|
|
| From: jerry |
2/03/99
11:40:09
|
| Subject: Quantum
entaglement |
post id:
2555
|
(Part 1)
Dear Jerry
(please call me Karl),
Hi, and thanks for your excellent and well
thought-out answer/comment! I have been trying to understand this stuff
for years! Quite frankly, I still don't understand it, so I'm not yet
qualified to answer it.
Would it be possible for you to post your
answer in the appropriate section, of the appropriate week, of the
Signal to Noise Section, of our homepage, so that everybody else
(67,000 pages down-loaded per week) can enjoy your answer as
well?
Cheers, karlkkkkk
>Dear Dr Karl, >I
am trying to get my head around this quantum stuff - and my
question >therefore is simple, "Do you agree with my arguments
below?" > >Many thanks. >Jerry. > >Quantum
superposition and entanglement. > Feb 26 1999 > >In
quantum mechanics we may consider an electron with the property
spin. >Whichever "direction" you measure the spin, you will always
find either spin >`up' or spin `down'. > >However, if
the spin of the electron has not been measured, then the >electron
is in a superposition of these two distinct states. > >It's a
little similar to a penny, spinning on the table-top. If you
slap >your hand on it, then it will either show heads or tails after
the >measurement, never something in between or "both". However,
before the >measurement, all that we can calculate about the
head/tail state of the >penny is that it will be either heads OR
tails after measurement, with >corresponding probabilities of each
state summing to 100%. With electrons >and photons the situation is
somewhat dissimilar in that a measurement does >not physically
prevent the particle from "spinning" since the term "spin" >when
applied to quantum particles does not actually mean "spin" in the
sense >that a penny spins on the table but the analogy does add some
degree of >understanding. (It is also not possible to catch and
measure a given >particle every time - so we are back into
statistics again for determining >the likelyhood that the two
particles are actually 100% entangled as it were >- a fine point in
the context of this argument.) > >We represent this
mathematically as two equal length (1/2) (50:50 chance of >heads or
tails) perpendicular vectors in an abstract space (a
so-called >Hilbert space). A superposition is defined as the vector
sum of these two >vectors. The vector we associate with a
superposition therefore lies in the >plane spanned by the vectors
`up' and `down' or 'heads' and 'tails'. >Different angles phi (the
angle of the superpotition vector) correspond to >different
superpositions and different probabilities (represented and a s
a >result of the relative lengths of the vectors) so that one rather
than the >other will prevail after measurement. It is easily
conceived that a system >may consist of a superposition vector that
traverses Hilbert space >dynamically with respect to some
independent variable such as time. In the >case of the penny, while
it is spinning fast, it's vector will have phi at >about pi/4
radians implying a 50:50 chance of falling heads or tails
after >measurement. If we imagine what happens to the vector if we
let the penny >spin to a halt without hitting it, then the vector
may be imagined to waver >about pi/4 and then rapidly fall to zero
or pi/2 when the penny finally >starts to spin with one particular
face up. The "heads" vector and "tails" >vector either shrinks to
zero or expands to one. If a penny was biased heads >or tails, then
the two vectors from which the superposition vector is >created
would be nominally unequal - but still sum to one. > >In the
case of electrons and photons, there is a system involving a pair
of >particles that are produced in the same source that are
entangled. This >means that, independent of subsequent separation in
distance, you may >determine the spin of one such particle and then
predict to 100% certainty >that the other particle has opposite
spin. At the risk of the effects of a >very bad pun... the
experiment performed in mid 1977 which actually observed >quantum
entanglement has spun-out many people. There has been talk
of >instantaneous information transfer, teleportation and
paradoxical meanings >with respect to special relativity and quantum
mechanics. As it turns out, >FLT signaling is NOT possible using
this system simply because the >measurement result of one particle
must subsequently be transmitted to the >owner of the other
particle, and this is subject to the rules of special >relativity. I
have read texts that use words like "spooky action at a >distance"
(borrowed from Einstein) and "Somehow the other photon "feels"
the >result of the measurement of the measured one." I've even read
text that >blames the confusion on limitations in our language! All
seem silly >explanations and I would like to pose the following
analogy using pennies as >a slightly better popular account of
quantum entanglement. > ...
continue
|
| From: jerry |
2/03/99
11:44:43
|
| Subject: re: Quantum
entaglement |
post id:
2557
|
(part
2)
>Mathematically, measurement of one of an entangled pair is
said to "collapse >the wave function" - a statement that does not
help the layman understand. >But the layman has a possibility of
understanding the superposition vector >explained earlier. What we
are representing by this superposition vector in >the case of the
spinning penny, is the probability of heads vs. tails before >the
penny has stopped spinning. In this macro-scale case the state
is >determinable either because of a measurement or because of
natural loss of >momentum. The "wave function" spoken of just now is
a "probability curve - a >distribution of probabilities spread over
an infinite range." and so >"collapsing the wavefunction" is
equivalent to drawing the mathematics from >the sphere of statistics
into the world of fact. Once a measurement has been >made, the
statistical distribution is no longer of any use because the
state >of the system becomes determinable. What we tend to do is
confuse the >mathematical concept of probability distribution with
actual physical fact. >Statistical representations of systems do not
target one particular state - >only the likelihood of finding a
given state. Let me now explain a two-penny >entanglement
system. > >Imagine this: I take a seemingly normal penny and
peel it apart so that I >now have two disks and I set them spinning
on different trays. Two people >who were NOT ALLOWED [thinks: "the
plank constant"] to witness the >creation of the entangled pennies
then walk away from each other each >carrying a tray until they are
far apart. One person looks at their penny >once it has stopped (or
stops it) and declares the state of the other penny. >The other
person takes a look at the stopped penny and finds that the
other >person's prediction is correct. > >How is this
possible? Simple. The original penny that was peeled apart
is >actually two pennies. Still don't get it? What if I said that
the original >penny was made of one double-headed penny and one
double-tailed penny? Now >it all makes sense. The outcome of the
experiment is actually determined at >the source - long before the
measurements were taken. They are guaranteed to >be complementary
since that is how we defined the system. Similarly, an >entangled
pair of photons can only coexist (entangled) upon creation in
the >source by having complementary characteristics and because of
the exclusion >rules of quantum mechanics - things like "two
electrons only may occupy the >same energy level". If they don't
have complementary characteristics - then >they are not entangled!.
In both cases - with the entangled pennies and with >entangled
photons, before actual measurement, we can only
mathematically >describe the state using the Hilbert space (or
similar tools). Once the >measurement is made the Hilbert space is
not required and facts can be >stated about the system regardless of
the subsequent separation of the >individual pennies or photons.
Before any measurement is made - even though >the outcome is
physically pre-determined, we have no idea what it is and >therefore
have to invoke the stochatic power of mathematical concepts
in >order to describe the system. It is the nature of these concepts
as >mathematical tools, not reality, which provoke the use of
language that >suggest that "Schrödinger's cat can be both dead and
alive". > >The important point to note about all teleportation
experiments and >entanglement experiments is that the entangled
particle must be created in >the same source. It would be impressive
indeed to be able to independently >create and entangled pair at
different spacetime coordinates but that has >never been
done. > >Could it be therefore that a "normal photon" for
instance is a bit like the >double-penny glued together
head-head-tail-tail so that it looks like a >familiar penny and the
production of an entangled pair is like peeling the >pennys apart?
In principle I can't see why
not.
[end]
|
| From: Terry Frankcombe |
2/03/99
14:14:27
|
| Subject: re: Quantum
entaglement |
post id:
2565
|
Hmm. While I don't pretend to
understand entanglement, I don't like the fact that you are using a
classical analogy to explain a very QM effect. Pennies are macroscopc and
therefore deterministic. Photons are microscopic and
probabilistic.
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| From: jerry |
2/03/99
14:56:22
|
| Subject: re: Quantum
entaglement |
post id:
2582
|
While I agree that trying to
explain a quantum idea using a macro analogy is questionable - What
alternatives are there? What I am trying to do is invent a hypothetical
macro system that we can all understand which, when modeled
mathematically, uses similar concepts as the quantum description. People
seem happy to explain the expanding universe in terms of rubber balloons
and flies, or raisin bread in the oven.
In my attempt, I use
spinning pennies, but point out clearly that the physical analogy is way
off the mark as far as quantum particles are concerned.
The main
point of the whole argument is to try and determine if the worldwide
confusion about quantum entanglement is due to an over emphasis on what
the stochatic mathematical model means as far as a physical system is
concerned at a point just before the wave function is collapsed. The
result is confusing or at best irrelevant. The physical implications of
trying to imagine a real system state that would be described by a system
actually IN superposition being bizarre but holding high media value. I
mean - people say daft things like, "The electron is everywhere at once."
No it's NOT! It's just that we are forced to work with probabilities of
where it is - and the mathematics says it can be anywhere (to a more or
lesser degree of certainty.)
In the example with the spinning
entangled pennies, it does not irk us too much to think of them as being
in both a "head" and a "tail" state until the point of measurement. And of
course, the act of measuring one will indeed predict the outcome of the
other and collapse the stochatic equations involved in the system as a
whole. But for us - since we set up the trick in the first place and are
privy to the initial conditions - we make no attempt to imagine the
pennies as talking to one another at the point of measurement! We also
have some kind of physical representation of a "head AND tail" state -
i.e. a spinning disk. In contrast, we have no decent visual representation
of a photon.
What I am looking for is someone who can say, "No -
your analogy is wrong - and this is why:…" Or someone who can enhance
the analogy in some way.
Cheers.
|
| From: Chris
(Avatar) |
2/03/99
15:03:09
|
| Subject: re: Quantum
entaglement |
post id:
2584
|
Well, I like the spinning
penny as an analogy for unresolved probabilities co-existing.
However I think you're overextending it in quantum entanglement
terms. I found from reading your account that the penny analogy didn't
really add anything to the issue of separation, and it is potentially very
confusing. For instance I thought you were going to get confused on the
spin issue - and whilst you extricated yourself by saying the penny spin
doesn't correlate with a particle's angular momentum, that section became
sloppy. (The fact that the penny spins is entirely irrelevant - what is
important is that we don't know whether it will be heads or tails till we
stop it, ie until we actively observe).
What you seem to be
basically asserting is that the twin photon system can be described by a
single wave function, which is a standard interpretation anyhow. And I
don't see how your split pennies help with that - in fact I'd have to say
it would probably do more to confuse people.
I find that a similar
problem occurs in GR, SR, etc where people take simplistic analogies (eg
the inflating balloon model of the expanding universe) and then over-use
them. The model is intended to help understanding about the physical
reality, not to substitute for it. In that sense, as I say, I thought the
spinning penny is a good analogy for unresolved probability or
superposition of states, but not for entanglement.
Hope this
helps! Chris
|
| From: Stephen Bosi |
2/03/99
15:11:16
|
| Subject: re: Quantum
entaglement |
post id:
2585
|
I'll tell you exactly why your
analogy is wrong. Because you said that the result was determined at the
moment the pennies were peeled apart. This is completely contrary to the
spirit of quantum mechanics as we presently understand it. Einstein wanted
to believe that in these kind of experiments, the result was predetermined
BEFORE observing the spin on one of the electrons (or the polarisation on
one of the photons), whereas the more conventional quantum explanation is
that the result is determined at the moment of measurement. The two
pictures are NOT equivalent and yield different experimental results. The
experiements have been done and the non-Einsteinian picture makes the
correct prediction.
|
| From: Chris
(Avatar) |
2/03/99
15:25:49
|
| Subject: re: Quantum
entaglement |
post id:
2588
|
The main
point of the whole argument is to try and determine if the worldwide
confusion about quantum entanglement is due to an over emphasis on what
the stochatic mathematical model means as far as a physical system is
concerned at a point just before the wave function is collapsed. The
result is confusing or at best irrelevant. The physical implications of
trying to imagine a real system state that would be described by a system
actually IN superposition being bizarre but holding high media value. I
mean - people say daft things like, "The electron is everywhere at once."
No it's NOT! It's just that we are forced to work with probabilities of
where it is - and the mathematics says it can be anywhere (to a more or
lesser degree of certainty.)
This argument has been
going on since the earliest Solvay Congresses in the '20s, and spawned
what we call the Copenhagen Interpretation of QM. You're arguing
the point of view of Einstein, et al, who insisted that the quantum theory
can not be a statistical mathematical theory without an underlying
description of the "physical reality" whatever that may be.
Bohr
and his supporters (and students) countered that since the underlying
reality is observation dependent it becomes less meaningful to try to
describe the physical situation prior to observation, as in "yes, but
what's actually going on before we look at Schroedinger's
cat?"
Terry is exactly right in his assertion that you can't really
attempt to model a QM system classically. It may help with visual cues,
etc, but to base your math on such a model is a mistake, after all QED is
the most mathematically accurate theory ever devised! Keep in mind, also,
that other visualisations such as schroedinger's cat, etc, were coined in
an attempt to point out how ridiculous the quantum theory is at a
macroscopic level!
What I am looking for is
someone who can say, "No - your analogy is wrong - and this is why:…"
Ok, your analogy is fine enough for a single spinning
penny representing an unobserved superposition of two possible
eigenstates.
Your analogy is confusing when you separate the
penny into two and remove them. I understand that you are trying to show
that the head and tail are interrelated before splitting, and remain that
way. However because you introduced the idea of collapsing the
wavefunction=stopping the penny spinning, you're in trouble. Stopping one
penny spinning will not stop the other. The lay person will get confused.
Since there is no physical connection between the two half pennies, how
does this improve on the situation with two separated photons? This is why
I think it helps with the single penny, but not with the
two.
Consider how your pennies will help explain the EPR paradox to
someone. The penny can only handle one variable with two possible
eigenstates. The heart of EPR is the second variable which is mutually
non-commuting with the first. I don't see how the pennies help
here.
Hope this
helps! Chris
|
| From: jerry |
2/03/99
16:05:47
|
| Subject: re: Quantum
entaglement |
post id:
2592
|
Said Chris: "I thought the
spinning penny is a good analogy for unresolved probability or
superposition of states, but not for entanglement"
Thank you for
your comments. I would like to reinforce the entanglement argument. ( We
have got out of phase. I'll digest your latest post in a while and reply
to it - but admit that my missive is confusing if it was interpreted as
meaning: [ "However because you introduced the idea of collapsing the
wavefunction=stopping the penny spinning, you're in trouble" ]. I never
intended to imply that as an equality. I'll have to re-read the original
post to see how that popped out! I've been flipping between QM and
classical terminology too much. Sorry.
If we can leave aside the
*spinning* pennies and concentrate on the initial conditions, the two
discs constructed from one doubled-headed and one double-tailed disc ,
H-H-T-T "look" at first glance like a single disc because of the way that
they are put together - back to back. What I am saying is, "this is an
entangled system in our hypothetical world." Then I say, that no observer
is allowed to be privy to the construction - in the same way that we are
barred from knowing what goes on at distances smaller than the plank
length. However, because we can peel these discs apart and THEN look at
them separately, we can infer that the system has certain rules. In our
hypothetical system the rules being perhaps, "No construction H-H-H-H is
allowed… only a maximum of two disks per object are allowed and they must
have complementary H and T"… and anything else that we might theorise and
test about the system.
"Entanglement - and the outcome of
subsequent measurements" therefore is a property of the initial
conditions. Maybe these discs can be created by a wacky energy change or
something - but only in the form H-H-T-T. If we work out how to "create"
two separate entities from the same source at the same instant, an H-H and
a T-T, such that they can subsequently be *separated* in space, this is
still an entangled system. Again, if we are not allowed to witness their
creation and construction at that point in time, we either have to look at
one of them or apply stochatic mathematics to determine probabilities
about the state of the system.
I would be surprised if no one has a
problem with the statement "Entanglement - and the outcome of subsequent
measurements" therefore is a property of the initial conditions." - only
for the fact that this is coming straight out of my analogy and I've never
read it anywhere with respect to QM.
It would sort of beg the
question, "Are all photons/electrons actually tightly coupled entangled
pairs that appear to be a single unit to an observer? Entangled pairs
still look normal but for the complementary characteristics." Could it be
that we are fooled into thinking that each of an entangled particle is bog
standard - just the same as a "normal" particle whereas the reality may be
that what we see as non-entangled particles are actually elaborate systems
of pairs that just look normal? Just like the head-head-tail-tail penny.
After all, if we are only allowed to look at a head-head penny once it has
been stopped, then we can't know what is on the other side, and may well
assume that it is a "normal" Head-tail penny. From this aspect - I see
comfortable analogies. Again, if we did many independent experiments with
"normal" pennies, we would find that 50% are heads, 50% are tails. We may
even come to the conclusion that each is constructed HT - even though they
are actually of HHTT construction. We may then further experiment with
peeled-apart pennies (the act of peeling we cannot see) and conclude that,
since the experiments never show with acceptable certainty that entangled
pairs both land heads or both tails, that they somehow communicated
instantaneously across any distance. We will never conclusively be able to
show that the actual construction of a separated entangled pair is HH ( or
TT )! And if that idea never occurs to us and we live on in the belief
that each separate entangled pair is HT - just like our idea of "normal"
discs, then the "spooky action at a distance" seems plausible as a
mathematical explanation but quite perplexing in reality. I can see why
Einstein balked.
|
| From: jerry |
2/03/99
16:15:17
|
| Subject: re: Quantum
entaglement |
post id:
2594
|
Thanks Stephen,
I'm not
trying to oust QM or take Einstein's side either - so I do appreciate your
comments. I'm just trying desparately to get my head around this
stuff.
Do you have any further details on the experiments of which
you speak?
[ The experiements have been done and the
non-Einsteinian picture makes the correct prediction.
]
| This
forum is un-moderated. The views and opinions expressed are those of the
individual poster and not the ABC. The ABC reserves the right to remove
offensive or inappropriate messages.
| From: Chris
(Avatar) |
3/03/99
9:13:47
|
| Subject: re: Quantum
entaglement |
post id:
2652
|
Stephen is probably referring
to the EPR paradox. In the late 60s John Bell wrote an inequality which
could help determine what happens when non-commuting variables in
entangled but separate particles are observed.
In the 80s Alain
Aspect devised a physical experiment to test the inequality. The results
came down in favour of Bohr - against Einstein (the two protagonists in
the original paradox).
The details of the inequality, and aspect's
experiments have been published, critiqued, etc. You will probably even
find them online - although physics review is the best place.
The
remaining controversy centres around the mathematical formulation of the
inequality and its correctness - or completeness - and some limitations
which may or may not have affected aspect's experiment. Dr Ed holds a
slightly different view to mine on the validity of aspect and bell, and
the arguments continue!! :o)
Hope this
helps! Chris
|
| From: jerry |
4/03/99
11:56:29
|
| Subject: re: Quantum
entaglement |
post id:
2751
|
Thanks Chris, I am aware of the
EPR "paradox". I've been reading up on Bell's theory and at least one
author actually states,
"The two photons are correlated when
measured because their potentialities-their indeterminate, wavelike
aspects-were never separate in the fist place." (pp65-67 "Who's afraid of
Schrodinger's Cat? Ian Marshall, Danah Zohar")
This is precisely
what I am saying with regard to the system of back to back
double-head,double-tailed pennies - nice to read that but I beg the
question, "Have I interpreted this correctly?".
Also,
according to the author of the web
page…
http://www.mtnmath.com/faq/meas-qm-faq-5.html
"…It
might seem that the tables have been turned on Einstein. The very argument
he used in EPR to show QM must be incomplete requires that hidden
variables models have explicit nonlocal operations. However it is
experiments and not theoretical arguments that now must decide the issue.
Although all experiments to date have produced results consistent with the
predictions of QM, there is general agreement that the existing
experiments are inconclusive3. There is no conclusive experimental
confirmation of the nonlocal predictions of QM. If these experiments
eventually confirm locality and not QM Einstein will be largely vindicated
for exactly the reasons he gave in EPR. Final vindication will depend on
the development of a more complete theory…"
3 P. G. Kwiat, P. H.
Eberhard, A. M. Steinberg, and R. Y. Chiao, Proposal for a loophole-free
Bell inequality experiment, Physical Reviews A, 49, 3209
(1994).
------------------
This bit that I have picked up on
is "There is no conclusive experimental confirmation of the nonlocal
predictions of QM"
Can anyone add any degree of credulity to this?
Does anyone know the current status of the certainties of these QM
experiments involving nonlocality?
|
| From: jerry |
5/03/99
14:33:51
|
| Subject: re: Quantum
entaglement |
post id:
2932
|
Hi,
A quote from
http://cosmopolis.com/topics/quantum-nonlocality.html
"...The
Phenomenon of Quantum Nonlocality Because the spin of a particle does
not exist until a measurement is made, the act of making the measurement
and determining the axis of spin of particle 1, will also determine the
spin of particle 2, no matter how far apart it is from particle 1.
Particle 2 will instantly respond to the state of particle 1, even if it
is on the other side of the universe..."
Is this really really
true ? Experimentally proven? I mean the bit about the "other" particle
"responding" - I don't mean 'just that we instantly "know" it's
state', I mean, is there an experiment that shows, say some interference
effect that vanishes or wobbles or something before the eyes of the
experimenters on the "other" particle at the instant that particle one's
spin is measured? Even if the other spin is not known by those far away
experimenters because they have to await the result of the spin
measurement from the first using normal signaling.
I think not
'cause then you could transmit a code by setting up an array of entangled
pairs, take them far apart and then "send" ones and zeros by measuring or
not measuring in the array. "Does watching ANY property of the other
particle or relationship between the two cause a collapse of the wave
function"?
Therefore, - back to my original analogy and conclusions
- that the spin states are predetermined. It's just the mathematics that
"pops" into actuality from probability.
Still struggling with this
one!
:0)
|
| From: Chris
(Avatar) |
7/03/99
16:11:12
|
| Subject: re: Quantum
entaglement |
post id:
3023
|
Jerry
Your struggle is
going to continue for quite some time because it is a struggle with
conceptualisation, which QM tends to resist.
I refer you again to
Bohr's interpretation. He pretty much comes straight out and says that QM
doesn't deal with "what happens before a measurement is made". The
theory is observation dependant, to the extent that traditional "reality"
is only defined on the basis of measurement.
In this sense, I
could describe the situation with entangled photons simply with a single
SWE (schroedinger wave equation). This is a powerful conceptual tool for
those who have looked at the mechanics of the quantum theory. Let us not
forget that QED, the crown jewel in the quantum theory, is the most
accurate mathematical theory ever devised.
Consider (for example)
the decay of a neutral kaon, at rest in the laboratory frame, into two
back to back photons which are then separated and individually examined.
Now ask yourself whether it is possible to describe the two photon system
by a single SWE (examine complimentary variables) and then ask what this
tells you about the system.
Now compare to a penny spinning which
is split into two. Which tells you more?
On your question about
Bell's theory and Aspect's experiments, yes both the inequality and the
experimental design and execution have been questioned. The experiment
ruled out hidden variables, and may still do so. However there is still
debate on the topic. I might add that if the aspect/bell result is shown
to be wrong, and there are hidden variables which account for non-locality
then I think your pennies are in even bigger trouble! :o)
Hope
this helps! Chris
|
This forum is un-moderated. The views and opinions
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the right to remove offensive or inappropriate messages.
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