Re: Cryonics punched cards and the brain

2016-04-29 Thread John Clark
On Fri, Apr 29, 2016 a John Mikes  wrote:

​> ​
> Bruno: do you have a good definition you could use for "physical"?
>

If it's physical then if it is of a large enough magnitude it can impact
one of the senses without any intermediary. That's why a number like a
billion is not physical, it has a large magnitude but a billion of
something is needed to effect the senses, a billion alone can't do
anything. A number is a idea, and a idea needs a physical brain to think it.

Given that Bruno talks about "3p" so much a better question to ask is "
Exactly what does the personal pronoun "you" mean?".  I didn't just provide
a list of synonyms,  ​I explained

​what "physical" means; but when Bruno is asked about "3p" it's all
circular definitions.

  John K Clark​

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Re: Non-locality and MWI

2016-04-29 Thread Bruce Kellett

On 29/04/2016 9:09 pm, Bruno Marchal wrote:

On 28 Apr 2016, at 03:33, Bruce Kellett wrote:
On 27/04/2016 4:57 pm, Bruno Marchal wrote:

On 27 Apr 2016, at 06:49, Bruce Kellett wrote:
On 27/04/2016 1:51 pm, Brent Meeker wrote:
That's pretty much the many-universes model that Bruno proposes. 
But it's non-local in the sense that the "matching scheme" must 
take account of which measurements are compatible, i.e. it "knows" 
the results even while they are  spacelike separated.
Exactly, the model assumes the results it is trying to get. It is 
not a local physical model because the statistics do not originate 
locally.


The statistic did originate locally. Alice and Bob did prepare the 
singlet state locally, and then travel away.


That is not strictly correct. The singlet state is conventionally 
prepared centrally between A and B so that the measurements can be 
made at spacelike separation. That would not be possible if A and B 
jointly prepare the state then move away.


The measurement? OK. Not the preparation.


They are in infinitely many worlds, and in each with opposite spin.


There are only two possible spin states for each -- so there are 
really only two distinct possible worlds. Multiplying copies of these 
two does not seem to accomplish much.


There is an infinity of possible states for each. There is an infinity 
of possible distinct possible worlds. In each one A's and B's particle 
spin are opposite/correlated, but neither Alice nor Bob can know which 
one.


I think you are getting confused by the basis problem again.


The cos^2(theta) is given by the math of the 1/sqrt(2)AB(I+>I-> - 
I->I+>)) = 1/sqrt(2)ABI+>I-> - 1/sqrt(2)ABI->I+>. With your 
explanation to Jesse, I keep the feeling that you talk like if Alice 
or Bob reduce the wave after their measurement, but they just 
localize themselves in the relative branches.


Certainly, the cos^2(theta/2) comes from applying the standard 
quantum rules to the singlet state
|psi> = (|+>|-> - |->|+>)/sqrt(2) (adding AB to this state adds 
nothing).


We need them to get all the statistics correct.

I think it would be instructive to actually go through the usual 
quantum derivation of the correlations because what you call 
"reducing the wave after the measurement" is actually the result of 
applying the standard quantum rules. It has nothing to do with 
so-called 'collapse' interpretations: it is simply in the theory.


Well, either the meaurement give specific outcome, or, if there is no 
physical collapse it is only an entanglement between A (or B) with the 
singlet state. That is why A and B are needed in the derivation.


A measurement results in an entanglement between the state and the 
observer. But in order for the observer to see only one result (and not 
a superposition) you need the projection postulate. That is decoherence, 
not a rejection of many worlds.


Quantum rules for measurement say that the initial state can be 
expanded in the basis corresponding to the particular measurement in 
question (contextuality). That is what the state |psi> above is -- 
the quantum expansion of the singlet state in the basis in which say 
Alice is doing her measurement.


OK, but that state does not represent two possible worlds. It looks 
like that for Alice because she has decided to make the measurement 
"in that base", but, as we know, the correlation does not depend on 
the choice of Alice's measurement. She will just entangled herself 
with the singlet state, whatever the base or measuring apparatus is.


Quantum rules then say that the result of the measurement (after 
decoherence has fully operated)


Decoherence is only the contagion of the superposition to the observer 
and/or his/her environment. It does not lead to a classical universe. 
That is only what the infinitely many Alice will phenomenologivally 
realize.


Decoherence is the basis for the (apparent) emergence of the classical 
from the quantum. Decoherence allows coarse-graining, partial tracing 
over environmental variables, and the other things that enable us to get 
definite experimental results.


is one of the eigenstates in the expansion, and the measurement 
result is the corresponding eigenvalue. In our case, there are two 
possibilities for Alice after her measurement is complete: result 
'+', with corresponding eigenstate |+>|->, or '-', with corresponding 
eigenstate |->|+>. There are no other possibilities, and Alice has a 
50% chance of obtaining either result, or of being in the 
corresponding branch of the evolved wave function.


That is correct phenomenologically. But QM-without collapse just say 
that we get a new Ipsi> equal to A(|+>|-> - |->|+>)/sqrt(2) = (A|+>|-> 
- A|->|+>)/sqrt(2). At no moment is Alice in front of only |+>|-> or 
|->|+>. The singlet state never disappear.


That is the basis of your confusion. What you are saying, in effect, is 
that the state is not reduced to the eigenvector corresponding to the 
obtained eigenvalue after meas

Re: Cryonics punched cards and the brain

2016-04-29 Thread John Mikes
Bruno: do you have a good definition you could use for "physical"?
(I mean: beyond what science calls physics in physical sciences).
*
In my agnostic mind whatever might be included into - even - some thinking
of potentially imaginable domains/factors/items/complexifiers etc. - "IS" -
existing in the Entirety of which we have had access only in a tiny-tiny
little fraction so far. Even that: adjusted to our (simple?) capabilities
of the 'contemporary'' human mind. (The perfect agnosticism).
I feel free to 'think' beyond whatever we can think of today.  Of course,
without substance. I.O.W.: to allow more to 'exist' than our knowables.

JOhn Mikes


On Wed, Apr 20, 2016 at 1:47 AM, Bruno Marchal  wrote:

>
> On 20 Apr 2016, at 00:12, John Clark wrote:
>
> On Tue, Apr 19, 2016 at 12:30 PM, Bruno Marchal  wrote:
> ​
>
>> ​> ​
>> "is" in which sense?
>>
>
> ​"​sense" in which sense?
>
> ​You must be a fan of Bill Clinton who notoriously said in answer to a
> question in a legal deposition:
>   ​
> "It depends on what the meaning of the word 'is' i
> ​s."​
>
>
>
>> ​> ​
>> Some multi or multimulti verses could be everything physical that there
>> is, but not everything needs to be physical
>>
>
> ​But physicists deal in the physical that why they're bored to tears when
> people start talking about what things would look like from places that are
> impossible to exist even in theory.  ​
>
>
>> ​> ​
>> exemple: the natural numbers, the complex numbers,
>>
>
> ​First of all we don't even know for certain that the Real Numbers exist
> much less the ​
>
> Complex Numbers, and even it they do they don't have a location. but a
> viewpoint ​does, it's a
> position of observation
> ​; ​and if that location is not inside the multiverse it does not exist.
>
>
>> ​> ​
>> but logically, it is conceivable to have structure containing themselves,
>>
>
> ​Fine, but it is not logical to have something that is not part of itself
> be part of itself; like a place that is not part of the multiverse you can
> ​stand on to look at it from the outside. The multiverse has no outside.
>
>
> That is why Nagel called it the point of view of nowhere, and sometimes I
> call something slightly similar the 0th person point of view. What you say
> does not refute what I said, given that here, the 0th point of view is
> given by the mathematics of the Everett Universal Wave. It just means that
> we look at the wave function of the universe assuming QM without collapse.
> And I have not use this, only any superposition coming from Alice and Bob
> entangling themselves with a singlet state (sometehing you have eliminate
> from the successive quotes, so we were leading astray from the topic).
>
> Bruno
>
>
>
> ​>> ​
>>> If the works of
>>> ​
>>> Galilee, Einstein
>>> ​
>>> or
>>> ​
>>> Maxwell
>>> ​
>>> were built on unphysical foundation
>>> ​s​
>>> then today nobody would remember their names, instead they are among the
>>> most
>>> ​famous​
>>>  physicists of all time. In fact Einstein came up with relativity by
>>> trying to imagine what the viewpoint would be of somebody moving at the
>>> speed of light and
>>> ​​
>>> discovered that viewpoint would produce logical contradictions
>>> ​,​
>>> and therefore CAN NOT EXIST.
>>
>>
>> ​> ​
>> No, he put itself at the place of a photon which does move at the speed
>> of light, and concluded to the laws of relativity and to the fact that the
>> photon can't have a mass non null. I think.
>>
>
> ​Einstein figured that ​if the fundamental laws of physics were worth
> anything then they must be true for any frame of reference, but from the
> frame of reference of somebody moving at 186,000 miles a second all
> electromagnetic waves would have a undulating shape that changes in space
> but not in time and light would have zero velocity. But that would be
> contrary to Maxwell's equations, therefore Einstein concluded that the
> viewpoint of a observer moving at 186,000 miles a second CAN NOT EXIST. And
> after that realization the rest of special relativity fell into place.
>
> ​> ​
>> Many works of many physicists are built in part (at least) on unphysical
>> foundation: mathematics.
>>
>
> I can't think of one. It's true that before Einstein proved them wrong
> people though non-Euclidean geometry was unphysical, but a place to stand
> outside the multiverse will always be unphysical because if it was physical
> it would be inside the multiverse.
>
>  John k Clark
>
>
>
>
>
> --
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>
> http://iridia.ulb.ac.be/~marchal/
>
>
>
> --
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Re: R: Re: R: Re: Non-locality and MWI

2016-04-29 Thread spudboy100 via Everything List
Here is a paper from the Journal of Cosmology, written by a comp sci professor 
at the University of Warwick, UK. I like it because of its logical flow, and, 
of course, no idea if its plausible, but it does correlate with MWI and the 
wave function, observers, and all that fun stuff of physics and 
computationalism. Anyone want to test drive this hypothesis and the logics? I 
like it, but don't know if this helps us? 



http://webcache.googleusercontent.com/search?q=cache:gSwPx43hKBsJ:journalofcosmology.com/JOC24/Forrest_Paper_2.pdf+&cd=2&hl=en&ct=clnk&gl=us


-Original Message-
From: Bruno Marchal 
To: everything-list 
Sent: Fri, Apr 29, 2016 8:19 am
Subject: Re: R: Re: R: Re: Non-locality and MWI




On 29 Apr 2016, at 09:41, 'scerir' via Everything List wrote:




 Da: spudboy100 via Everything List 
 Data: 28/04/2016 21.46
 A: 
 Ogg: Re: R: Re: Non-locality and MWI
 
 Is there any practical technical use for MWI as applied science. Just asking?
 

Dunno. Quantum computers?

Maybe there is a Many Interpretations Conjecture :-)


Interpretations of quantum mechanics, unlike Gods, are not jealous, and thus it 
is safe to
believe in more than one at the same time. 



Well, only because we tolerate non-sense in religion. I am not sure we can do 
that for a long time.









So if the many-worlds interpretation makes it
easier to think about the research you're doing in April, and the Copenhagen
interpretation makes it easier to think about the research you're doing in 
June, the
Copenhagen interpretation is not going to smite you for praying to the 
many-worlds
interpretation. At least I hope it won't, because otherwise I'm in big trouble.
---Peter Shor



Same with religion. We need only to have, relatively to the facts, consistent 
views, with ourselves, and eventually with each others.










I believe in every interpretation of quantum mechanics to the extent it points 
out
the problem, and disbelieve in every interpretation to the extent it claims to 
have solved it.

Good! I believe the same for the religions.


Bruno









--Scott Aaronson





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Re: R: Re: Non-locality and MWI

2016-04-29 Thread spudboy100 via Everything List
Ok, thanks. Yes, I read Deutsches interp some years back. I also like his 
later, Constructor theory, but this is sort of off topic. 



-Original Message-
From: Bruno Marchal 
To: everything-list 
Sent: Fri, Apr 29, 2016 8:09 am
Subject: Re: R: Re: Non-locality and MWI




On 29 Apr 2016, at 04:16, Stathis Papaioannou wrote:






On 29 April 2016 at 07:27, spudboy100 via Everything List 
 wrote:

Hah! Well somebody will get rich of we take the Everett stuff as fact. Not 
likely myself for all this. 

 
 
Sincerely,
 
Your humble clone



Kill off the poor ones and then you're sure to be the rich one.




That seems to me like cutting of the right part of a wooden rule to get only a 
left part.


Spudboy, MWI is only an attempt to make sense of QM. Its practical application 
is the same as QM. Now David Deustch would mention Quantum computer, that he 
discovered thanks to the MWI. 


MWI = taken the reality of the superposed states seriously, as already the two 
slits experiment with one photon illustrates that we should do.


For me, but also for Deutsch and for Everett MWI = QM-without collapse. 
Everett's published paper, even its long text, does not mention "many world" 
but only a new theory: the old one minus the physical collapse of the wave.


Bruno










 
-- 

Stathis Papaioannou
 



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Re: R: Re: R: Re: Non-locality and MWI

2016-04-29 Thread Bruno Marchal


On 29 Apr 2016, at 09:41, 'scerir' via Everything List wrote:



Da: spudboy100 via Everything List 
Data: 28/04/2016 21.46
A: 
Ogg: Re: R: Re: Non-locality and MWI

Is there any practical technical use for MWI as applied science.  
Just asking?



Dunno. Quantum computers?

Maybe there is a Many Interpretations Conjecture :-)

Interpretations of quantum mechanics, unlike Gods, are not jealous,  
and thus it is safe to


believe in more than one at the same time.



Well, only because we tolerate non-sense in religion. I am not sure we  
can do that for a long time.






So if the many-worlds interpretation makes it

easier to think about the research you're doing in April, and the  
Copenhagen


interpretation makes it easier to think about the research you're  
doing in June, the


Copenhagen interpretation is not going to smite you for praying to  
the many-worlds


interpretation. At least I hope it won't, because otherwise I'm in  
big trouble.


---Peter Shor



Same with religion. We need only to have, relatively to the facts,  
consistent views, with ourselves, and eventually with each others.






I believe in every interpretation of quantum mechanics to the extent  
it points out


the problem, and disbelieve in every interpretation to the extent it  
claims to have solved it.



Good! I believe the same for the religions.

Bruno





--Scott Aaronson




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Re: R: Re: R: Re: Cryonics punched cards and the brain

2016-04-29 Thread Bruno Marchal


On 15 Apr 2016, at 17:45, 'scerir' via Everything List wrote:


On 14 Apr 2016, at 20:25, 'scerir' via Everything List wrote:


MWI: "local" or not?

There are papers *trying* to explain "local" in MWI. In example:

http://philsci-archive.pitt.edu/504/2/cracow.pdf


That's a good one, imo.

..
..


Note that with computationalism, we might still expect some physical  
non-locality, and so it is my "physical intuition" which makes me  
skeptical. Despite I think that physics is only an appearance  
emerging from arithmetic see from inside by computable objects, I  
tend to infer from observation and reasoning that both QM and  
special relativity are plausibly correct, together with some minimal  
amount of physical realism (but not physical fundamentalism). Non  
locality would hurt badly that feeling. Physics would no more have  
any relation with a reality independent of ourself, and would go  
farer in weirdness than what we can expect from digital mechanism!


Bruno


Imo "local" (and perhaps also "deterministic") sounds crazy in MWI.  
"Separable" would be better?

?
On the contrary. MWI restores locality and deteminacy in the 3p  
picture, and get indeterminacy and non-locality in the first person  
plural views, well in accord with computationalism.






Right now, I'm reading something . “It appears that an  
understanding is possible via the notion of information. Information  
seen as the possibility of obtaining knowledge. Then quantum  
entanglement describes a situation where information exists about  
possible correlations between possible future results of possible  
future measurements without any information existing for the  
individual measurements. The latter explains quantum randomness, the  
first quantum entanglement. And both have significant consequences  
for our customary notions of causality. It remains to be seen what  
the consequences are for our notions of space and time, or space- 
time for that matter. Space-time itself cannot be above or beyond  
such considerations. I suggest we need a new deep analysis of space- 
time, a conceptual analysis maybe analogous to the one done by the  
Viennese physicist-philosopher Ernst Mach who kicked Newton’s  
absolute space and absolute time form their throne. The hope is that  
in the end we will have new physics analogous to Einstein’s new  
physics in the two theories of relativity.” --A. Zeilinger: http://edge.org/response-detail/26790




No problem with "information", except that the word is tarditionnally  
called in may different senses, and often blurr the distinction  
between the private meaning/intepretation of the 3p information, or  
just the 3p information like with Shannon. Then, the reasoning from  
computationalism, or from QM-without collapse, shows that you can't  
avoid the multidreams. If that is Zeilinger wish, I think it cannot be  
done. It would certainly make physics depart a lot of what we can  
expect from computationalism.


Bruno










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Re: R: Re: Non-locality and MWI

2016-04-29 Thread Bruno Marchal


On 29 Apr 2016, at 04:16, Stathis Papaioannou wrote:




On 29 April 2016 at 07:27, spudboy100 via Everything List > wrote:
Hah! Well somebody will get rich of we take the Everett stuff as  
fact. Not likely myself for all this.


Sincerely,
Your humble clone

Kill off the poor ones and then you're sure to be the rich one.


That seems to me like cutting of the right part of a wooden rule to  
get only a left part.


Spudboy, MWI is only an attempt to make sense of QM. Its practical  
application is the same as QM. Now David Deustch would mention Quantum  
computer, that he discovered thanks to the MWI.


MWI = taken the reality of the superposed states seriously, as already  
the two slits experiment with one photon illustrates that we should do.


For me, but also for Deutsch and for Everett MWI = QM-without  
collapse. Everett's published paper, even its long text, does not  
mention "many world" but only a new theory: the old one minus the  
physical collapse of the wave.


Bruno






--
Stathis Papaioannou

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Re: R: Re: Non-locality and MWI

2016-04-29 Thread spudboy100 via Everything List

Ah! Now you speak of the policies of the Ruling Class, which need no physics, 
or many worlds, just self centered behavior. Also, chances are via Hugh 
Everett, because I am not already rich, I am one of the others, as being a rich 
clone is not my wave function. 


-Original Message-
From: Stathis Papaioannou 
To: everything-list 
Sent: Thu, Apr 28, 2016 10:17 pm
Subject: Re: R: Re: Non-locality and MWI







On 29 April 2016 at 07:27, spudboy100 via Everything List 
 wrote:

Hah! Well somebody will get rich of we take the Everett stuff as fact. Not 
likely myself for all this.


Sincerely,
Your humble clone



Kill off the poor ones and then you're sure to be the rich one.


 
-- 

Stathis Papaioannou


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Re: Non-locality and MWI

2016-04-29 Thread Bruno Marchal


On 28 Apr 2016, at 03:33, Bruce Kellett wrote:


On 27/04/2016 4:57 pm, Bruno Marchal wrote:

On 27 Apr 2016, at 06:49, Bruce Kellett wrote:
On 27/04/2016 1:51 pm, Brent Meeker wrote:
That's pretty much the many-universes model that Bruno proposes.  
But it's non-local in the sense that the "matching scheme" must  
take account of which measurements are compatible, i.e. it  
"knows" the results even while they are  spacelike separated.
Exactly, the model assumes the results it is trying to get. It is  
not a local physical model because the statistics do not originate  
locally.


The statistic did originate locally. Alice and Bob did prepare the  
singlet state locally, and then travel away.


That is not strictly correct. The singlet state is conventionally  
prepared centrally between A and B so that the measurements can be  
made at spacelike separation. That would not be possible if A and B  
jointly prepare the state then move away.


The measurement? OK. Not the preparation.





They are in infinitely many worlds, and in each with opposite spin.


There are only two possible spin states for each -- so there are  
really only two distinct possible worlds. Multiplying copies of  
these two does not seem to accomplish much.



There is an infinity of possible states for each. There is an infinity  
of possible distinct possible worlds. In each one A's and B's particle  
spin are opposite/correlated, but neither Alice nor Bob can know which  
one.







The cos^2(theta) is given by the math of the 1/sqrt(2)AB(I+>I-> - I- 
>I+>)) = 1/sqrt(2)ABI+>I-> - 1/sqrt(2)ABI->I+>. With your  
explanation to Jesse, I keep the feeling that you talk like if  
Alice or Bob reduce the wave after their measurement, but they just  
localize themselves in the relative branches.


Certainly, the cos^2(theta/2) comes from applying the standard  
quantum rules to the singlet state
|psi> = (|+>|-> - |->|+>)/sqrt(2) (adding AB to this state adds  
nothing).


We need them to get all the statistics correct.


I think it would be instructive to actually go through the usual  
quantum derivation of the correlations because what you call  
"reducing the wave after the measurement" is actually the result of  
applying the standard quantum rules. It has nothing to do with so- 
called 'collapse' interpretations: it is simply in the theory.


Well, either the meaurement give specific outcome, or, if there is no  
physical collapse it is only an entanglement between A (or B) with the  
singlet state. That is why A and B are needed in the derivation.







Quantum rules for measurement say that the initial state can be  
expanded in the basis corresponding to the particular measurement in  
question (contextuality). That is what the state |psi> above is --  
the quantum expansion of the singlet state in the basis in which say  
Alice is doing her measurement.


OK, but that state does not represent two possible worlds. It looks  
like that for Alice because she has decided to make the measurement  
"in that base", but, as we know, the correlation does not depend on  
the choice of Alice's measurement. She will just entangled herself  
with the singlet state, whatever the base or measuring apparatus is.




Quantum rules then say that the result of the measurement (after  
decoherence has fully operated)


Decoherence is only the contagion of the superposition to the observer  
and/or his/her environment. It does not lead to a classical universe.  
That is only what the infinitely many Alice will phenomenologivally  
realize.




is one of the eigenstates in the expansion, and the measurement  
result is the corresponding eigenvalue. In our case, there are two  
possibilities for Alice after her measurement is complete: result  
'+', with corresponding eigenstate |+>|->, or '-', with  
corresponding eigenstate |->|+>. There are no other possibilities,  
and Alice has a 50% chance of obtaining either result, or of being  
in the corresponding branch of the evolved wave function.


That is correct phenomenologically. But QM-without collapse just say  
that we get a new Ipsi> equal to A(|+>|-> - |->|+>)/sqrt(2) = (A|+>|->  
- A|->|+>)/sqrt(2). At no moment is Alice in front of only |+>|-> or   
|->|+>. The singlet state never disappear.






The question now arises as to how the formalism describes Bob's  
measurement, assuming that it follows that of Alice (there will  
always be a Lorentz frame in which that is true for spacelike  
separations. For timelike separations, it is either true, or we  
reverse the A/B labels so that it is true.) Since the description of  
the state does not depend on the separation between A and B, after A  
gets '+' and her eigenstate is |+>|->, Bob must measure the state |- 
> in the direction of his magnet. To get the relative probabilities  
for his results, we must rotate the eigenfunction from Alice's basis  
to the basis appropriate for Bob's measurement. This is the standard  
rotation of a spinor,

R: Re: R: Re: Non-locality and MWI

2016-04-29 Thread 'scerir' via Everything List


Da: spudboy100 via Everything List 

Data: 28/04/2016 21.46

A: 

Ogg: Re: R: Re: Non-locality and MWI



Is there any practical technical use for MWI as applied science. Just asking?



Dunno. Quantum computers?

Maybe there is a Many Interpretations Conjecture :-)

Interpretations
of quantum mechanics, unlike Gods, are not jealous, and thus it is safe to

believe
in more than one at the same time. So if the many-worlds interpretation makes
it

easier
to think about the research you're doing in April, and the Copenhagen

interpretation
makes it easier to think about the research you're doing in June, the

Copenhagen
interpretation is not going to smite you for praying to the many-worlds

interpretation.
At least I hope it won't, because otherwise I'm in big trouble.

---Peter
Shor
I believe in every interpretation of quantum mechanics to the extent it points 
outthe problem, and disbelieve in every interpretation to the extent it claims 
to have solved it.--Scott Aaronson

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