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Early 1980s
≈ 50
Two detectors more
than 13 m apart,
detector can be
switched after
particle has left
source
Complete randomness is observed if
there is only one detector, half of the
time the + bulb flashes, half of the time
the – bulb flashes
If there are two identical detectors, each
of them taken separately observed
complete randomness as well, i.e. same
number of + and - flashes
When one makes a correlation
between the result sequences from
both detectors, one observes that
when there is a plus on one side there is
always a minus on the other side,
perfect anti-correlation
Change the + and – signs on one
detector and you will observe perfect
correlations, in the correlation
setting/sign convention, replace the
bulbs at + with a green bulb, then you
will observe correlated green or red
flash pairs, the + and – signs can then
be removed
Putting the detectors very far apart makes sure
there is no connection between the two of them
Observing perfect correlations of two
distant detectors that have no connection
between them can be explained simply
by the assumption that the particle carries
an instruction set that is identical to each
of the identical appearing detectors,
(or if anti-correlation is observed, the
natural conclusion is that the instruction
set must simply be opposite, it is still one
set of instructions, a two value thing,
only)
Now we need to have a more
complicated detector with three different
settings, 1, 2, 3, so there are the nine (32)
different cases
11, 22, 33, when we will observe perfect
correlation,
12, 21, 13, 31, 23, 32 when we will
observed correlation one quarter of the
time
e.g. all ravens that
have been
observed so far
were black, that’s
why we can
concluded that all
ravens are black
More facts
Each of the four lights flashes just about half of the time green and half of the time
red given a long enough run to be statistically sound. The difference between the
number of red or green flashes diminishes as the number of test runs increases.
It is not possible to transmit any kind of information from one detector to the other,
even if one tried, the separated observer on the other end will always observe
about as many red flashes at green flashes
it is only after the experiment has been made and the
observations are compared that the remarkable
correlations are revealed !!!
by relativity, the question which detector detected his particle first is meaningless
as simultaneity in 4 dimensional space time means an event is only simultaneous if
it is observed at the same 3D space and 3+1D time. Hence there will always be an
observer standing closer to detector A who observes A going off before detector B
which is much further away from him. He cannot argue about this with an observer
that stands much closer to detector B, who just observes the opposite. By special
relativity, both are correct.
and six mixed
instruction
sets for the
other six
mixed switch
settings:
RRG, RGR,
GRR, GGR,
GRG, and
RGG for the
Just eight (23)
instruction sets
would do,
RRR, GGG, i.e.
two where there is
the same color for
the three identical
switch settings 11,
22, and 33, ..
Note that the particles must carry three
instruction sets, e.g. RRG, i.e. possess three
kinds of properties, e.g. two different colors,
small or big sizes, tetrahedral or cubic shapes
Only two of these properties get ever measured,
i.e. must really exist, while the third is never
measured, may as well not exist!!! Actually it is
one of the hidden variables that EPR required,
but the experiment shows that the prediction on
the assumption that there are three properties,
including a hidden variable that is never
measured, are not borne out in experiments !!!
Quantum mechanics has no problem to predict
the experimental outcome, one just has to
accept that [Sx,Sz] ╪ [Sz,Sx], i.e. do not
commute just like momentum and position, in a
sense, spin does not exist before it is measured
http://phet.colorado.edu/sims/ster
n-gerlach/stern-gerlach_en.html
Rather than having the axes perpendicular to each
other, we have then parallel for settings 11, 22, and 33,
and misaligned with respect to each other by 120º for
settings 12, 21, 13, 31, 23, and 32
"There are more
things in heaven and
earth, Horatio,
than are dreamt of in
your philosophy."
William Shakespeare

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lecture is the moon there.pdf

  • 1.
  • 2.
  • 3.
  • 5. Two detectors more than 13 m apart, detector can be switched after particle has left source
  • 6. Complete randomness is observed if there is only one detector, half of the time the + bulb flashes, half of the time the – bulb flashes If there are two identical detectors, each of them taken separately observed complete randomness as well, i.e. same number of + and - flashes When one makes a correlation between the result sequences from both detectors, one observes that when there is a plus on one side there is always a minus on the other side, perfect anti-correlation Change the + and – signs on one detector and you will observe perfect correlations, in the correlation setting/sign convention, replace the bulbs at + with a green bulb, then you will observe correlated green or red flash pairs, the + and – signs can then be removed Putting the detectors very far apart makes sure there is no connection between the two of them
  • 7. Observing perfect correlations of two distant detectors that have no connection between them can be explained simply by the assumption that the particle carries an instruction set that is identical to each of the identical appearing detectors, (or if anti-correlation is observed, the natural conclusion is that the instruction set must simply be opposite, it is still one set of instructions, a two value thing, only) Now we need to have a more complicated detector with three different settings, 1, 2, 3, so there are the nine (32) different cases 11, 22, 33, when we will observe perfect correlation, 12, 21, 13, 31, 23, 32 when we will observed correlation one quarter of the time e.g. all ravens that have been observed so far were black, that’s why we can concluded that all ravens are black
  • 8.
  • 9.
  • 10. More facts Each of the four lights flashes just about half of the time green and half of the time red given a long enough run to be statistically sound. The difference between the number of red or green flashes diminishes as the number of test runs increases. It is not possible to transmit any kind of information from one detector to the other, even if one tried, the separated observer on the other end will always observe about as many red flashes at green flashes it is only after the experiment has been made and the observations are compared that the remarkable correlations are revealed !!! by relativity, the question which detector detected his particle first is meaningless as simultaneity in 4 dimensional space time means an event is only simultaneous if it is observed at the same 3D space and 3+1D time. Hence there will always be an observer standing closer to detector A who observes A going off before detector B which is much further away from him. He cannot argue about this with an observer that stands much closer to detector B, who just observes the opposite. By special relativity, both are correct.
  • 11. and six mixed instruction sets for the other six mixed switch settings: RRG, RGR, GRR, GGR, GRG, and RGG for the Just eight (23) instruction sets would do, RRR, GGG, i.e. two where there is the same color for the three identical switch settings 11, 22, and 33, ..
  • 12. Note that the particles must carry three instruction sets, e.g. RRG, i.e. possess three kinds of properties, e.g. two different colors, small or big sizes, tetrahedral or cubic shapes Only two of these properties get ever measured, i.e. must really exist, while the third is never measured, may as well not exist!!! Actually it is one of the hidden variables that EPR required, but the experiment shows that the prediction on the assumption that there are three properties, including a hidden variable that is never measured, are not borne out in experiments !!! Quantum mechanics has no problem to predict the experimental outcome, one just has to accept that [Sx,Sz] ╪ [Sz,Sx], i.e. do not commute just like momentum and position, in a sense, spin does not exist before it is measured
  • 13.
  • 14. http://phet.colorado.edu/sims/ster n-gerlach/stern-gerlach_en.html Rather than having the axes perpendicular to each other, we have then parallel for settings 11, 22, and 33, and misaligned with respect to each other by 120º for settings 12, 21, 13, 31, 23, and 32
  • 15. "There are more things in heaven and earth, Horatio, than are dreamt of in your philosophy." William Shakespeare