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An operational approach to spacetime symmetries: Lorentz transformations from quantum communication

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An operational approach to spacetime symmetries: Lorentz transformations from quantum communication
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In most approaches to fundamental physics, spacetime symmetries are postulated a priori and then explicitly implemented in the theory. This includes Lorentz covariance in quantum field theory and diffeomorphism invariance in quantum gravity, which are seen as fundamental principles to which the final theory has to be adjusted. In this paper, we suggest, within a much simpler setting, that this kind of reasoning can actually be reversed, by taking an operational approach inspired by quantum information theory. We consider observers in distinct laboratories, with local physics described by the laws of abstract quantum theory, and without presupposing a particular spacetime structure. We ask what information-theoretic effort the observers have to spend to synchronize their descriptions of local physics. If there are 'enough' observables that can be measured universally on several different quantum systems, we show that the observers' descriptions are related by an element of the orthochronous Lorentz group , together with a global scaling factor. Not only does this operational approach predict the Lorentz transformations, but it also accurately describes the behavior of relativistic Stern–Gerlach devices in the WKB approximation, and it correctly predicts that quantum systems carry Lorentz group representations of different spin. This result thus hints at a novel information-theoretic perspective on spacetime.
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Source <Elektronik>SpinFeldquantSpezifisches GewichtElektronBildqualitätAngeregter ZustandNetztransformatorBasis <Elektrotechnik>DiagrammFlussdiagrammComputeranimation
MessungFeldquantMessgerätTeilchenZylinderblockSpinWeltraumSpiel <Technik>MonatEisenbahnbetriebMessungPatrone <Munition>FeldquantFACTS-AnlageVorlesung/Konferenz
MessungComputeranimationFlussdiagramm
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ALICE <Teilchendetektor>Satz <Drucktechnik>WarmumformenGruppenlaufzeitFeldquantTagesanbruchSchwache LokalisationBlatt <Papier>Angeregter ZustandProzessleittechnikCocktailparty-EffektPagerKalenderjahrVorlesung/Konferenz
Transkript: Englisch(automatisch erzeugt)
In the last few years, a new paradigm has emerged in theoretical physics. This paradigm seeks to understand space-time structure through concepts from quantum information. For example, one studies the interplay of geometries and entanglement entropies and tries to understand in particular the emergence of geometry from universal entanglement properties of quantum systems.
In our paper, we ask a different kind of question, but still within the same paradigm. We ask, is there a quantum origin to the local symmetry group of space-time? In other words, can we understand the Lorentz transformations from a quantum information perspective? Now, the Lorentz transformations have an inherently operational interpretation,
namely they translate between different reference frames, and as such they translate between different descriptions of the same physics. But the physics that all observers describe is ultimately quantum in nature, and therefore it's natural to ask, if we have different observers describing quantum physics, how can the descriptions differ and how can these different descriptions be related?
The key point is that we ask this question without assuming a specific space-time structure, and in particular we do not assume what the signature even dimension of space-time is, we only assume the validity of quantum theory in the local laboratories of observers. In our paper, we then actually derive the Lorentz transformations
of 3-plus-1-dimensional Minkowski space in this framework under certain assumptions. Now what are these assumptions and how do we achieve this? We have two observers, Alice and Bob, in their local laboratories, who have never met before, but can communicate. We consider the following task. Alice asks Bob on the phone to send her a specific quantum state.
If they have never met before, they will describe quantum states differently, and so Bob will not know Alice's choice of bases, and he will send the wrong quantum state. For any specific quantum system, for example an electron, Alice and Bob can synchronize the descriptions. For example, by sending a complete basis of states,
they can find a transformation, let's call it t, that translates Alice's description into Bob's. This synchronization allows them to win the game. But do they have to repeat the synchronization for all kinds of quantum systems? This could become an arbitrarily complex task, because there may be infinitely many different kinds of systems,
and a priori, the synchronizations for different kinds of systems could be unrelated. But we know from experience that this is not the case in our universe. The synchronization for all systems are related. We therefore ask, how can one understand this empirical fact from a quantum information perspective? We identify a new concept that offers an operational account for this,
the concept of universal measurement devices. Such a device allows an observer to measure a fixed observable on different kinds of quantum systems universally. For example, think of a Stern-Gerlach device that measures the spin of different kinds of particles. The key benefit is that these devices allow observers to transfer the synchronization of one kind of system to another.
We show that if there are sufficiently many universally measurable observables, then Alice and Bob can synchronize their descriptions of all quantum systems at once. And if certain consistency conditions are satisfied, we show that this gives rise to the Lorentz group. So how do we interpret this result?
Have we now re-derived special relativity in the dimension and signature of space-time? Not directly, because our setting does not by itself view the immediate geometric space-time picture. However, the result is very suggestive of the space-time interpretation, because after all, the local symmetry group of space-time is nothing but the dictionary between different observer's descriptions of physics.
Our paper therefore does propose a new quantum information perspective on the origin of the local symmetry group and thereby the dimension and signature of space-time. And this is what we seek to exploit in further work.