nLab quantum observables as groupoid convolution -- references

Quantum observable algebras as Groupoid algebras

Quantum observable algebras as Groupoid algebras

The original derivation of the Heisenberg picture of quantum mechanics, introducing N×NN \times N matrix algebra for transitions between NN measurable states of atomic spectra, by

was argued by

to be fruitfully understood as the groupoid convolution algebra of the pair groupoid of transitions between NN elements.

Later but more generally, the “algebra of (selective) measurement” originally envision by

is argued to be, in modern language, the groupoid convolution algebras of groupoids whose morphisms reflect transitions between possible quantum measurement-outcomes – by:

and as such further developed in:

Proof that non-perturbative quantum observables on Yang-Mill fluxes through a surface form a convolution algebra:

Last revised on March 1, 2025 at 11:48:23. See the history of this page for a list of all contributions to it.