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Physlib.QuantumMechanics.OperatorAlgebra.Dynamics.Automorphism

Automorphisms of the bounded operators

Reversible transformations of a quantum system act on its observable algebra by ⋆-automorphisms.

For a complex Hilbert space `H`, every ⋆-automorphism of `B(H)` is implemented by unitary conjugation: `A ↦ U A U⋆`.

Two unitaries implement the same transformation exactly when they differ by a scalar phase. Consequently, `Aut⋆(B(H)) ≅ U(H) / U(1) ≅ PU(H)`, the projective unitary group.

For Hamiltonian dynamics, this projective ambiguity corresponds to the freedom to shift a Hamiltonian by a scalar multiple of the identity.

5 declarations

theorem

Every ⋆\star-automorphism of B(H)\mathcal{B}(H) is a unitary conjugation

Let HH be a complex Hilbert space and B(H)\mathcal{B}(H) be the algebra of bounded linear operators on HH. Every C\mathbb{C}-algebra ⋆\star-automorphism Φ:B(H)→B(H)\Phi: \mathcal{B}(H) \to \mathcal{B}(H) is implemented by unitary conjugation. That is, for any such ⋆\star-automorphism Φ\Phi, there exists a unitary operator U∈B(H)U \in \mathcal{B}(H) such that Φ(A)=UAU∗\Phi(A) = U A U^* for all A∈B(H)A \in \mathcal{B}(H).

theorem

Equality of unitary automorphisms of B(H)\mathcal{B}(\mathcal{H}) iff unitaries differ by a scalar phase

Let H\mathcal{H} be a complex Hilbert space and B(H)\mathcal{B}(\mathcal{H}) denote the algebra of bounded linear operators on H\mathcal{H}. For any two unitary operators u,v∈B(H)u, v \in \mathcal{B}(\mathcal{H}), the ⋆\star-automorphisms of B(H)\mathcal{B}(\mathcal{H}) implemented by conjugation—defined by A↦uAu∗A \mapsto uAu^* and A↦vAv∗A \mapsto vAv^* respectively—are equal if and only if there exists a scalar phase c∈U(1)c \in U(1) (i.e., a complex number cc with ∣c∣=1|c| = 1) such that u=cvu = cv.

definition

Projective unitary group PU(H)PU(\mathcal{H})

Let H\mathcal{H} be a complex Hilbert space. The **projective unitary group** PU(H)PU(\mathcal{H}) is defined as the quotient of the group of unitary operators U(H)U(\mathcal{H}) by the kernel of the conjugation homomorphism Ad:U(H)→Aut⋆(B(H))\text{Ad}: U(\mathcal{H}) \to \text{Aut}_{\star}(\mathcal{B}(\mathcal{H})), which maps a unitary UU to the ⋆\star-automorphism A↦UAU∗A \mapsto U A U^*. This quotient identifies unitary operators that differ only by a scalar phase c∈Cc \in \mathbb{C} (where ∣c∣=1|c| = 1).

instance

PU(H)PU(\mathcal{H}) is a group

Let H\mathcal{H} be a complex Hilbert space. The projective unitary group PU(H)PU(\mathcal{H}) is equipped with a group structure. This structure is the quotient group structure derived from the unitary group U(H)U(\mathcal{H}) and the kernel of the conjugation homomorphism Ad:U(H)→Aut⋆(B(H))\text{Ad}: U(\mathcal{H}) \to \text{Aut}_{\star}(\mathcal{B}(\mathcal{H})).

definition

Group isomorphism PU(H)≅Aut⋆(B(H))PU(H) \cong \text{Aut}_{\star}(\mathcal{B}(H))

Let HH be a complex Hilbert space and B(H)\mathcal{B}(H) be the algebra of bounded linear operators on HH. There is a group isomorphism between the projective unitary group PU(H)PU(H) and the group of C\mathbb{C}-algebra ⋆\star-automorphisms of B(H)\mathcal{B}(H), denoted by Aut⋆(B(H))\text{Aut}_{\star}(\mathcal{B}(H)). This isomorphism identifies each projective unitary (an equivalence class of unitaries [U][U]) with the unique ⋆\star-automorphism it implements via conjugation, A↦UAU∗A \mapsto UAU^*.