Abstract Stabilizer convolution channels in odd-prime dimensions have a natural description in finite-field phase space. We analyze these channels using Clifford symmetry and show that, for a fixed environmental state, the maximal single-letter coherent information is unchanged under Clifford-equivalent choices of the stabilizer convolution matrix. This reduces the apparently quadratic family of admissible stabilizer convolutions, at the one-use level, to sign-orbit classes of a single finite-field parameter. We also isolate quadratic cases in which the induced Clifford symmetry becomes either the identity or phase-space inversion; these cases give symmetry-protected families with zero maximal single-letter coherent information. To complement this symmetry analysis, we introduce a minimal weighted magic entropy and prove that it sharpens the magic-relative-entropy upper bound for positive convolution channels at the single-letter level. Finally, we define the single-letter coherent-information power of a convolution and show that the optimizing environmental state may be taken to be pure. Small-dimensional numerical examples illustrate the sign-orbit classification and show that coherent-information enhancement is governed by the finite-field convolution parameter rather than by dimension alone.
Abstract Stabilizer convolution channels in odd-prime dimensions have a natural description in finite-field phase space. We analyze these channels using Clifford symmetry and show that, for a fixed environmental state, the maximal single-letter coherent information is unchanged under Clifford-equivalent choices of the stabilizer convolution matrix. This reduces the apparently quadratic family of admissible stabilizer convolutions, at the one-use level, to sign-orbit classes of a single finite-field parameter. We also isolate quadratic cases in which the induced Clifford symmetry becomes either the identity or phase-space inversion; these cases give symmetry-protected families with zero maximal single-letter coherent information. To complement this symmetry analysis, we introduce a minimal weighted magic entropy and prove that it sharpens the magic-relative-entropy upper bound for positive convolution channels at the single-letter level. Finally, we define the single-letter coherent-information power of a convolution and show that the optimizing environmental state may be taken to be pure. Small-dimensional numerical examples illustrate the sign-orbit classification and show that coherent-information enhancement is governed by the finite-field convolution parameter rather than by dimension alone.
We study how Clifford interactions with a fixed environment determine quantum transmission, in a setting that extends positive discrete quantum convolution . We characterize when Clifford operations on the environment can be replaced by operations on the signal input and the two outputs, and classify the interactions under local Clifford transformations . For pure stabilizer environments, we determine the noiseless, dephasing, and completely depolarizing parts of the channel directly from the interaction and environmental stabilizers, obtaining its quantum and private capacities . This reveals a distinction between interactions: those locally equivalent to positive convolution produce entanglement-breaking channels for every pure stabilizer environment, whereas every other interaction in the class admits noiseless quantum transmission with a suitable pure stabilizer environment . For positive convolution, environmental Clifford transport also allows us to separate the stabilized coordinates of an arbitrary mixed environment . These coordinates carry only a classical label shared by the receiver and environment, so removing them preserves quantum and private capacities . The resulting channel reduction yields a private-capacity bound by the modified relative entropy of magic of the environmental state .
Quantum convolution provides a discrete-variable analogue of classical convolution, with the mean state capturing the stabilizer structure preserved under repeated convolution. We establish a finite-step entropy hierarchy generated by compatible stabilizer dephasings. Along every compatible isotropic flag, the entropy increases toward the mean-state entropy ceiling, while the relative-entropy distance to the mean state decomposes exactly into successive coherence losses and a terminal classical nonuniformity. Optimizing over compatible subspaces yields an intrinsic entropy profile of the state. For quantum convolutional channels, Weyl covariance reduces the one-shot classical communication problem to minimal output entropy. A spectral-transfer argument shows that suitable stabilizer inputs reproduce stabilizer-measurement distributions of the environment as channel-output spectra. This gives a computable Holevo lower bound over all complete stabilizer measurements; its compatible restriction is characterized by the entropy hierarchy and refines the previous mean-state bound of Bu, Gu, and Jaffe. The bound is exact for stabilizer-diagonal environments, for which the Holevo capacity is strongly additive, and yields a single-letter formula for a nonstabilizer qutrit family. The same family also exhibits a coexistence region with simultaneously positive classical and quantum communication rates
In this paper, we focus on discrete-variable quantum systems of odd prime dimension. We investigate the quantum capacity of stabilizer convolution channels under a variety of environmental states. Inspired by the recent result of Bu and Jaffe [Phys. Rev. Lett. 134, 050202 (2025)], our main contribution is to generalize the analysis beyond the discrete beam splitter---which is only applicable for odd prime dimensions $d\ensuremath{\ge}7$---to broader classes of stabilizer convolutions, allowing us to explore the behavior of magic resources in lower dimensions such as d=3 and d=5, where their role in enhancing quantum capacity has remained unclear. In fact, many of our mathematical results are derived under the broader setting of positive convolutions, not limited strictly to stabilizer convolutions.
Monitored quantum circuits combine scrambling with measurement-conditioned state updates, while non-Clifford perturbations inject magic into otherwise stabilizer-compatible dynamics. Rigorous results on stationary magic and its weak-injection asymptotics remain limited even for finite-dimensional Clifford-based monitored models.
We study an N-qudit process of prime local dimension d. Each cycle draws a fresh uniform global Clifford unitary, applies a local weak non-Clifford rotation and a projective measurement on one qudit, and then returns to the inverse Clifford frame. For every fixed injection strength, we prove that the induced pure-state Markov chain has a unique invariant probability measure and attracts every initial law geometrically in Wasserstein distance. At zero injection, the invariant law is supported on the finite stabilizer layer. After rescaling transverse deviations from this layer, the resulting blown-up stationary laws converge weakly to the invariant law of an affine tangent recursion. Combining this tangent law with Poisson representations and the first nonzero local resource germs determines the sharp vanishing rates of stationary magic. For every fixed N≥2, odd-prime Gross--Wigner mana admits a linear expansion with a strictly positive coefficient, whereas qubit 2-stabilizer Rényi entropy admits a quadratic expansion with a strictly positive coefficient. For N=1, both stationary resource averages vanish identically for all injection strengths. The distinct orders arise from the different local resource geometries, together with quadratic-order zero-reference branch contributions in qubit case.
Magic states enable universal, fault-tolerant quantum computation within the stabilizer framework. Their non-stabilizerness supplies the resource needed to bypass the Eastin-Knill theorem while allowing fault-tolerant distillation. Although many measures of magic exist, not every nonzero-magic state is known to be distillable, and many of currently known distillable states are special cases of Clifford-stabilizer states, defined as pure states uniquely stabilized by finite Clifford subgroups. We develop a general framework for group-covariant functionals on Hermitian operators, introducing the notions of G-stabilizer spaces, states, and codes for arbitrary finite subgroups G⊂U(H). We define analytic families of G-covariant functionals and prove that any G-invariant pure state is extremal for a broad class of derived functionals, including symmetric, max-type, and Rényi-type functionals, whenever the underlying family is G-covariant. This extremality holds for purity-preserving variations orthogonal to the stabilized subspace. Specializing to the Pauli and Clifford groups, we recover the extremality structure of canonical magic measures such as mana, stabilizer Rényi entropies, generalized Rényi entropies, and stabilizer fidelity, and show that Clifford-stabilizer states extremize them. We classify such states for qubits, qutrits, ququints, and two-qubit systems, identifying new candidates for magic distillation. We further propose an inefficient distillation protocol for a two-qubit magic state with stabilizer fidelity exceeding standard benchmarks, and conjecture that SIC-POVM fiducial states are Clifford-stabilizer states.
Magic -- the resource enabling quantum computational advantage beyond stabilizer circuits -- has a clean phase-space characterization in odd prime dimensions that qubits notoriously lack. We study C(rho), the l_1 distance from a state's discrete Wigner function to the stabilizer polytope, and determine its exact geometry. For a single qubit with Bloch vector r we prove the closed form C = max(0, ||r||_1 - 1)/2, so the maximum is (sqrt(3)-1)/2, attained at the eight face states. For products of single-qubit states, C(rho_1 x ... x rho_n) <= prod_i (1 + C(rho_i)) - 1, with equality whenever every factor has Bloch sign product r_x r_y r_z <= 0; this includes the exact tensor powers ((1+sqrt(3))/2)^n - 1 and the exact maximum of C over fully separable n-qubit states.
Because no discrete Wigner function for qubits is Clifford covariant, any such measure is frame dependent, and we identify which of its features are not. For a single qubit there are exactly two valid frames up to phase-space translation and C is identical on both. Pauli-covariant two-qubit frames number 2048 up to translation, and across them the ratio C(rho_Rx)/C(rho_Ry) takes the values 1/2, 1 and 2. In every one of these frames some stabilizer state has negative Wigner entries, a consequence of the Mermin-Peres square, so the two-qubit bound Gamma >= 1 + C/2 against the robustness of magic Gamma is frame independent.
Within the Wootters frame we prove integer values 1, 2, 1 of the tightness ratio kappa := (Gamma-1)/C for three families in the two-qubit repetition codespace, with explicit certificates. For n-qubit GHZ phase states we prove Gamma = |sin phi| + |cos phi| for all n and C >= 2^(floor(n/2)-1) (|sin phi| + |cos phi| - 1), tight for n = 2 and, by exact linear programming, for n = 3, 4, so kappa decays exponentially. Finally, C is not a magic monotone, so it cannot replace Gamma in distillation bounds.