G
glen herrmannsfeldt
(snip, I wrote)
Thinking about it again, the coupling between the two, classically,
is the probability of the particle emitted from one hitting the other.
That makes the argement for it being squared more obvious.
Yes. About the only point I was trying to make is that in quantum
mechanics things are rarely infinite and rarely zero, but instead
really huge and really tiny.
(snip)
OK, but it is a slightly different problem. To make EPR tests work,
you have to be careful that you don't disturb the quantum state.
For quantum randomness, you want the systems to be uncoupled, but
will find that there is (a very small amount) of coupling.
More specifically, and the experiment that took longer to do than
some other ones, two particles can be created coupled, separated
in distance, and then have their state measured. Even when the
time between the two measurements is less than the distance
bewteen them divided by c, (so that no signal could propagate)
they are still found to keep their state.
Yes. The point that I was trying to make, with a very simplified
example, is that quantum systems, like PRNGs, have a finite number
of states. It might be a really huge number, though.
And then you have to extract some of that state information and
generate bits from it.
-- glen
(snip)
Thinking about it again, the coupling between the two, classically,
is the probability of the particle emitted from one hitting the other.
That makes the argement for it being squared more obvious.
You can predict something based upon that overlap, but what you can
predict is only a shift in the probability distribution. The actual
decay time is still a perfectly random selection from that distribution.
You cannot predict the actual time until the next decay. No matter how
much information you have, the time until the next decay could be either
arbitrarily long or arbitrarily short, without violating any of the laws
of quantum physics as they are currently understood. That is the
fundamental distinction between quantum randomness and
pseudo-randomness. If you knew the full internal state of a
pseudo-random number generator, and the algorithm it uses, you could
determine the next random number precisely.
Yes. About the only point I was trying to make is that in quantum
mechanics things are rarely infinite and rarely zero, but instead
really huge and really tiny.
(snip)
It's not just a matter of some of the universe's state information being
hidden from us. Einstein, Podalsky and Rosen (EPR) tried to interpret
quantum uncertainty as being due to "hidden variables" - state
information about the universe that we were unaware of (and which we
might inherently be incapable of being aware of). They deliberately left
the details of what that state information was and how it influences the
measurements completely unspecified. Despite leaving it unspecified,
they were able to describe a quantum-mechanical experiment, and a
statistic that could be calculated from measurements that could be taken
while running that experiment. They rigorously derived a requirement
that this statistic must be greater than or equal to 1, regardless of
how the hidden variables actually worked. Quantum mechanics, on the
other hand, predicted that the value of that statistic should be 0.5.
From this, EPR concluded that quantum mechanics was unrealistic, and
could therefore be, at best, only an approximation to reality.
OK, but it is a slightly different problem. To make EPR tests work,
you have to be careful that you don't disturb the quantum state.
For quantum randomness, you want the systems to be uncoupled, but
will find that there is (a very small amount) of coupling.
At the time their paper was published, it was not possible to conduct
the experiment with sufficient precision to clearly distinguish a value
of 1 from a value of 0.5. Many years later, when scientist were finally
able to perform it, reality decided not to cooperate with EPR's concept
of "realism". The measured value unambiguously confirmed the quantum
mechanical prediction, violating the constraint that EPR had derived
from assuming that hidden variables were involved.
Scientists still believe that quantum mechanics can only be an
approximation to reality - but it's no longer because of the
fundamental role that true randomness plays in the theory.
More specifically, and the experiment that took longer to do than
some other ones, two particles can be created coupled, separated
in distance, and then have their state measured. Even when the
time between the two measurements is less than the distance
bewteen them divided by c, (so that no signal could propagate)
they are still found to keep their state.
I don't want to start an extended discussion of EPR - even experts get
into long pointless arguments talking about it. I just want to say that,
when I talk about "really random", I'm talking about the kind of thing
that EPR were implicitly assuming was inherently impossible when they
derived their limit equation.
Yes. The point that I was trying to make, with a very simplified
example, is that quantum systems, like PRNGs, have a finite number
of states. It might be a really huge number, though.
And then you have to extract some of that state information and
generate bits from it.
-- glen