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  2. Bohr–Einstein debates - Wikipedia

    en.wikipedia.org/wiki/Bohr–Einstein_debates

    These thoughts of Einstein would set off a line of research into hidden variable theories, such as the Bohm interpretation, in an attempt to complete the edifice of quantum theory. If quantum mechanics can be made complete in Einstein's sense, it cannot be done locally; this fact was demonstrated by John Stewart Bell with the formulation of ...

  3. Quantum nonlocality - Wikipedia

    en.wikipedia.org/wiki/Quantum_nonlocality

    Bohmian mechanics provides such a completion of quantum mechanics, with the introduction of hidden variables; however the theory is explicitly nonlocal. [18] The interpretation therefore does not give an answer to Einstein's question, which was whether or not a complete description of quantum mechanics could be given in terms of local hidden ...

  4. Quantum entanglement - Wikipedia

    en.wikipedia.org/wiki/Quantum_entanglement

    Quantum entanglement is the phenomenon of a group of particles being generated, interacting, or sharing spatial proximity in such a way that the quantum state of each particle of the group cannot be described independently of the state of the others, including when the particles are separated by a large distance.

  5. No-communication theorem - Wikipedia

    en.wikipedia.org/wiki/No-communication_theorem

    In physics, the no-communication theorem (also referred to as the no-signaling principle) is a no-go theorem in quantum information theory. It asserts that during the measurement of an entangled quantum state , it is impossible for one observer to transmit information to another observer, regardless of their spatial separation.

  6. Action at a distance - Wikipedia

    en.wikipedia.org/wiki/Action_at_a_distance

    Albert Einstein wrote to Max Born about issues in quantum mechanics in 1947 and used a phrase translated as "spooky action at a distance", and in 1964, John Stewart Bell proved that quantum mechanics predicted stronger statistical correlations in the outcomes of certain far-apart measurements than any local theory possibly could. [25]

  7. Bell's theorem - Wikipedia

    en.wikipedia.org/wiki/Bell's_theorem

    Einstein argued persistently that quantum mechanics could not be a complete theory. His preferred argument relied on a principle of locality: Consider a mechanical system constituted of two partial systems A and B which have interaction with each other only during limited time. Let the ψ function before their interaction be given.

  8. Principle of locality - Wikipedia

    en.wikipedia.org/wiki/Principle_of_locality

    The principle of locality plays a critical role in one of the central results of quantum mechanics. In 1935 Albert Einstein, Boris Podolsky, and Nathan Rosen, with their EPR paradox thought experiment, raised the possibility that quantum mechanics might not be a complete theory.

  9. History of quantum mechanics - Wikipedia

    en.wikipedia.org/wiki/History_of_quantum_mechanics

    The end of the first era of quantum mechanics was triggered by de Broglie's publication of his hypothesis of matter waves, [1]: 268 leading to Schrödinger's discovery of wave mechanics for matter. Accurate predictions of the absorption spectrum of hydrogen ensured wide acceptance of the new quantum theory. [1]: 275