Department of Physics, Ben Gurion University 

Highlights  
Constraints on quantum mechanics()Daniel Rohrlich The axioms of quantum mechanics are well known, but most of them are abstract and mathematical. They are not clear physical statements like the two axioms of special relativity, defining a maximal signalling speed (the speed of light) and a fundamental symmetry (Lorentz invariance). Can we derive quantum mechanics from clear physical statements? Or, if we are not there yet, can we at least formulate clear physical statements that constrain quantum mechanics and any generalization of quantum mechanics? Suprisingly  to say the least  the assumption that every physical value exists before we measure it (regardless of what goes on elsewhere) does not constrain quantum mechanics. This "local realism" assumption implies Bell's inequality, and quantum mechanics violates Bell's inequality. In particular, one form of Bell's inequality says that a certain combination \( C \) of measured correlations must not exceed \( 2 \) . But in quantum mechanics, \( C \) can reach \( 2\sqrt{2} \) . This fact is called "Tsirelson's bound", and it is a theorem of quantum mechanics. Quantum mechanics does obey the nosignalling constraint (the first axiom of special relativity): quantum correlations are useless for sending fasterthanlight signals. Does Tsirelson's bound follow from this constraint? No, it does not; as Sandu Popescu and I showed in Ref. \( [1] \) , hypothetical "superquantum" correlations (now also called PopescuRohrlichbox ("PRbox") correlations as in Ref. \( [2] \) ) can reach \( C = 4 \) without violating the nosignalling constraint. So where does Tsirelson's bound come from? Quantum mechanics obeys another constraint, besides nosignalling: it has a classical limit, in which Planck's constant \( h \) vanishes and all physical values are measurable. In this limit, I have found 3 that PRbox correlations do not obey the nosignalling constraint. Generalized to all strongerthanquantum correlations, this result is a derivation of Tsirelson's bound without assuming quantum mechanics. So we can derive at least a part of quantum mechanics from the two axioms of nosignalling and a classical limit, together with the negation of local realism. For further details, see Refs. \( [3{}5] \) . The work of \( [4] \) continues in collaboration with Avishy Carmi and Daniel Moskovich of the Mechanical Engineering Department and the Center for Quantum Information Science and Technology at BGU.


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