Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Origami ISA Pulse Sequences: Optimal Control of the 731 Gate Set — DRAG as ISA Typing, Triality as Berry Phase, and the G₂ Circuit Depth of the SPIN Opcode

Ian Richard C Buckley

Published Jun 13, 2026• 0 citations
Publisher

Abstract

PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The Origami ISA opcodes are physical pulses: TWIST is a microwave rotation, SPLIT is an entangling gate, and the pentagon identity d² = 0 is a pulse-level constraint — violation means leakage. DRAG (Derivative Removal via Adiabatic Gate) is the ISA type checker that enforces this constraint, keeping TWIST within the correct representation subspace. ISA-augmented GRAPE reduces leakage by 63% vs standard GRAPE on a two-qudit transmon model (experiment x411a). The SPIN opcode implements triality — the order-3 outer automorphism of Spin(8) that cyclically permutes its three 8-dimensional irreps (8ᵥ, 8ₛ, 8꜀), with G₂ = Fix(triality). As a Fano-point permutation, SPIN costs exactly 12 CNOTs. Its phase component (i√7/2, not a root of unity) requires either O(log^c(1/ε)) Solovay-Kitaev approximation or a native G₂-symmetric Hamiltonian — the pulse-level expression of associamancy (experiment x411b). The Weyl group W(G₂) ≅ D₆ has order 12. All closed loops in G₂ parameter space give holonomies in this discrete group, giving topological protection unavailable to SU(2) holonomic gates (whose Berry phases are continuous). G₂ holonomic gates are exact under any continuous deformation that stays within one Weyl chamber (experiment x411c). Level-2 (associamancy) is the first resource level with topological protection built in. Keywords: origami ISA, pulse control, GRAPE, DRAG, triality, SPIN opcode, Berry phase, G₂, Weyl group, holonomic gates, transmon, trapped ion, 731 ISA, associamancy, optimal control

DOI
10.5281/zenodo.20680609

Related papers

The Origami ISA as a Typed Quantum DSL: Dependent Types, Linear Types, and the Schur Boundary as a Type Error

Ian Richard C Buckley

PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The Origami ISA — five opcodes (SPLIT, SPLAT, TWIST, FLIP, FLOP) corresponding to Pachner moves on a triangulated simplicial complex — is already a combinator library, but without a machine-checkable type system. This paper makes the type system explicit, yielding three progressively expressive type systems and one key theorem: associamancy is a compile-time type error. Type System 1 — Simple types. Wire types are irreducible representation labels Rep(G) for a gauge group G. For the Origami ISA: G = SU(2), types are spins j ∈ {0, ½, 1, …}. For the 731 ISA: G = G₂, types are Dynkin labels (p,q). For the financial Pacioli ISA: G = (ℝ₊, ×), types are currencies. The Pentagon identity d² = 0 becomes a typing rule: SPLAT(SPLIT(x)) must return the trivial representation 1. Any circuit producing a non-trivial output is ill-typed — this is the type-level expression of the leakage criterion introduced in Paper 411. Type System 2 — Linear types. Every wire is usable exactly once, encoding the quantum no-cloning theorem. SPLIT is the unique duplication primitive (1 → 4 wires, the Pachner move); FLOP is the unique elimination primitive (trace / Born rule). The category-theoretic model is a symmetric monoidal category extending the ZX-calculus to Rep(G)-typed wires over arbitrary compact groups G. Type System 3 — Dependent types. The output type of SPLIT depends on the input type via the Clebsch-Gordan decomposition: SPLIT_CG : (j : Rep(G)) → Σ(j₁ j₂ j₃ j₄ : Rep(G)). CG(j; j₁, j₂, j₃, j₄) ≠ 0 The fibred-category model (Grothendieck fibration over Rep(G)) captures this: the Schur boundary ν₂ ≠ 0 selects the associative subcategory (Origami ISA, regime 2) from the full category (731 ISA, regime 3). The Schur boundary as a TypeError. The Frobenius-Schur indicator ν₂ ∈ {−1, 0, +1} partitions wire types into two subtypes: AssocWire (ν₂ ≠ 0, Origami ISA) and FullWire (ν₂ = 0 allowed, 731 ISA). The SPIN opcode — the generator of triality, the order-3 outer automorphism of Spin(8) with G₂ = Fix(triality) — has type FullWire → FullWire with the constraint ν₂ = 0. Applying SPIN to an AssocWire raises a TypeError at circuit construction time, before any hardware is consulted. Associamancy (Paper 407) is no longer only a resource-theoretic concept — it is a compile-time type mismatch. The three-level resource hierarchy as a type tower: Level Resource Wire subtype Protection 0 Stabiliser Any Rep(SU(2)) None 1 Standard magic AssocWire (ν₂ ≠ 0) None 2 Associamancy FullWire (ν₂ = 0) Discrete Berry phase (W(G₂), order 12) The Pacioli Combinator Library as the financial instance. The PCL (Paper 306) — typed combinators flow, sequence, choose, fold — is the financial instance of this DSL with G = (ℝ₊, ×). The Pacioli identity (every debit has a credit) is d² = 0 at the financial instance. The same typed circuit compiles to quantum hardware, financial risk models, or nuclear spectroscopy; only the gauge group G and the wire type interpretation change. Python prototype included: ISACircuit class with runtime type checking; spin() raises TypeError if ν₂ ≠ 0; pentagon_check() validates d² = 0 at construction time. Keywords: Origami ISA, typed DSL, linear types, dependent types, Schur boundary, associamancy, no-cloning, Pentagon identity, Clebsch-Gordan, Pacioli combinator library, symmetric monoidal category, ZX-calculus, G₂, triality, type theory, quantum circuits

•Jun 13, 2026•0 citations

The Fano Plane is the Right Way to Think About Qubits: A Practitioner's Guide to the Origami ISA and Associamancy for Quantum Computing Researchers

Ian Richard C Buckley

PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. A practitioner's primer for quantum computing researchers. No knowledge of octonions, sheaf theory, or category theory is assumed. Knowledge of stabiliser states, the Clifford group, and T-gates is assumed. The central message: the structure of the 3-qubit Pauli group is secretly governed by the Fano plane PG(2,2), and the Fano plane is the geometry of the 731 instruction set architecture (731 ISA) — a unified framework for quantum computation that organises every opcode as a Pachner move on a simplicial complex. The framework reveals three levels of quantum computational resource:• Level 0 (Clifford): stabiliser states; Gottesman-Knill simulable; the Fano lines are the free sector.• Level 1 (Standard magic): T-gates; Wigner function negativity; non-Clifford but accessible to the Origami ISA (regime 2).• Level 2 (Associamancy): the SPIN opcode; the Schur boundary; genuinely complex irreps of PSL(2,7); not accessible to any associative hardware. The Origami ISA (five opcodes: SPLIT, SPLAT, TWIST, FLIP, FLOP) subsumes Bell sampling, qudit stabiliser learning, and the abelian hidden subgroup problem as special cases. The 731 ISA adds SPIN and BIND, unlocking Level 2. This primer is a companion to "The Topology of Risk" (doi:10.5281/zenodo.20642983), which covers the same H⁰/H¹/H² framework applied to financial risk. Keywords: quantum computing, Fano plane, Origami ISA, 731 ISA, stabiliser states, magic states, associamancy, Schur boundary, primer, tutorial, hidden subgroup problem, MBQC, photonics

•Jun 12, 2026•0 citations

The Opcode Rosetta Stone: A Universal ISA Dictionary for Exactly Solvable Quantum Models

Ian Richard C Buckley

PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The seven opcodes of the Origami instruction-set architecture (ISA) — FLOP, SPLIT, TWIST, LABEL, BIND, FLIP, SPLAT — play structurally identical roles across every exactly solvable quantum model with a phase transition. This paper establishes a universal dictionary: FLOP is always the fermionisation map (Jordan–Wigner / slave-boson / Majorana representation); SPLIT is always the diagonalisation (Bogoliubov / Bethe rapidity / stabiliser expansion); TWIST is always the gap check (Berry phase / Chern number / spectral gap); LABEL is always the sector projection (gauge fixing / stabiliser projection / Bethe vacuum). BIND — the three-body frog vertex — is the unique opcode whose presence or absence determines whether a phase supports Abelian or non-Abelian anyons. Two theorems are proved. The BIND = Non-Abelian theorem: a gapped topological phase has non-Abelian anyonic order if and only if its minimal ISA programme contains BIND. The Universal Phase Boundary theorem: for any model in the SU(2)q family at q = exp(iπβ), the quantum phase transition is a TWIST failure at β = 1/2, where the quantum dimension d{1/2}(β) = 2cos(πβ) = 0 exactly. A master table across twelve models — toric code, Kitaev honeycomb, TFIM, XXZ chain, string nets, quantum doubles, SYK, MBQC, ZX-calculus, and others — makes the dictionary explicit. The Origami ISA is the universal language in which condensed-matter physicists, quantum-information theorists, and representation theorists describe the same computation under different names. Keywords instruction set architecture, exactly solvable models, topological order, non-Abelian anyons, quantum phase transitions, Origami ISA, Jordan–Wigner transformation, Bogoliubov transformation, Bethe ansatz, toric code, Kitaev honeycomb, XXZ chain, string-net condensation, quantum doubles, SYK model, MBQC, ZX-calculus, Frobenius algebra, quantum groups, Berry phase, BIND theorem, β-ladder, tensor networks, categorical quantum mechanics

•Jun 19, 2026•0 citations

The Meld ISA: Complex-MGE, Quantum Algorithm Discovery, and the T-Gate as Octonion Obstruction

Ian Richard C Buckley

PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. We complete the TRS trilogy — Origami ($\beta\to\infty$, tropical, classical), Forge ($0<\beta<\infty$, real, statistical), Meld ($\beta=it$, complex, quantum) — by showing that the Meld ISA is the quantum circuit model expressed in the TRS semiring language. Three results follow. Result 1 (ISA completeness). The Clifford group equals the Meld ISA without the BIND opcode. Universal quantum computation equals Meld plus BIND. The T-gate $T = \mathrm{diag}(1,, e^{i\pi/4})$ is the BIND opcode at $j=\tfrac{1}{2}$ — the Fano associator obstruction of Paper 407, applied to qubit representations. The magic-typing classification of Papers 365/366 maps exactly onto the 731-ISA opcode hierarchy: Clifford gates occupy Fano-line orbits (SPLIT/FLIP/TWIST at Clifford angles); the T-gate occupies the non-collinear Fano triple (BIND). Result 2 (Quantum algorithm factory). Every classical algorithm of the form $\arg\max_{g\in G} f(g)$ over an abelian group $G$ has a $\mathbb{C}$-MGE quantum counterpart $\mathbb{C}\text{-MGE}(f) = \mathrm{SPLIT}_G \cdot \mathrm{FLIP}(f) \cdot \mathrm{SPLAT}$, giving exponential speedup via quantum Fourier sampling whenever $G$ is abelian and $f$ has a hidden subgroup concentrating Fourier mass. Shor's algorithm decomposes into three ISA layers: Layer 1 (Origami — classical modular exponentiation), Layer 2 (Meld — QFT as SPLIT-TWIST-FLIP cascade), Layer 3 (Origami — measurement as tropical projection). "Frozen-Shor" (Origami ISA, $\beta\to\infty$) recovers classical exhaustive search at cost $O(N)$. "Warm-Shor" (Forge ISA, real $\beta$) gives Grover-like $O(\sqrt{N})$ thermal concentration. Full Shor (Meld, $\beta=it$) achieves $O(\log N)$ via destructive interference — a resource unavailable in either real ISA. New algorithm candidates follow by identifying the symmetry group of the target problem: equivariant ML, quantum persistent homology (Lloyd-Garnerone-Zanardi 2016), and Boson Sampling (Aaronson-Arkhipov 2011) all fit the five-step factory template. Result 3 (ML-KEM structural no-go). ML-KEM (Module-LWE) is immune because LWE noise exponentially suppresses every Fourier component: $\mathbb{E}{\mathbf{e}\sim D\sigma}[e^{i\langle\xi,\mathbf{e}\rangle}] = e^{-|\xi|^2\sigma^2/2}$. No Fourier peak exists; SPLAT cannot extract a period. The deeper reason is that worst-case LWE reduces to the dihedral hidden subgroup problem (Regev 2002) — a non-abelian problem for which no efficient Meld program is known. Breaking ML-KEM would require a BIND opcode capable of distinguishing dihedral cosets, a capability not established for the current 731-Meld. The $H^k$ complexity ladder (Paper 420) is realised by the trilogy: $H^0$ (tree) = Origami, $H^1$ (loop) = Forge/BPP, $H^2$ (surface) = Meld/BQP. The T-gate is the $H^2$ generator that lifts computation off the stabiliser submanifold into the curved interior of the Fisher information metric. Series: Paper 258 (Origami ISA) → Paper 419 (Forge ISA) → Paper 443 ($\oplus_\beta$ semiring, six pairs) → Paper 453 (multi-sector Forge) → Paper 454 (this paper — Meld ISA, trilogy complete). Related identifiers (Cites) Paper 258 Origami ISA: doi:10.5281/zenodo.19916429 Paper 419 Forge ISA: doi:10.5281/zenodo.20694527 Paper 443 ⊕_β semiring: doi:10.5281/zenodo.20752384 Paper 407 Associamancy: doi:10.5281/zenodo.20702223 Paper 365 Fano Magic Factory: doi:10.5281/zenodo.20541583 Paper 366 CS Magic Composition: doi:10.5281/zenodo.20541665 Paper 445 Kitaev anyons: doi:10.5281/zenodo.20752352 Paper 453 Multi-sector Forge: doi:10.5281/zenodo.20773423 Paper 420 H^k complexity ladder: doi:10.5281/zenodo.20773526

•Jun 20, 2026•0 citations

The Origami ISA and the State Hidden Subgroup Problem: SPLAT as Fourier Sampling

Ian Richard C Buckley

PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. Hinsche, Eisert & Carrasco (PRX Quantum 7, 020337, 2026) introduced the abelian state hidden subgroup problem (StateHSP) and showed it is solved by quantum Fourier sampling via the character POVM Π_λ = (1/|G|) Σ_g χ̄_λ(g) R(g). We show this entire framework is an instance of the Origami ISA: the character POVM is the SPLAT opcode (fibre integration on the group algebra sheaf), and the full algorithm is the canonical SPLIT→SPLAT pipeline. Three corollaries: (1) Bell sampling is SPLAT on 2 copies with the SWAP representation over G=ℤ₂ⁿ. (2) Qudit stabiliser learning at d=3 is SPLAT on 3 copies, native to the TriQ register at depth O(1). (3) The StateHSP is H⁰ recovery — the hidden subgroup H is the zeroth sheaf cohomology H⁰(Γ_G, F_ψ) of the symmetry sheaf, and the O(log|G|/ε) sample complexity follows from H¹=0 (anticoncentration). The non-abelian extension — requiring the SPIN opcode and genuine complex irreps — is treated in the companion paper (doi:10.5281/zenodo.20667170). Keywords: quantum computing, hidden subgroup problem, Fourier sampling, SPLAT, Origami ISA, Bell sampling, stabiliser learning, sheaf cohomology, TriQ register, character POVM, abelian

•Jun 12, 2026•0 citations

The Forge ISA: A Temperature-Parameterised Instruction Set for Thermodynamic Computation

Ian Richard C Buckley

PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The Origami ISA executes algorithms as Pachner moves on simplicial complexes at inverse temperature β→∞ (the discrete, tropical limit). The Meld identifies the β→0 limit, where the same opcodes become the operators of smooth Hodge theory. The Forge ISA is the bridge: the same five opcodes (SPLIT, SPLAT, FLOP, FLIP, TWIST) running at finite inverse temperature β under a Gibbs distribution over H¹-weighted configurations. A Forge ISA programme at inverse temperature β is an Origami ISA programme on a sheaf ℱ over a simplicial complex X, where FLOP corrections are applied with probability proportional to the Gibbs weight exp(−β‖H¹(s)‖), and the Maslov–Gibbs Einsum (MGE) is the unique β-correct implementation. The critical temperature β*(ρ) = (3/8) ln(1/(1−ρ)), where ρ = β₁/|E| is the load factor (first Betti number divided by edge count), is the universal threshold separating the efficient (β < β*) from the stalled (β > β*) regime, empirically confirmed across eight algorithm classes. The Topological Resonance Synthesis (TRS) mandate (five purity conditions) ensures the Forge ISA is thermodynamically correct: β appears only in the Hamiltonian via the MGE; conformal, symplectic, and adiabatic structure are preserved throughout. Standard machine learning optimisers (Adam, dropout, batch normalisation) violate one or more of these conditions. The vorton is the elementary sampler — a single draw from the Gibbs distribution P_β on the state manifold — and the snap event is crystallisation at the harmonic representative of H¹. The Forge ISA is the engine of the TRS trilogy: the Origami ISA (cold reservoir, β→∞), the Forge ISA (the cycle, 0 < β < ∞), and the Meld (hot reservoir, β→0). Keywords instruction set architecture, thermodynamic computation, Gibbs distribution, inverse temperature, Origami ISA, The Meld, TRS trilogy, Maslov–Gibbs Einsum, MGE, simplicial complexes, sheaf theory, H¹ cohomology, Hodge theory, critical temperature, β-ladder, vorton, snap event, Carnot cycle, information geometry, topological resonance synthesis, differentiable programming, tropical geometry, adiabatic computation, Fisher metric

•Jun 15, 2026•0 citations
PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The Origami ISA opcodes are physical pulses: TWIST is a microwave rotation, SPLIT is an entangling gate, and the pentagon identity d² = 0 is a pulse-level constraint — violation means leakage. DRAG (Derivative Removal via Adiabatic Gate) is the ISA type checker that enforces this constraint, keeping TWIST within the correct representation subspace. ISA-augmented GRAPE reduces leakage by 63% vs standard GRAPE on a two-qudit transmon model (experiment x411a). The SPIN opcode implements triality — the order-3 outer automorphism of Spin(8) that cyclically permutes its three 8-dimensional irreps (8ᵥ, 8ₛ, 8꜀), with G₂ = Fix(triality). As a Fano-point permutation, SPIN costs exactly 12 CNOTs. Its phase component (i√7/2, not a root of unity) requires either O(log^c(1/ε)) Solovay-Kitaev approximation or a native G₂-symmetric Hamiltonian — the pulse-level expression of associamancy (experiment x411b). The Weyl group W(G₂) ≅ D₆ has order 12. All closed loops in G₂ parameter space give holonomies in this discrete group, giving topological protection unavailable to SU(2) holonomic gates (whose Berry phases are continuous). G₂ holonomic gates are exact under any continuous deformation that stays within one Weyl chamber (experiment x411c). Level-2 (associamancy) is the first resource level with topological protection built in. Keywords: origami ISA, pulse control, GRAPE, DRAG, triality, SPIN opcode, Berry phase, G₂, Weyl group, holonomic gates, transmon, trapped ion, 731 ISA, associamancy, optimal control
PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The Origami ISA — five opcodes (SPLIT, SPLAT, TWIST, FLIP, FLOP) corresponding to Pachner moves on a triangulated simplicial complex — is already a combinator library, but without a machine-checkable type system. This paper makes the type system explicit, yielding three progressively expressive type systems and one key theorem: associamancy is a compile-time type error. Type System 1 — Simple types. Wire types are irreducible representation labels Rep(G) for a gauge group G. For the Origami ISA: G = SU(2), types are spins j ∈ {0, ½, 1, …}. For the 731 ISA: G = G₂, types are Dynkin labels (p,q). For the financial Pacioli ISA: G = (ℝ₊, ×), types are currencies. The Pentagon identity d² = 0 becomes a typing rule: SPLAT(SPLIT(x)) must return the trivial representation 1. Any circuit producing a non-trivial output is ill-typed — this is the type-level expression of the leakage criterion introduced in Paper 411. Type System 2 — Linear types. Every wire is usable exactly once, encoding the quantum no-cloning theorem. SPLIT is the unique duplication primitive (1 → 4 wires, the Pachner move); FLOP is the unique elimination primitive (trace / Born rule). The category-theoretic model is a symmetric monoidal category extending the ZX-calculus to Rep(G)-typed wires over arbitrary compact groups G. Type System 3 — Dependent types. The output type of SPLIT depends on the input type via the Clebsch-Gordan decomposition: SPLIT_CG : (j : Rep(G)) → Σ(j₁ j₂ j₃ j₄ : Rep(G)). CG(j; j₁, j₂, j₃, j₄) ≠ 0 The fibred-category model (Grothendieck fibration over Rep(G)) captures this: the Schur boundary ν₂ ≠ 0 selects the associative subcategory (Origami ISA, regime 2) from the full category (731 ISA, regime 3). The Schur boundary as a TypeError. The Frobenius-Schur indicator ν₂ ∈ {−1, 0, +1} partitions wire types into two subtypes: AssocWire (ν₂ ≠ 0, Origami ISA) and FullWire (ν₂ = 0 allowed, 731 ISA). The SPIN opcode — the generator of triality, the order-3 outer automorphism of Spin(8) with G₂ = Fix(triality) — has type FullWire → FullWire with the constraint ν₂ = 0. Applying SPIN to an AssocWire raises a TypeError at circuit construction time, before any hardware is consulted. Associamancy (Paper 407) is no longer only a resource-theoretic concept — it is a compile-time type mismatch. The three-level resource hierarchy as a type tower: Level Resource Wire subtype Protection 0 Stabiliser Any Rep(SU(2)) None 1 Standard magic AssocWire (ν₂ ≠ 0) None 2 Associamancy FullWire (ν₂ = 0) Discrete Berry phase (W(G₂), order 12) The Pacioli Combinator Library as the financial instance. The PCL (Paper 306) — typed combinators flow, sequence, choose, fold — is the financial instance of this DSL with G = (ℝ₊, ×). The Pacioli identity (every debit has a credit) is d² = 0 at the financial instance. The same typed circuit compiles to quantum hardware, financial risk models, or nuclear spectroscopy; only the gauge group G and the wire type interpretation change. Python prototype included: ISACircuit class with runtime type checking; spin() raises TypeError if ν₂ ≠ 0; pentagon_check() validates d² = 0 at construction time. Keywords: Origami ISA, typed DSL, linear types, dependent types, Schur boundary, associamancy, no-cloning, Pentagon identity, Clebsch-Gordan, Pacioli combinator library, symmetric monoidal category, ZX-calculus, G₂, triality, type theory, quantum circuits
PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. A practitioner's primer for quantum computing researchers. No knowledge of octonions, sheaf theory, or category theory is assumed. Knowledge of stabiliser states, the Clifford group, and T-gates is assumed. The central message: the structure of the 3-qubit Pauli group is secretly governed by the Fano plane PG(2,2), and the Fano plane is the geometry of the 731 instruction set architecture (731 ISA) — a unified framework for quantum computation that organises every opcode as a Pachner move on a simplicial complex. The framework reveals three levels of quantum computational resource:• Level 0 (Clifford): stabiliser states; Gottesman-Knill simulable; the Fano lines are the free sector.• Level 1 (Standard magic): T-gates; Wigner function negativity; non-Clifford but accessible to the Origami ISA (regime 2).• Level 2 (Associamancy): the SPIN opcode; the Schur boundary; genuinely complex irreps of PSL(2,7); not accessible to any associative hardware. The Origami ISA (five opcodes: SPLIT, SPLAT, TWIST, FLIP, FLOP) subsumes Bell sampling, qudit stabiliser learning, and the abelian hidden subgroup problem as special cases. The 731 ISA adds SPIN and BIND, unlocking Level 2. This primer is a companion to "The Topology of Risk" (doi:10.5281/zenodo.20642983), which covers the same H⁰/H¹/H² framework applied to financial risk. Keywords: quantum computing, Fano plane, Origami ISA, 731 ISA, stabiliser states, magic states, associamancy, Schur boundary, primer, tutorial, hidden subgroup problem, MBQC, photonics
PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The seven opcodes of the Origami instruction-set architecture (ISA) — FLOP, SPLIT, TWIST, LABEL, BIND, FLIP, SPLAT — play structurally identical roles across every exactly solvable quantum model with a phase transition. This paper establishes a universal dictionary: FLOP is always the fermionisation map (Jordan–Wigner / slave-boson / Majorana representation); SPLIT is always the diagonalisation (Bogoliubov / Bethe rapidity / stabiliser expansion); TWIST is always the gap check (Berry phase / Chern number / spectral gap); LABEL is always the sector projection (gauge fixing / stabiliser projection / Bethe vacuum). BIND — the three-body frog vertex — is the unique opcode whose presence or absence determines whether a phase supports Abelian or non-Abelian anyons. Two theorems are proved. The BIND = Non-Abelian theorem: a gapped topological phase has non-Abelian anyonic order if and only if its minimal ISA programme contains BIND. The Universal Phase Boundary theorem: for any model in the SU(2)q family at q = exp(iπβ), the quantum phase transition is a TWIST failure at β = 1/2, where the quantum dimension d{1/2}(β) = 2cos(πβ) = 0 exactly. A master table across twelve models — toric code, Kitaev honeycomb, TFIM, XXZ chain, string nets, quantum doubles, SYK, MBQC, ZX-calculus, and others — makes the dictionary explicit. The Origami ISA is the universal language in which condensed-matter physicists, quantum-information theorists, and representation theorists describe the same computation under different names. Keywords instruction set architecture, exactly solvable models, topological order, non-Abelian anyons, quantum phase transitions, Origami ISA, Jordan–Wigner transformation, Bogoliubov transformation, Bethe ansatz, toric code, Kitaev honeycomb, XXZ chain, string-net condensation, quantum doubles, SYK model, MBQC, ZX-calculus, Frobenius algebra, quantum groups, Berry phase, BIND theorem, β-ladder, tensor networks, categorical quantum mechanics
PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. We complete the TRS trilogy — Origami (β→∞\beta\to\inftyβ→∞, tropical, classical), Forge (0<β<∞0<\beta<\infty0<β<∞, real, statistical), Meld (β=it\beta=itβ=it, complex, quantum) — by showing that the Meld ISA is the quantum circuit model expressed in the TRS semiring language. Three results follow. Result 1 (ISA completeness). The Clifford group equals the Meld ISA without the BIND opcode. Universal quantum computation equals Meld plus BIND. The T-gate T=diag(1,,eiπ/4)T = \mathrm{diag}(1,, e^{i\pi/4})T=diag(1,,eiπ/4) is the BIND opcode at j=12j=\tfrac{1}{2}j=21​ — the Fano associator obstruction of Paper 407, applied to qubit representations. The magic-typing classification of Papers 365/366 maps exactly onto the 731-ISA opcode hierarchy: Clifford gates occupy Fano-line orbits (SPLIT/FLIP/TWIST at Clifford angles); the T-gate occupies the non-collinear Fano triple (BIND). Result 2 (Quantum algorithm factory). Every classical algorithm of the form arg⁡max⁡g∈Gf(g)\arg\max_{g\in G} f(g)argmaxg∈G​f(g) over an abelian group GGG has a C\mathbb{C}C-MGE quantum counterpart C-MGE(f)=SPLITG⋅FLIP(f)⋅SPLAT\mathbb{C}\text{-MGE}(f) = \mathrm{SPLIT}_G \cdot \mathrm{FLIP}(f) \cdot \mathrm{SPLAT}C-MGE(f)=SPLITG​⋅FLIP(f)⋅SPLAT, giving exponential speedup via quantum Fourier sampling whenever GGG is abelian and fff has a hidden subgroup concentrating Fourier mass. Shor's algorithm decomposes into three ISA layers: Layer 1 (Origami — classical modular exponentiation), Layer 2 (Meld — QFT as SPLIT-TWIST-FLIP cascade), Layer 3 (Origami — measurement as tropical projection). "Frozen-Shor" (Origami ISA, β→∞\beta\to\inftyβ→∞) recovers classical exhaustive search at cost O(N)O(N)O(N). "Warm-Shor" (Forge ISA, real β\betaβ) gives Grover-like O(N)O(\sqrt{N})O(N​) thermal concentration. Full Shor (Meld, β=it\beta=itβ=it) achieves O(log⁡N)O(\log N)O(logN) via destructive interference — a resource unavailable in either real ISA. New algorithm candidates follow by identifying the symmetry group of the target problem: equivariant ML, quantum persistent homology (Lloyd-Garnerone-Zanardi 2016), and Boson Sampling (Aaronson-Arkhipov 2011) all fit the five-step factory template. Result 3 (ML-KEM structural no-go). ML-KEM (Module-LWE) is immune because LWE noise exponentially suppresses every Fourier component: Ee∼Dσ[ei⟨ξ,e⟩]=e−∣ξ∣2σ2/2\mathbb{E}{\mathbf{e}\sim D\sigma}[e^{i\langle\xi,\mathbf{e}\rangle}] = e^{-|\xi|^2\sigma^2/2}Ee∼Dσ[ei⟨ξ,e⟩]=e−∣ξ∣2σ2/2. No Fourier peak exists; SPLAT cannot extract a period. The deeper reason is that worst-case LWE reduces to the dihedral hidden subgroup problem (Regev 2002) — a non-abelian problem for which no efficient Meld program is known. Breaking ML-KEM would require a BIND opcode capable of distinguishing dihedral cosets, a capability not established for the current 731-Meld. The HkH^kHk complexity ladder (Paper 420) is realised by the trilogy: H0H^0H0 (tree) = Origami, H1H^1H1 (loop) = Forge/BPP, H2H^2H2 (surface) = Meld/BQP. The T-gate is the H2H^2H2 generator that lifts computation off the stabiliser submanifold into the curved interior of the Fisher information metric. Series: Paper 258 (Origami ISA) → Paper 419 (Forge ISA) → Paper 443 (⊕β\oplus_\beta⊕β​ semiring, six pairs) → Paper 453 (multi-sector Forge) → Paper 454 (this paper — Meld ISA, trilogy complete). Related identifiers (Cites) Paper 258 Origami ISA: doi:10.5281/zenodo.19916429 Paper 419 Forge ISA: doi:10.5281/zenodo.20694527 Paper 443 ⊕_β semiring: doi:10.5281/zenodo.20752384 Paper 407 Associamancy: doi:10.5281/zenodo.20702223 Paper 365 Fano Magic Factory: doi:10.5281/zenodo.20541583 Paper 366 CS Magic Composition: doi:10.5281/zenodo.20541665 Paper 445 Kitaev anyons: doi:10.5281/zenodo.20752352 Paper 453 Multi-sector Forge: doi:10.5281/zenodo.20773423 Paper 420 H^k complexity ladder: doi:10.5281/zenodo.20773526
PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. Hinsche, Eisert & Carrasco (PRX Quantum 7, 020337, 2026) introduced the abelian state hidden subgroup problem (StateHSP) and showed it is solved by quantum Fourier sampling via the character POVM Π_λ = (1/|G|) Σ_g χ̄_λ(g) R(g). We show this entire framework is an instance of the Origami ISA: the character POVM is the SPLAT opcode (fibre integration on the group algebra sheaf), and the full algorithm is the canonical SPLIT→SPLAT pipeline. Three corollaries: (1) Bell sampling is SPLAT on 2 copies with the SWAP representation over G=ℤ₂ⁿ. (2) Qudit stabiliser learning at d=3 is SPLAT on 3 copies, native to the TriQ register at depth O(1). (3) The StateHSP is H⁰ recovery — the hidden subgroup H is the zeroth sheaf cohomology H⁰(Γ_G, F_ψ) of the symmetry sheaf, and the O(log|G|/ε) sample complexity follows from H¹=0 (anticoncentration). The non-abelian extension — requiring the SPIN opcode and genuine complex irreps — is treated in the companion paper (doi:10.5281/zenodo.20667170). Keywords: quantum computing, hidden subgroup problem, Fourier sampling, SPLAT, Origami ISA, Bell sampling, stabiliser learning, sheaf cohomology, TriQ register, character POVM, abelian
PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The Origami ISA executes algorithms as Pachner moves on simplicial complexes at inverse temperature β→∞ (the discrete, tropical limit). The Meld identifies the β→0 limit, where the same opcodes become the operators of smooth Hodge theory. The Forge ISA is the bridge: the same five opcodes (SPLIT, SPLAT, FLOP, FLIP, TWIST) running at finite inverse temperature β under a Gibbs distribution over H¹-weighted configurations. A Forge ISA programme at inverse temperature β is an Origami ISA programme on a sheaf ℱ over a simplicial complex X, where FLOP corrections are applied with probability proportional to the Gibbs weight exp(−β‖H¹(s)‖), and the Maslov–Gibbs Einsum (MGE) is the unique β-correct implementation. The critical temperature β*(ρ) = (3/8) ln(1/(1−ρ)), where ρ = β₁/|E| is the load factor (first Betti number divided by edge count), is the universal threshold separating the efficient (β < β*) from the stalled (β > β*) regime, empirically confirmed across eight algorithm classes. The Topological Resonance Synthesis (TRS) mandate (five purity conditions) ensures the Forge ISA is thermodynamically correct: β appears only in the Hamiltonian via the MGE; conformal, symplectic, and adiabatic structure are preserved throughout. Standard machine learning optimisers (Adam, dropout, batch normalisation) violate one or more of these conditions. The vorton is the elementary sampler — a single draw from the Gibbs distribution P_β on the state manifold — and the snap event is crystallisation at the harmonic representative of H¹. The Forge ISA is the engine of the TRS trilogy: the Origami ISA (cold reservoir, β→∞), the Forge ISA (the cycle, 0 < β < ∞), and the Meld (hot reservoir, β→0). Keywords instruction set architecture, thermodynamic computation, Gibbs distribution, inverse temperature, Origami ISA, The Meld, TRS trilogy, Maslov–Gibbs Einsum, MGE, simplicial complexes, sheaf theory, H¹ cohomology, Hodge theory, critical temperature, β-ladder, vorton, snap event, Carnot cycle, information geometry, topological resonance synthesis, differentiable programming, tropical geometry, adiabatic computation, Fisher metric