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Symplectomorphism
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==Quantizations== Representations of finite-dimensional subgroups of the group of symplectomorphisms (after Δ§-deformations, in general) on [[Hilbert space]]s are called ''quantizations''. When the Lie group is the one defined by a Hamiltonian, it is called a "quantization by energy". The corresponding operator from the [[Lie algebra]] to the Lie algebra of continuous linear operators is also sometimes called the ''quantization''; this is a more common way of looking at it in physics. {{see also| phase space formulation| geometric quantization|non-commutative geometry}}
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