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No-go theorem

In theoretical physics, a no-go theorem is a theorem that states that a particular situation is not physically possible. Specifically, the term describes results in quantum mechanics like Bell's theorem and the Kochen–Specker theorem that constrain the permissible types of hidden variable theories which try to explain the apparent randomness of quantum mechanics as a deterministic model featuring hidden states. In theoretical physics, a no-go theorem is a theorem that states that a particular situation is not physically possible. Specifically, the term describes results in quantum mechanics like Bell's theorem and the Kochen–Specker theorem that constrain the permissible types of hidden variable theories which try to explain the apparent randomness of quantum mechanics as a deterministic model featuring hidden states. The Weinberg–Witten theorem states that massless particles (either composite or elementary) with spin j > ​1⁄2 cannot carry a Lorentz-covariant current, while massless particles with spin j > 1 cannot carry a Lorentz-covariant stress-energy. The theorem is usually interpreted to mean that the graviton (j = 2) cannot be a composite particle in a relativistic quantum field theory. In quantum information theory, a no-communication theorem is a result that gives conditions under which instantaneous transfer of information between two observers is impossible.

[ "Brouwer fixed-point theorem", "Fundamental theorem", "Picard–Lindelöf theorem", "No-cloning theorem", "Quantum no-deleting theorem", "Haag's theorem", "Full employment theorem", "Superdeterminism", "Rice–Shapiro theorem", "Erdős–Kac theorem", "No-broadcast theorem", "Free will theorem", "Gap theorem" ]
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