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InfOCF Solver: Quantum Conic Optimization

Updated 14 January 2026
  • InfOCF solver is an interior‐point method for quantum-information conic programs, leveraging quantum relative entropy and noncommutative operator perspectives.
  • It employs a modular Python architecture with specialized barrier oracles and homogeneous self-dual embedding to ensure rapid convergence.
  • The solver achieves high precision in handling both symmetric and nonsymmetric cones, integrating seamlessly with Python modeling tools like PICOS.

The InfOCF solver is an interior-point method specialized for quantum-information-theoretic conic programs, notably those involving quantum relative entropy (QRE) and noncommutative perspectives of operator convex functions. Implemented within the QICS (Quantum Information Conic Solver) package, InfOCF provides a modular, high-precision open-source tool for tackling both symmetric (e.g., semidefinite programs) and non-symmetric conic optimization problems central to quantum information theory (He et al., 2024).

1. Mathematical Structure of Conic Programs

The core computational object is a Cartesian product cone K\mathcal{K} comprised of:

  • The positive semidefinite cone (H+)(\mathbb{H}_+),
  • Quantum relative-entropy cones,
  • Cones defined by noncommutative operator perspectives.

For Hermitian matrices of size nn, Hn={XCn×n:X=X}\mathbb{H}^n = \{X \in \mathbb{C}^{n\times n} : X^\dagger = X\} and H++n={X0}\mathbb{H}^n_{++} = \{X \succ 0\}. The QRE cone is

KQREn={(t,X,Y)R×H++n×H++n:tTr[X(logXlogY)]}.\mathcal{K}_{\mathrm{QRE}}^n = \left\{ (t, X, Y) \in \mathbb{R} \times \mathbb{H}^n_{++} \times \mathbb{H}^n_{++}: t \geq \mathrm{Tr}[X(\log X - \log Y)] \right\}.

The barrier function is

FQRE(t,X,Y)=log(tTr[X(logXlogY)])logdetXlogdetY,F_{\mathrm{QRE}}(t, X, Y) = -\log(t - \mathrm{Tr}[X(\log X - \log Y)]) - \log\det X - \log\det Y,

and is self-concordant with complexity parameter ν=1+2n\nu = 1 + 2n. More generally, for operator-convex ff, the noncommutative perspective Pf(X,Y)=Y1/2f(Y1/2XY1/2)Y1/2P_f(X, Y) = Y^{1/2} f(Y^{-1/2} X Y^{-1/2}) Y^{1/2} defines analogous cones and barriers (He et al., 2024).

2. Primal–Dual and Homogeneous Self-Dual Embedding

The solver targets problems of the form

minxc,xs.t.Ax=b,xK\min_x \langle c, x \rangle \quad \mathrm{s.t.}\quad A x = b, \quad x \in \mathcal{K}

with dual

maxy,zb,ys.t.ATy+z=c,zK.\max_{y, z} -\langle b, y\rangle\quad \mathrm{s.t.}\quad A^T y + z = c,\, z \in \mathcal{K}^*.

The homogeneous self-dual embedding introduces variables (x,y,z,s,τ,κ)(x, y, z, s, \tau, \kappa) and linear embedding equations L(ω)=0L(\omega) = 0 coupling primal and dual feasibility and strict conic interiority. Central-path conditions enforce z+μF(s)=0z + \mu \nabla F(s) = 0, τκ=μ\tau\kappa = \mu for a scaling parameter μ>0\mu >0, leading as μ0\mu\to 0 to optimality or certificate of infeasibility (He et al., 2024).

3. Cone Barrier Oracles

Each cone block in K\mathcal{K} must implement oracles supporting:

  • Membership tests (including interior checks),
  • Evaluation of the barrier gradient F\nabla F and Hessian 2F\nabla^2 F,
  • Hessian–vector and (optionally) inverse Hessian–vector products.

For the QRE cone, F(t,X,Y)F(t,X,Y) as above has

tF=1z,DXF=1z(logXlogY+I)X1\nabla_t F = -\frac{1}{z},\qquad \mathsf{D}_X F = \frac{1}{z}(\log X - \log Y + I) - X^{-1}

with z=tTr[X(logXlogY)]z = t - \mathrm{Tr}[X(\log X - \log Y)]. DYF\mathsf{D}_Y F and the Hessian are implemented via equivariant spectral calculus and divided differences. For noncommutative perspectives, differentiation exploits spectral mapping and blockwise Hessians of dimension $2n$ (He et al., 2024).

4. Interior-Point Algorithm and Complexity

A Newton system (linearization of the KKT/central-path conditions) is solved at each IPM iteration. This typically reduces to a Schur complement system in the dual variables: SΔy=r^,S=A(GTHG)1ATS \Delta y = \hat{r},\qquad S = A (G^T H G)^{-1} A^T where HH is a block-diagonal barrier Hessian. Per-iteration complexity is dominated by forming/factoring the Schur complement, O(m3)O(m^3) for mm equality constraints. The overall iteration complexity is

O(νlog1ϵ)O\left(\sqrt{\nu}\,\log\frac{1}{\epsilon}\right)

with total barrier parameter ν\nu and target accuracy ϵ\epsilon. Sparsity and Hermitian structure are exploited to accelerate large-scale instances (He et al., 2024).

5. Software Architecture and Implementation

The Python implementation is modular: a Model class encapsulates coefficients, constraints, and cones; the Solver class manages initialization, iteration, and step selection. Each cone block is a Python module with barrier([x](https://www.emergentmind.com/topics/stability-index-x)), grad(x), hess(x,v), and, where needed, hess_inv(x,v) interfaces. Linear algebra uses NumPy for dense, SciPy for sparse ops, and Numba for JIT-accelerated spectral routines. PSD cones leverage the Fujisawa–Kojima–Nakata approach for sparse AH1ATA H^{-1} A^T assembly. Hermitian variables are stored in real-valued or complex format, vectorized internally (He et al., 2024).

QICS integrates with PICOS, a general Python modeling language. Users can construct quantum-entropy-constrained problems in PICOS and solve them via QICS:

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import picos
P = picos.Problem()
X = picos.SymmetricVariable('X', n)
Y = picos.SymmetricVariable('Y', n)
P.set_objective('min', picos.quantrelentr(X, Y))
P.add_constraint(picos.maindiag(X) == 1)
P.solve(solver='qics')
This allows seamless model definition and invocation of the InfOCF solver as a backend.

6. Illustrative Use Case and Performance

A canonical example is the 2×22 \times 2 QRE-closeness problem: minYS2  S((21 12)Y)s.t.  Y11=Y22=1,Y0.\min_{Y \in \mathbb{S}^2}\;S_\parallel\Bigl( \begin{pmatrix}2 & 1 \ 1 & 2\end{pmatrix} \,\|\, Y \Bigr) \quad \text{s.t.}\; Y_{11} = Y_{22} = 1,\, Y \succeq 0. Modeling and solving this within QICS proceeds via the outlined Python API, using the QRE cone. On this task, InfOCF converges in 7 iterations (barrier parameter=5), reporting primal and dual objective values agreeing to at least $5$ significant digits and reporting an optimal YY with off-diagonal $0.5$. This demonstrates the solver's precision and the suitability of its barrier oracles for nonsymmetric cones (He et al., 2024).

7. Applications, Scope, and Extensions

The InfOCF solver enables high-accuracy solutions of structured conic programs arising in quantum information theory, e.g.,

  • Semidefinite programming (SDP) with quantum-entropy constraints,
  • Optimization involving noncommutative perspectives,
  • Problems requiring exact handling of the quantum relative entropy.

Its design permits extension to novel cones with operator-convex function barriers, and it is architected for efficient sparse instances and large-scale Hermitian matrix variables. Integration with Python modeling frameworks encourages broader adoption in quantum information, mathematical optimization, and operator algebra applications (He et al., 2024).

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