Definition

A qutrit is a quantum system whose state is three-dimensional over C\mathbb C, hence isomorphic after choosing an to

HC3.H\cong\mathbb C^3.

Its pure states are rays in C3\mathbb C^3, and its general states are positive trace-one operators ρM3(C)\rho\in M_3(\mathbb C).

Coordinates and observables

In a basis {0,1,2}\{|0\rangle,|1\rangle,|2\rangle\}, a is

ψ=α0+β1+γ2,α2+β2+γ2=1,|\psi\rangle=\alpha|0\rangle+\beta|1\rangle+\gamma|2\rangle, \qquad |\alpha|^2+|\beta|^2+|\gamma|^2=1,

modulo a common phase. Thus the pure-state space is CP2\mathbb{CP}^2.

The observables are

h3(C)={AM3(C):A=A},\mathfrak h_3(\mathbb C)=\{A\in M_3(\mathbb C):A^*=A\},

a real under AB=12(AB+BA)A\circ B=\tfrac12(AB+BA); see the .

Comparison with a qubit

A qutrit has three basis levels rather than two. Its mixed-state space is not a Euclidean ball: the Bloch-ball description is special to two dimensions. A chosen two-dimensional subspace of C3\mathbb C^3 determines an embedded , but no such subspace is canonical without extra data.

“Octonionic qutrit” terminology

The h3(O)\mathfrak h_3(\mathbb O) resembles h3(C)\mathfrak h_3(\mathbb C) with octonionic entries and is informally called the observable algebra of an “octonionic qutrit.” This is an analogy about , not an ordinary complex-Hilbert-space qutrit.

References
  1. Michael A. Nielsen and Isaac L. Chuang, Quantum Computation and Quantum Information, tenth-anniversary edition, Cambridge University Press, 2010. DOI record. Relevant: finite-dimensional state spaces and density operators.
  2. John C. Baez and Paul Schwahn, “The Standard Model Gauge Group from the Exceptional Jordan Algebra,” 2026. arXiv record. Relevant: §1.