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Author Topic:   Quantum Entanglement - what is it?
RAZD
Member (Idle past 1431 days)
Posts: 20714
From: the other end of the sidewalk
Joined: 03-14-2004


Message 31 of 117 (313009)
05-17-2006 11:12 PM
Reply to: Message 29 by cavediver
05-17-2006 9:13 PM


Re: More On Bell's Theorem... problems.
What are you measuring with one set of sensors (one for each particle in a pair)?
For any coupled pair you get the same results, but you also get 50% red and 50% green, agreed?
What are you measuring with a second set of sensors set up to give you two different results for the same particle:
For any coupled pair you get different results, and you also get 50% red and 50% green.
Now, {deep breath}, what are you really testing with the apparatus?
If I look at it such that 2 and 3 are interchangeable with respect to 1, 1 and 3 are interchangeable with respect to 2 and 1 and 2 are interchangeable with respect to 3 -- that only same switch settings result in same results, and 1-2 or 1-3 result in different results (and logically how can they not?)
Then I get a grid like this:
Detector A's Position
| 1 | 2 | 3 |
---------------
1 | S | D | D |
2 | D | S | D | Detector B's Position
3 | D | D | S |
---------------
... with a 3/6 instead of a 5/4 distribution? THAT MAKES IT WORSE!!!
What changed? The arbitrary assignment of results as "D" category.
And why is 12 or 21 always different?
When 13, 31 are always "same" while 2-3 and 3-2 are always "different" ...
Ask yourself that about the photons and the polarized plates.
The problem is that we know that sometimes the results will be the same with the different switch settings, so how do you model that? We know that the 5/4 grid is arbitrary (in it's assignment of "S" to 1-3 and 3-1), and we know that the 3/6 grid is false.
The orientations wrt x y and z are all independent.
True, but what are you measuring? You are measuring magnetic field with regard to (re yr wrt abbrv btw) x y and z planes. You have no idea how strong the field is or how tilted it is wrt the measurment plane, so all you can tell is north = positive axis side of the plane or north = negative axis side of the plane. Each sensor will measure + or - for (virtually) every particle (we can argue about the relative infinity of ones |exactly| perpendicular to the plane - no field measured - vs the vast infinity of all the other orientations later).
Coupled pairs measured by the same axis sensors will always have the same results - agrees with both "coupled" and "entangled" concepts.
Coupled pairs measured by different axis sensors will sometimes be the same and sometimes be different. The assignment of "S" and "D" in the grid is bogus. It is not based on what is measured.
If we look at probabilities of "S" and probabilities of "D" for 3 sets of detectors with positive orientations at 120o intervals so that we have 0o to 60o centered on {1+}, 60o to 120o centered on {2-}, 120o to 180o centered on {3+}, 180o to 240o centered on {1-}, 240o to 300o centered on {2+} and 300o to 360o centered on {3-}, then for any particle that reads {1+} also reads {2-} and {3-} ... you get a SDD distribution (one pair of sensors - 2&3 -agrees the other two pairs of sensors - 1&2 and 1&3 - disagree).
Plugging this into the grid you get:
Detector A's Position
| 1 | 2 | 3 |
---------------------
1 | SSS | SDD | DSD |
2 | DDS | SSS | DDS | Detector B's Position
3 | DSD | SDD | SSS |
---------------------
Using multiples to represent rough probabilities in each box. Add up all the "S"s and all the "D"s and you get 15/13. Whether it is GB's or polarized photons. Closer eh?
{abe}Is this what is being measured?
No, not really. Only two sensors are used at a time. You either have same setting or different setting, that's why earlier I had:
Detector A's Position
| 1 | 2 |
-----------
1 | S | D | Detector B's Position
2 | D | S |
---------
plus
Detector A's Position
| 1 | 3 |
-----------
1 | S | D | Detector B's Position
3 | D | S |
---------
plus
Detector A's Position
| 3 | 2 |
-----------
3 | S | D | Detector B's Position
2 | D | S |
---------
{/abe}
But it will have to wait as it's 2am and I'm wacked.
I get up at 5am here, it's all relative eh?
Enjoy
zzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzz
Edited by RAZD, : correction, added material

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This message is a reply to:
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JustinC
Member (Idle past 4869 days)
Posts: 624
From: Pittsburgh, PA, USA
Joined: 07-21-2003


Message 32 of 117 (313021)
05-17-2006 11:51 PM
Reply to: Message 28 by RAZD
05-17-2006 8:35 PM


Re: More On Bell's Theorem... problems.
RAZD writes
quote:
Detector A's Position
| 1 | 2 |
---------
1 | S | D | Detector B's Position
2 | D | S |
---------
plus
Detector A's Position
| 1 | 3 |
---------
1 | S | D | Detector B's Position
3 | D | S |
---------
plus
Detector A's Position
| 3 | 2 |
---------
3 | S | D | Detector B's Position
2 | D | S |
---------
Obviously resulting in a 50:50 distribution
This is all very confusing because you don't specify what coding you are using. How can you make a judgement about sameness or differentness if you don't know the coding.
The possible codings are:
RRR GGG RRG GGR RGG GRR GRG RGR
Pick anyone and put them into you're three grids. You don't get a 50/50 split with anyone of them.
For example, use RRG. You get
Detector A's Position
| 1 | 2 |
---------
1 | RR | RR | Detector B's Position
2 | RR | RR |
---------
plus
Detector A's Position
| 1 | 3 |
---------
1 | RR | GR| Detector B's Position
3 | RG | GG |
---------
plus
Detector A's Position
| 3 | 2 |
---------
3 | GG | RG | Detector B's Position
2 | GR | RR |
---------
What you get, is 8 that are the same, and 4 that are different. But when you factor in that you are double counting some combinations, what you get is 5/4.
You get 55.55% (5/4) the same with all combinations except RRR and GGG, where you get 100%.
So in order to get the 50% split, you obviously aren't using any of the codings above.
The question, then, is, "what coding are you using to get a 50/50 split and also to get the 11RR 11GG 22RR etc. correspondences?"
Edited by JustinC, : aesthetics

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RAZD
Member (Idle past 1431 days)
Posts: 20714
From: the other end of the sidewalk
Joined: 03-14-2004


Message 33 of 117 (313033)
05-18-2006 12:47 AM
Reply to: Message 32 by JustinC
05-17-2006 11:51 PM


Re: More On Bell's Theorem... problems.
But you are confusing 3 "states" with 3 "measurements"
you only have two measurements at a time, sensor {A} or sensor {B}.
The possible codings are:
RRR GGG RRG GGR RGG GRR GRG RGR
Now take one "possible coding" out of each set and match it up to the right 2x2 box and then add up all the possibilities.
RRX GGX RRX GGX RGX GRX GRX RGX (2x2 grid #1)
RXR GXG RXG GXR RXG GXR GXG RXR (2x2 grid #2)
XRR XGG XRG XGR XGG XRR XRG XGR (2x2 grid #3)
The X's are NOT measured.
Sum up the results, each line has 4 same and 4 different. Total 12/12.
But when you factor in that you are double counting some combinations, ...
Or double counting all data? (it would be triple, except for the X's) Check the columns for each letter position.
Thanks.

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fallacycop
Member (Idle past 5546 days)
Posts: 692
From: Fortaleza-CE Brazil
Joined: 02-18-2006


Message 34 of 117 (313034)
05-18-2006 12:47 AM
Reply to: Message 31 by RAZD
05-17-2006 11:12 PM


More On Bell's Theorem
Actually, RAZD the patern of probabilities you would have to explain is this:
Detector A's Position
| -1--1--1- | -2--2--2- | -3--3--3- |
----------------------------------------
1 | S : 100% | S : 25% | S : 25% |
1 | D : 0% | D : 75% | D : 75% |
----------------------------------------
2 | S : 25% | S : 100% | S : 25% | Detector B's Position
2 | D : 75% | D : 0% | D : 75% |
----------------------------------------
3 | S : 25% | S : 25% | S : 100% |
3 | D : 75% | D : 75% | D : 0% |
----------------------------------------
Where the percents after D : represent the probability of getting different light colors
and the percents after S : represent the probabilities of getting the same color
Observe that the average over the table is D : 50% and S : 50%
Same for any column or row.
But it shows an average of S : 100% and D : 0% in the diagonal.
No classical experiment can reproduce these features. Try it

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JustinC
Member (Idle past 4869 days)
Posts: 624
From: Pittsburgh, PA, USA
Joined: 07-21-2003


Message 35 of 117 (313045)
05-18-2006 1:43 AM
Reply to: Message 33 by RAZD
05-18-2006 12:47 AM


Re: More On Bell's Theorem... problems.
quote:
But you are confusing 3 "states" with 3 "measurements"
you only have two measurements at a time, sensor {A} or sensor {B}.
I don't think so. I am taking two measurements, signified by the the two character nature of RR, GG, RG, and GR.
quote:
Now take one "possible coding" out of each set and match it up to the right 2x2 box and then add up all the possibilities.
RRX GGX RRX GGX RGX GRX GRX RGX (2x2 grid #1)
RXR GXG RXG GXR RXG GXR GXG RXR (2x2 grid #2)
XRR XGG XRG XGR XGG XRR XRG XGR (2x2 grid #3)
This is where I lose you. The same coding is present in both "things" emitted (because of the 11RR, 11GG, 22RR, 22GG, etc. correlation), so you have to use two coding strings to see what is going on.
Only one measurement is taken from each coding, so to accurately reflect what is going on with Grid 1, you have to use two strings.
For the first box of Grid 1 (1/1), you'd get
1st detector: RXX GXX RXX GXX RXX GXX GXX RXX
2nd detector: RXX GXX RXX GXX RXX GXX GXX RXX
2nd box (2/1)
1st detector: XRX XGX XRX XGX XGX XRX XRX XGX
2nd detector RXX GXX RXX GXX RXX GXX GXX RXX
etc. You get the picture.
When you cross out only one letter when you write
RRX GGX RRX GGX RGX GRX GRX RGX (2x2 grid #1)
you are implying that somehow the two detectors are taking two measurments from one code. But the code is in both "things." They are two codes, and they have to be the same.
Look at the original diagram (I tried to reproduce it but it got botched up somehow). The squiggily emitter lines represent the same code going out, so replace them mentally with one of the 8 possibilities.
Do you disagree with this?
Edited by JustinC, : No reason given.
Edited by JustinC, : No reason given.

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Son Goku
Inactive Member


Message 36 of 117 (313087)
05-18-2006 3:41 AM
Reply to: Message 17 by RAZD
05-16-2006 8:59 PM


Re: A goldmine of responses ...
Thanks, I have looked it up, and was unconvinced. This is, in fact, where I started with this. It could also be that you are not measuring what you think you are measuring. Bell's Theorem arbitrarily assumes three conditions to get the pattern of nine possible combinations and the 5/4 inequality
I think you might have missed something. It assumes some axioms characteristic of any Classical Theory, not even Newton’s or Lagrange’s, but any conceivable classical theory that could be constructed.
It turns out any Classical Theory will obey the inequalities no matter what its character.
However any Quantum Theory won't.
When we run the experiment the inequalities don't hold, which is very solid evidence against a pre-assigned state, a lá Classical Mechanics.

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cavediver
Member (Idle past 3669 days)
Posts: 4129
From: UK
Joined: 06-16-2005


Message 37 of 117 (313105)
05-18-2006 5:58 AM
Reply to: Message 31 by RAZD
05-17-2006 11:12 PM


Re: More On Bell's Theorem... problems.
Ok, unfortunately this has to be brief... more later tonight... so much confusion, so little time
What are you measuring with one set of sensors (one for each particle in a pair)?
Firstly, let me again emphasise: I DON'T CARE! All that matters are the experimental data and some way of replicating it. FALLACYCOP has very kindly expressed the actual observed probabilities in the grid that have to be replicated. To delve into the mechanism is unnecessary and just adds to the confusion.
With both the gyros and the photons, you get a roughly even mix of same and different when the switches are in different positions:
e.g. 12RG 12GG 12GR 12GR 12RG 12RR 12RR 12GG etc
same with 13, 21, 23, and 31.
With enough runs, the photons will get you exactly 50% RR/GG and 50% RG/GR. At the same time they will get you exactly 100% RR/GG with 11, 22, or 33. You will not get this with your gyros.
As JustinC has pointed out, your move to three 2x2 grids is overcounting: you have the 11, 22, and 33 results listed twice. This is why your conclusion is wrong.
By moving to your earlier four axis version, or your 3 rotations of each axis in the post to which I am replying is just hopelessly complicating the situation. The challange is simple: replicate the results of the experiment I described - not some other experiment.
Edited by cavediver, : No reason given.

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RAZD
Member (Idle past 1431 days)
Posts: 20714
From: the other end of the sidewalk
Joined: 03-14-2004


Message 38 of 117 (313117)
05-18-2006 7:49 AM
Reply to: Message 35 by JustinC
05-18-2006 1:43 AM


Re: More On Bell's Theorem... problems.
JustinC, msg 35 writes:
I don't think so. I am taking two measurements, signified by the the two character nature of RR, GG, RG, and GR.

A
| G | R |
---------------
G | S | D |
B ---------------
R | D | S |
---------------
Precisely. It is a binary measurement of 3 switches. The next question is what gives you those results....

A A
| G | R | | G | R |
--------------- ---------------
G | 1-1 | 1-2 | G | 3-2 | 2-1 |
B --------------- B ---------------
R | 1-3 | 2-3 | R | 3-1 | 1-1 |
--------------- ---------------
A A
| G | R | | G | R |
--------------- ---------------
G | 2-2 | 2-3 | G | 3-1 | 3-2 |
B --------------- B ---------------
R | 2-1 | 1-3 | R | 1-2 | 2-2 |
--------------- ---------------
A A
| G | R | | G | R |
--------------- ---------------
G | 3-3 | 3-1 | G | 2-1 | 1-3 |
B --------------- B ---------------
R | 3-2 | 1-2 | R | 2-3 | 3-3 |
--------------- ---------------
... you are implying that somehow the two detectors are taking two measurments from one code. But the code is in both "things." They are two codes, and they have to be the same.
The problem is that you have both the code and the measurement to get the result.
Edited by RAZD, : Corrected one 3-1 to 3-2 per JustinC's good eye. (msg 48) thanks.

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Son Goku
Inactive Member


Message 39 of 117 (313132)
05-18-2006 8:51 AM


Entangelment and collapse.
Let us say that I have a particle called A and a particle called B.
If A is in a spin up state then we label it with:
|A up>
If A is in a spin down state then we label it:
|A down>
If A is in a superposition of spin up and down then:
|State of A> = |A up> + |A down>
The same goes for B.
If I write a state:
|State of A and B> = |A up>|B down>
That means A and B are part of the same system with A being up and B being down.
Now lets we get A and B and entangle them, to give the following state:
|State of A and B> = |A up>|B down> - |A down>|B up>
This means A and B are part of the same system and that system is in a superposition of the two system states "A is up, B is down" and the system state "A is down, B is up".
Now I send A and B off in opposite direction and somebody far away measures A to be spin up.
This means the system cannot be in the state "|A down>|B up>" as A was measured to be spin up, so the system collapses to:
|State of A and B> = |A up>|B down>
So B has to be down, because that is all that is left in the state.
When I measure B, this indeed turns out to be the case.
The whole paradox is that the system went from:
|State of A and B> = |A up>|B down> - |A down>|B up>
to
|State of A and B> = |A up>|B down>
instantly.
As soon as A was measured it pulled out the "|A down>|B up>" part across the whole universe.

Replies to this message:
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Modulous
Member
Posts: 7801
From: Manchester, UK
Joined: 05-01-2005


Message 40 of 117 (313137)
05-18-2006 9:02 AM
Reply to: Message 22 by cavediver
05-17-2006 5:09 AM


I'm terribly confused, but in a good way
Hi there,
I think I understand the situation here, but my head hurts trying to understand the consequences. So let me try and put down in words what I think is happening in the experiment and see where that leads me. I'll word the macroworld explanation in terms of communications rather than gyroscopes, since that makes more sense to me.
We have a box that fires a signal to two receivers. That signal can be any one of the 23 states of a three string binary code. For convenience we'll stick to Rs and Gs rather than throwing in 1s and 0s.
The two receivers have a randomly selected switch that is either one of three settings. There are thus 32 switch positions.
When a receiver gets the signal it uses the switch setting as a rule to determine what colour light to illuminate. Position one selects 'bit' 1 of the string. For example if the string is RXX and the switch position is 1, the red light goes on.
OK. This is where my mind melts...
For any mixed string of Rs and Gs the we would expect to see 55.5% of the lights being the same. And if we include RRR and GGG (where for obvious reasons the lights are always the same), we conclude that we should see the same lights shine more than 55.5% of the time.
But we don't?
*melting brain*
Obviously in our macro experiment we do, but when we get to the quantum level we don't?
Everything that follows makes no sense at all to my poor brain. This rhetorical question confused me totally:
So how do both lights know to be the same colour when the switches are the in the same setting???
I thought that was obvious - the experimental setup more or less defines that this is the behaviour we should see. I'm not seeing any of this being relevant. Maybe its the 50% result, how is this possible? No wait, don't answer that, the question should be - 50% am I reading this right and is this relevant to entanglement somehow?

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cavediver
Member (Idle past 3669 days)
Posts: 4129
From: UK
Joined: 06-16-2005


Message 41 of 117 (313142)
05-18-2006 9:36 AM
Reply to: Message 40 by Modulous
05-18-2006 9:02 AM


Re: I'm terribly confused, but in a good way
*melting brain*
Is the desired and correct outcome. Einstein didn't object to this out of boredom But hey, according to RAZ, everyone from Einstein, Pauli, Fermi onwards has got it wrong and RAZ has cracked it and I'm 100 poorer
We have a box that fires a signal to two receivers.
Yes
That signal can be any one of the 2^3 states of a three string binary code
I've no idea. That might be a way of getting the observed output. Let's see...
The two receivers have a randomly selected switch that is either one of three settings. There are thus 3^2 switch positions.
Yes
When a receiver gets the signal it uses the switch setting as a rule to determine what colour light to illuminate
It appears so, but again, I haven't looked in the box so I am not sure. If you were to try to construct this experiment results yourself, it sounds like a good way of proceeding.
Position one selects 'bit' 1 of the string. For example if the string is RXX and the switch position is 1, the red light goes on.
I really don't know, but it sounds like a plan.
For any mixed string of Rs and Gs the we would expect to see 55.5% of the lights being the same. And if we include RRR and GGG (where for obvious reasons the lights are always the same), we conclude that we should see the same lights shine more than 55.5% of the time.
Yes, I agree. Your experiment should produce those results.
But we don't?
No, not in my experiment. But then, I don't know what's in my apparatus.
Obviously in our macro experiment we do, but when we get to the quantum level we don't?
No, my experiment built of real macro-sized objects produces the 50% result and your apparatus seems to produce 55%+.
My conclusion is that your apparatus is not a good model of my apparatus.
So how do both lights know to be the same colour when the switches are the in the same setting???
...when at the same time we observe 50% of the light pairs the same.
It's obvious if we allow 55%+, as that is what your experiment produces. But that's not what my experiment does...

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cavediver
Member (Idle past 3669 days)
Posts: 4129
From: UK
Joined: 06-16-2005


Message 42 of 117 (313143)
05-18-2006 9:40 AM
Reply to: Message 39 by Son Goku
05-18-2006 8:51 AM


Re: Entangelment and collapse.
So very true SG, but unfortunately explaining it this way just "supports" the idea of hidden variables. The mystery of the antisymmetric state only really becomes apparent through the probability argument.

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Son Goku
Inactive Member


Message 43 of 117 (313148)
05-18-2006 9:48 AM
Reply to: Message 42 by cavediver
05-18-2006 9:40 AM


Re: Entangelment and collapse.
That's true. Reading over it again it does kind of lend itself to it.
For anyboy who is interested the more modern version of Bell's experiments are called the Aspect experiments.
Described over the course of four pages here.

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cavediver
Member (Idle past 3669 days)
Posts: 4129
From: UK
Joined: 06-16-2005


Message 44 of 117 (313154)
05-18-2006 10:02 AM
Reply to: Message 40 by Modulous
05-18-2006 9:02 AM


Re: I'm terribly confused, but in a good way
By the way Mod, please realise that as obtuse as my reply sounds, I am attempting to get you to think about this the right way.
If we get the same colour when the switches are in the same position (but no knoweldge of which colour) then we conclude
a) some signal is being sent from one detector to the other to let it know the switch position
b) some pre-coding exists that enables the same colour to appear at both detectors.
c) something else
The whole business with the RGG nonsense is to show that there is no coding possible that gives the experiemental result. Thus we must abandon b). a) goes against all of relativity, so c) seems in order...

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Modulous
Member
Posts: 7801
From: Manchester, UK
Joined: 05-01-2005


Message 45 of 117 (313159)
05-18-2006 10:17 AM
Reply to: Message 41 by cavediver
05-18-2006 9:36 AM


and the penny begins to drop
I read your other reply, but I think this response works, because it did get me to think.
No, my experiment built of real macro-sized objects produces the 50% result and your apparatus seems to produce 55%+.
So the end result is that there is no coding scheme that could produce the same lights/same switch result and the 50% result at the same time? Is this related to Bell's Theorem that has been brought up? I should probably go try and understand that before going much further, huh?
We get the 50% result: something 'spooky' is going on (ie no coding and no other communication between boxes). I'll need to think on this one awhile (and re-read the thread a couple of times), but I think I understand better now, thanks. My next challenge is to try and understand RAZD's objections.

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 Message 41 by cavediver, posted 05-18-2006 9:36 AM cavediver has replied

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 Message 46 by cavediver, posted 05-18-2006 10:22 AM Modulous has not replied
 Message 47 by fallacycop, posted 05-18-2006 1:12 PM Modulous has not replied

  
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