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Woit · 2025-10-20
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§25 · en · machine_draft · machine-draft-not-reviewed
This method turns unitary symmetries of classical phase space into unitary representations of symmetry groups on quantum state spaces. It is explained in detail here because it applies to simple systems such as the -dimensional harmonic oscillator and will also be fundamental to our later study of quantum field theory. In that setting, the observables of interest are operators in a Lie algebra representation, built from quadratic combinations of annihilation and creation operators. They arise from the constructions in this chapter applied to unitary group actions on phase space, which is infinite-dimensional in quantum field theory.