[ExI] R: Re: Cramer on impossibility of FTL communication
scerir at alice.it
scerir at alice.it
Wed Sep 2 18:06:46 UTC 2015
----Messaggio originale----
Da: atymes at gmail.com
Data: 1-set-2015 2.27
A: "ExI chat list"<extropy-chat at lists.extropy.org>
Cc: <scerir at alice.it>
Ogg: Re: [ExI] Cramer on impossibility of FTL communication
In this case, the problem seems to be the limited speed of transmission of information about the information.
If you entangle photons A and B, let B travel away, then measure A, you know what B is...but your knowledge of it is not immediately available where B is. You can tell people, but that itself does not travel faster than light. As far as B and those around it are concerned, B remains entangled until the light cone of your measurement of A reaches them.
Is that not the case?
######
Hi Adrian,
Yes and no.
If you have a source of entangled photons and this source is much much closer to
location A than to location B, and if A and B are close enough, an observer O could jump from A to B and you can imagine he could perform magic tricks.
In other words ... in general the problem arises because obsevers are
local, and quantum correlations are not. But if you have ... nonlocal
observers ....
No story in space-time can describe nonlocal correlations: we have no tool
in our story-toolbox to talk about nonlocal correlations (Gisin). Hence,
we usually say things like "event A influences event B", or
"event A has a spooky action at a distance on event B" or
"event A causes a collapse of the wavefunction at location B".
But we know that this is all wrong: there is no time ordering between the
events A and B ("acausality"). Hence no story in time is
appropriate. Moreover, the distance between A and B is irrelevant. Hence
the distance should not occur in our story.
A good review paper about all that (and about many different - and very
often also smart - attempts to build quantum signalling machines) is this
one, by GianCarlo Ghirardi
http://arxiv.org/abs/1305.2305.
See also
http://arxiv.org/abs/1306.1133
http://arxiv.org/abs/1411.0893 .
Ghirardi is the "G" of the GRW interpretation.
For different arguments see Gisin here (Appendix B)
http://arxiv.org/pdf/1011.3440v1.pdf
Scarani and Gisin here
http://www.unige.ch/gap/quantum/_media/publications:bib:v35_328.pdf
Another interesting point is the speed of quantum information or, to say it
better, the speed of quantum "influences" (between the two parts
of the entangled quantum system, i.e. the two parts of a bi-photon). There
are
many interesting papers.
http://arxiv.org/abs/1110.3795 (The experimental violation of Bell
inequalities using spacelike separated measurements precludes the
explanation of quantum correlations through causal influences propagating
at subluminal speed. Yet, any such experimental violation could always be
explained in principle through models based on hidden influences
propagating at a finite speed v>c, provided v is large enough. Here, we
show that for any finite speed v with c<v<infinity, such models
predict correlations that can be exploited for faster-than-light
communication. This superluminal communication does not require access to
any hidden physical quantities, but only the manipulation of measurement
devices at the level of our present-day description of quantum
experiments. Hence, assuming the impossibility of using nonlocal
correlations for superluminal communication, we exclude any possible
explanation of quantum correlations in terms of influences propagating at
any finite speed. Our result uncovers a new aspect of the complex
relationship between multipartite quantum nonlocality and the
impossibility of signalling.)
http://arxiv.org/abs/1304.0532 (We discuss models that attempt to provide
an explanation for the violation of Bell inequalities at a distance in
terms of hidden influences. These models reproduce the quantum
correlations in most situations, but are restricted to produce local
correlations in some configurations. The argument presented in Bancal et
al., Nature Physics 8, 867, (2012), applies to all of these models, which
can thus
be proved to allow for faster-than-light communication. In other words, the
signalling character of these models cannot remain hidden.)
http://arxiv.org/abs/1011.3440 (Are There Quantum Effects Coming from
Outside Space-time? Nonlocality, free will and "no many-worlds".)
http://arxiv.org/abs/1002.1392 (In Bell inequality tests, the evolution of
the wavefunction is not covariant, i.e. not invariant under velocity boost
that change the time ordering of events, but the laws that govern the
probability distribution of possible results are. In this note I
investigate what this could mean and whether there could be some covariant
"real quantum stuff". This clarifies the implication of the Free
Will Theorem and of relativistic spontaneous localization models based on
the flash ontology (GRW). Some implications for the concept of time(s) are
spelled out.)
http://arxiv.org/abs/0808.3316 (A real spooky action at a distance
wouldrequire a faster than light influence defined in some hypothetical
universally privileged reference frame. Here we put stringent experimental
bounds on the speed of all such hypothetical influences. We performed a
Bell test during more than 24 hours between two villages separated by 18
km and approximately east-west oriented, with the source located precisely
in the middle. We continuously observed 2-photon interferences well above
the Bell inequality threshold. Taking advantage of the Earth's
rotation, the configuration of our experiment allowed us to determine, for
any hypothetically privileged frame, a lower bound for the speed of this
spooky influence. For instance, if such a privileged reference frame
exists and is such that the Earth's speed in this frame is less than
10^-3 that of the speed of light, then the speed of this spooky influence
would have to exceed that of light by at least 4 orders of magnitude.)
http://arxiv.org/abs/quant-ph/0212078 (We study the apparent nonlocality of
quantum mechanics as a transport problem. If space is a physical entity
through which quantum information QI must be transported, then one can
define its speed. If not, QI exists apart from space, making space in some
sense 'nonphysical'. But we can still assign a `speed' of QI
to such models based on their properties. In both cases, classical
information must still travel at "c", though in the latter case
the origin of local spacetime itself is a puzzle. We consider the
properties of different regimes for this speed of QI, and relevant quantum
interpretations. For example, we show that the Many Worlds Interpretation
MWI is nonlocal because it is what we call `spatially complete'.)
http://arxiv.org/abs/quant-ph/0508016 (This article identifies a series of
properties common to all theories that do not allow for superluminal
signaling and predict the violation of Bell inequalities. Intrinsic
randomness, uncertainty due to the incompatibility of two observables,
monogamy of correlations, impossibility of perfect cloning, privacy of
correlations, bounds in the shareability of some states; all these
phenomena are solely a consequence of the no-signaling principle and
nonlocality. In particular, it is shown that for any distribution, the
properties of (i) nonlocal, (ii) no arbitrarily shareable and (iii)
positive secrecy content are equivalent.)
http://arxiv.org/abs/quant-ph/0503007 (In relativity there is space-time
out there. In quantum mechanics there is entanglement. Entanglement
manifests itself by producing correlations between classical events (e.g.
the firing of some detectors) at any two space-time locations. If the
locations are time-like separated, i.e. one is in the future of the other,
then there is no specific difficulty to understand the correlations. But
if the two locations are space-like separated, the problem is different.
How can the two space-time locations out there know about what happens in
each other without any sort of communication? If space-time really exists,
the locations must do something like communicating. Or it was all set up
at the Beginning. But the correlations depend also on the free choice of
the experimentalists, one in each space-time location. This allowed John
Bell to derive his inequality and the experimentalists to violate it, thus
refuting the assumption that it was all set up at the beginning: the
Correlations can't be explained by common causes.)
http://arxiv.org/abs/quant-ph/0410025 (Since Bell's theorem, it is
known that quantum correlations cannot be described by local variables
(LV) alone: if one does not want to abandon classical mechanisms for
correlations, a superluminal form of communication among the particles
must be postulated. A natural question is whether such a postulate would
imply the possibility of superluminal signaling. Here we show that the
assumption of finite-speed superluminal communication indeed leads to
signaling when no LV are present, and more generally when only LV
derivable from quantum statistics are allowed. When the most general LV
are allowed, we
prove in a specific case that the model can be made again consistent with
relativity, but the question remains open in general.)
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