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Quantum codes on a lattice with boundary

Mixed citation behavior. Most common role is background (67%).

48 Pith papers citing it
Background 67% of classified citations
abstract

A new type of local-check additive quantum code is presented. Qubits are associated with edges of a 2-dimensional lattice whereas the stabilizer operators correspond to the faces and the vertices. The boundary of the lattice consists of alternating pieces with two different types of boundary conditions. Logical operators are described in terms of relative homology groups.

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Vine Codes: Low-Overhead Quantum LDPC Codes on a Planar Square Grid

quant-ph · 2026-06-18 · unverdicted · novelty 8.0

Vine codes generalize directional codes to open planar boundaries, delivering up to 28% fewer data/measure qubits at circuit distance 7 and better simulated performance than the surface code at 10^{-3} noise while using fewer total qubits.

Holographically Emergent Gauge Theory in Symmetric Quantum Circuits

quant-ph · 2025-11-26 · unverdicted · novelty 8.0

Averaging symmetric Z_N quantum circuits over random noise produces a noisy surface code whose logical information is protected against symmetric errors up to a threshold, with charge-sharpening transitions coinciding with bulk confinement transitions that differ for N≤4 versus N>4.

Gauss law codes and vacuum codes from lattice gauge theories

quant-ph · 2026-04-07 · unverdicted · novelty 8.0

Gauss law codes identify the full gauge-invariant sector as the code space while vacuum codes restrict to the matter vacuum, with the two shown to be unitarily equivalent for finite gauge groups.

Quantum metrology via partial quantum error correction

quant-ph · 2026-05-08 · unverdicted · novelty 7.0 · 2 refs

Partial QEC on superpositions of code states suppresses parallel weight-l noise by p^floor((l+1)/2) while preserving super-SQL metrology performance using local operators and an adaptive imprinter strategy.

Non-linear Sigma Model for the Surface Code with Coherent Errors

cond-mat.stat-mech · 2026-03-26 · unverdicted · novelty 7.0

A non-linear sigma model maps surface-code decoding under coherent errors to distinct replica limits, exposing a thermal-metal phase for suboptimal decoders that is absent in optimal decoding.

The Structure of Circle Graph States

quant-ph · 2026-03-09 · unverdicted · novelty 7.0

Circle graphs are closed under r-local complementation and bipartite circle graph states correspond one-to-one with planar code states whose MBQC is classically simulable.

Higher Gauging and Non-invertible Condensation Defects

hep-th · 2022-04-05 · unverdicted · novelty 7.0

Higher gauging of 1-form symmetries on surfaces in 2+1d QFT yields condensation defects whose fusion rules involve 1+1d TQFTs and realizes every 0-form symmetry in TQFTs.

Magic state cultivation: growing T states as cheap as CNOT gates

quant-ph · 2024-09-26 · unverdicted · novelty 7.0

Magic state cultivation prepares high-fidelity T states with an order of magnitude fewer qubit-rounds than prior distillation methods by gradually growing them within a surface code under depolarizing noise.

Algebra of Bivariate-Bicycle Surface Codes

quant-ph · 2026-06-07 · unverdicted · novelty 6.0

BBS code dimension equals the algebraic multiplicity of finite nonzero common roots of the defining bivariate polynomials, enabling a root-based prescription for arbitrary boundary shapes that avoids corner corrections when edge conditions hold.

Barbell Codes: qLDPC Codes for Superconducting Quantum Hardware

quant-ph · 2026-06-04 · unverdicted · novelty 6.0

Barbell codes are a family of qLDPC codes with a matching superconducting chip layout enabling constant hardware complexity, simulated to preserve logical information over trillions of QEC cycles at 10^{-4} physical noise with under 30 data qubits per logical qubit.

Homomorphic Quantum Error Correction

quant-ph · 2026-05-25 · unverdicted · novelty 6.0

Establishes necessary and sufficient criterion for [[n,1,d]] stabilizer codes to preserve code space under restricted transversal block-Pauli masking U_enc(a,b)=(X^a Z^b)^⊗n for homomorphic quantum error correction.

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