Ok, here's a brief overview and derivation:
Suppose I have an experiment involving two entangled photons which are set up to share the same unmeasured axis of electric field polarization (that is to say that whenever one photon is found to be polarized at a certain angle, the other photon is polarized along the same axis at the same or opposite angle, and likewise when the first photon is found to be polarized orthogonal to the angle of measurement). In the experiment, I will measure each of the entangled photons' polarizations at opposite ends of the lab, with random selectors at each end of the lab independently choosing the axis of polarization for the measurements at those ends. The choices of measurement axes at each end of the lab will occur near enough to the times of measurement such that these choices cannot be communicated between the photons with lightspeed signals until after they've been measured.
For this experiment, suppose I have a possibility of choosing between three different axes of measurement to check if the photons have electric field polarizations along those axes. Let's call them axes A, B and C, with (for simplicity) B and C being displaced from A by $$120^\circ$$ and $$240^\circ$$, respectively. According to any local hidden variable theory, we can measure a photon's polarization about one axis and then determine what we would have measured along another axis by measuring its entangled pair along the second axis, since the same polarization values are always yielded by both photons when measured along the same axis. Thus, for each axis we can define a hidden variable which tells us whether the photons have any polarization when measured along that axis, and these variables in turn depend on some set of deterministic variables belonging to the local hidden variable theory. If we separate the two ends of the lab sufficiently far apart, no lightspeed or slower signal can be exchanged between the two photons in order for the choice of a measurement axis (and subsequent measurement) at one end to affect the hidden variables possessed by the photon which is measured at the other end.
Each time a photon pair is generated, there are eight different hidden variable possibilities which will be denoted in the following form: {+A,+B,-C} denotes, as an example, the case where measurements along either axes A or B will yield photons with polarization along those axes, but measurements along axis C will yield none. Then we have eight possible scenarios for the hidden variables determining the polarization of each photon pair:
1. {+A,+B,+C}
2. {+A,+B,-C}
3. {+A,-B,+C}
4. {+A,-B,-C}
5. {-A,+B,+C}
6. {-A,+B,-C}
7. {-A,-B,+C}
8. {-A,-B,-C}
Are we all agreed so far?
Suppose I have an experiment involving two entangled photons which are set up to share the same unmeasured axis of electric field polarization (that is to say that whenever one photon is found to be polarized at a certain angle, the other photon is polarized along the same axis at the same or opposite angle, and likewise when the first photon is found to be polarized orthogonal to the angle of measurement). In the experiment, I will measure each of the entangled photons' polarizations at opposite ends of the lab, with random selectors at each end of the lab independently choosing the axis of polarization for the measurements at those ends. The choices of measurement axes at each end of the lab will occur near enough to the times of measurement such that these choices cannot be communicated between the photons with lightspeed signals until after they've been measured.
For this experiment, suppose I have a possibility of choosing between three different axes of measurement to check if the photons have electric field polarizations along those axes. Let's call them axes A, B and C, with (for simplicity) B and C being displaced from A by $$120^\circ$$ and $$240^\circ$$, respectively. According to any local hidden variable theory, we can measure a photon's polarization about one axis and then determine what we would have measured along another axis by measuring its entangled pair along the second axis, since the same polarization values are always yielded by both photons when measured along the same axis. Thus, for each axis we can define a hidden variable which tells us whether the photons have any polarization when measured along that axis, and these variables in turn depend on some set of deterministic variables belonging to the local hidden variable theory. If we separate the two ends of the lab sufficiently far apart, no lightspeed or slower signal can be exchanged between the two photons in order for the choice of a measurement axis (and subsequent measurement) at one end to affect the hidden variables possessed by the photon which is measured at the other end.
Each time a photon pair is generated, there are eight different hidden variable possibilities which will be denoted in the following form: {+A,+B,-C} denotes, as an example, the case where measurements along either axes A or B will yield photons with polarization along those axes, but measurements along axis C will yield none. Then we have eight possible scenarios for the hidden variables determining the polarization of each photon pair:
1. {+A,+B,+C}
2. {+A,+B,-C}
3. {+A,-B,+C}
4. {+A,-B,-C}
5. {-A,+B,+C}
6. {-A,+B,-C}
7. {-A,-B,+C}
8. {-A,-B,-C}
Are we all agreed so far?
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