Two elementary proofs of the Wigner theorem on symmetry in quantum mechanics
arXiv:0808.0779 · doi:10.1016/j.physleta.2008.09.052
Abstract
In quantum theory, symmetry has to be defined necessarily in terms of the family of unit rays, the state space. The theorem of Wigner asserts that a symmetry so defined at the level of rays can always be lifted into a linear unitary or an antilinear antiunitary operator acting on the underlying Hilbert space. We present a proof of this theorem which is both elementary and economical. Central to our proof is the recognition that a given Wigner symmetry can, by post-multiplication by a unitary symmetry, be taken into either the identity or complex conjugation. Our analysis involves a judicious interplay between the effect a given Wigner symmetry has on certain two-dimensional subspaces and the effect it has on the entire Hilbert space.
arXiv commentA second proof of Wigner's theorem added and, consequently, the title slightly changed. 8 pages, Latex, no figures
References in corpus (3)
Cited by in corpus (15)
- An elementary proof for the non-bijective version of Wigner's theorem
- Applications of Noether conservation theorem to Hamiltonian systems
- An alternative proof of Wigner theorem on quantum transformations based on elementary complex analysis
- Generalising Wigner's theorem
- Reflections on the four facets of symmetry: how physics exemplifies rational thinking
- Prepare-and-Magic: Semi-Device Independent Magic Certification in the Prepare-and-Measure Scenario
- Revisiting quantum field theory in Rindler spacetime with superselection rules
- Supercomputer simulations of transmon quantum computers
- Classical Light Beams and Geometric Phases
- Wigner's Theorem for stabilizer states and quantum designs
- Are almost-symmetries almost linear?
- (No) Wigner Theorem for C*-algebras
- Enlargement of symmetry groups in physics: a practitioner's guide
- Wigner's theorem revisited
- Some aspects of the interplay between bipartite correlations and quantum channels