which path P actually went down? When does the pilot wave "disappear" from the path that doesn't contain P?
Any other interesting interpretations or points about this experiment?
Simple Analysis
P passes S and enters the state A+B before encountering any part of a detector. Upon encountering A1/B1 it becomes entangled in the state ##A\otimes A1 + B\otimes B1## (abusing notation here so that A1 here represents P interacting with the 1st part of the detector in path A). At this point entanglement destroys the pure state of P itself (P itself is in a mixed state, disallowing interference), but the pure state of the larger system remains: interference is possible using the bigger system of P, A1 and B1.
After the next interaction with A2/B2 the state becomes ##A \otimes A1 \otimes A2 + B \otimes B1 \otimes B2 ##. Now P with the first portion of the detectors decohered, but by including the 2nd part of the detectors we could still produce interference between the two alternatives A/B.
Above repeats to A3/B3, A4/B4, ... until we "see a flash" from detector A or B (via AN or BN).
Interpretations / Questions
Decoherence
Some people reportedly believe decoherence solves the measurement problem. In the context of this experiment, do some believe that decoherence of P after interacting with the first portion of the measuring device constitutes collapse? If so, how do they explain the interference that can occur in the larger system P,A1,B1? If not, how do they mark a particular step where collapse occurred?
Pilot-wave theory
If, at any time in this experiment, interference between the two paths can be created, then when & how do you reveal which path P actually went down? When does the pilot wave "disappear" from the path that doesn't contain P?
Any other interesting interpretations or points about this experiment?