Physlib

QuantumInfo.ForMathlib.HermitianMat.LiebConcavity

Main result for DPI

We derive the concavity of the trace functional `σ ↦ Tr[(σ^s H σ^s)^p]` from the Lieb–Ando trace inequalities proved in `LiebAndoTrace.lean`.

Density and continuity lemmas for PD/PSD extension

Helper lemmas for the core concavity proof

Core concavity on positive definite matrices

10 declarations

abbrev

Star-algebra isomorphism Matd(C)L(Cd)\text{Mat}_d(\mathbb{C}) \cong \mathcal{L}(\mathbb{C}^d)

Let dd be a natural number. Φ\Phi is the C\mathbb{C}-star-algebra isomorphism between the space of d×dd \times d complex matrices Matd(C)\text{Mat}_d(\mathbb{C}) and the space of continuous linear operators L(Cd)\mathcal{L}(\mathbb{C}^d) on dd-dimensional Euclidean space. This isomorphism identifies each matrix with its corresponding linear operator while preserving the addition, multiplication, scalar multiplication, and the star operation (Hermitian adjoint).

theorem

Φ\Phi is continuous

Let dd be a natural number. The star-algebra isomorphism Φ:Matd(C)L(Cd)\Phi : \text{Mat}_d(\mathbb{C}) \to \mathcal{L}(\mathbb{C}^d), which identifies a complex d×dd \times d matrix with its corresponding continuous linear operator on the dd-dimensional Euclidean space Cd\mathbb{C}^d, is a continuous function.

theorem

The image Φ(A)\Phi(A) of a Hermitian matrix AA is a self-adjoint operator

Let dd be a natural number. Let AA be a d×dd \times d Hermitian matrix over C\mathbb{C} and AmatA_{\text{mat}} be its underlying matrix representation. Let Φ:Matd(C)L(Cd)\Phi: \text{Mat}_d(\mathbb{C}) \cong \mathcal{L}(\mathbb{C}^d) be the star-algebra isomorphism that identifies a complex d×dd \times d matrix with its corresponding continuous linear operator on the dd-dimensional Euclidean space Cd\mathbb{C}^d. Then the linear operator Φ(Amat)\Phi(A_{\text{mat}}) is self-adjoint.

theorem

0A    0Φ(A)0 \le A \implies 0 \le \Phi(A) for Hermitian matrices AA

Let dd be a type and AA be a d×dd \times d complex Hermitian matrix. If AA is positive semidefinite (denoted as 0A0 \le A in the Loewner order), then the corresponding continuous linear operator Φ(A)\Phi(A) acting on the dd-dimensional Euclidean space Cd\mathbb{C}^d is also positive semidefinite (denoted as 0Φ(A)0 \le \Phi(A)).

theorem

Φ\Phi Maps Positive Definite Matrices to Positive Definite Operators

Let dd be a non-empty index set and Cd\mathbb{C}^d denote the corresponding dd-dimensional Euclidean space. Let AA be a d×dd \times d complex Hermitian matrix. If the underlying matrix of AA is positive definite (i.e., A0A \succ 0), then its image under the star-algebra isomorphism Φ\Phi is a strictly positive operator on Cd\mathbb{C}^d, belonging to the set of operators with a strictly positive spectrum (0,)(0, \infty).

theorem

Φ\Phi Commutes with Continuous Functional Calculus: Φ(f(A))=f(Φ(A))\Phi(f(A)) = f(\Phi(A))

Let AA be a d×dd \times d complex Hermitian matrix and f:RRf: \mathbb{R} \to \mathbb{R} be a function. Let Φ:Matd(C)L(Cd)\Phi: \text{Mat}_d(\mathbb{C}) \cong \mathcal{L}(\mathbb{C}^d) be the C\mathbb{C}-star-algebra isomorphism that identifies a complex matrix with its corresponding bounded linear operator on dd-dimensional Euclidean space. Then the continuous functional calculus commutes with Φ\Phi, such that Φ(f(A))=f(Φ(A)).\Phi(f(A)) = f(\Phi(A)).

theorem

Φ\Phi Commutes with Real Power ArA^r for A0A \ge 0

Let AA be a d×dd \times d complex Hermitian matrix such that AA is positive semidefinite (A0A \ge 0). For any real number rRr \in \mathbb{R}, let ArA^r denote the real power of AA defined via functional calculus. Let Φ:Matd(C)L(Cd)\Phi : \text{Mat}_d(\mathbb{C}) \cong \mathcal{L}(\mathbb{C}^d) be the star-algebra isomorphism identifying a complex matrix with its corresponding continuous linear operator on the dd-dimensional Euclidean space. Then the following identity holds: Φ(Ar)=(Φ(A))r\Phi(A^r) = (\Phi(A))^r

theorem

Tr(Φ(M))=tr(M)\text{Tr}(\Phi(M)) = \text{tr}(M)

For any complex d×dd \times d matrix MM, the trace of the linear operator Φ(M)\Phi(M) on the dd-dimensional Euclidean space Cd\mathbb{C}^d is equal to the matrix trace of MM, that is: Tr(Φ(M))=tr(M)\text{Tr}(\Phi(M)) = \text{tr}(M) where Φ:Matd(C)L(Cd)\Phi: \text{Mat}_d(\mathbb{C}) \to \mathcal{L}(\mathbb{C}^d) is the star-algebra isomorphism between the space of complex matrices and continuous linear operators.

theorem

Re(Tr(Φ(M)))=Re(Tr(M))\text{Re}(\text{Tr}(\Phi(M))) = \text{Re}(\text{Tr}(M))

Let MMatd(C)M \in \text{Mat}_d(\mathbb{C}) be a complex d×dd \times d matrix. Let Φ:Matd(C)L(Cd)\Phi : \text{Mat}_d(\mathbb{C}) \cong \mathcal{L}(\mathbb{C}^d) be the star-algebra isomorphism that identifies a matrix with its corresponding continuous linear operator on dd-dimensional Euclidean space. Then the real part of the trace of the operator Φ(M)\Phi(M) is equal to the real part of the trace of the matrix MM: Re(Tr(Φ(M)))=Re(Tr(M))\text{Re}(\text{Tr}(\Phi(M))) = \text{Re}(\text{Tr}(M))

theorem

Concavity of the trace functional σTr[(σα12αHσα12α)αα1]\sigma \mapsto \text{Tr} \left[ \left( \sigma^{\frac{\alpha - 1}{2\alpha}} H \sigma^{\frac{\alpha - 1}{2\alpha}} \right)^{\frac{\alpha}{\alpha - 1}} \right] for α>1\alpha > 1

Let HH be a d×dd \times d positive semidefinite Hermitian matrix over the complex numbers C\mathbb{C} (i.e., H0H \ge 0). For any real number α>1\alpha > 1, the function mapping a positive semidefinite Hermitian matrix σ\sigma to the trace functional σTr[(σα12αHσα12α)αα1]\sigma \mapsto \text{Tr} \left[ \left( \sigma^{\frac{\alpha - 1}{2\alpha}} H \sigma^{\frac{\alpha - 1}{2\alpha}} \right)^{\frac{\alpha}{\alpha - 1}} \right] is concave on the set of positive semidefinite matrices {σHermd(C)σ0}\{\sigma \in \text{Herm}_d(\mathbb{C}) \mid \sigma \ge 0\}.