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Definitions for Renormalization algorithm with graph enhancement

Definition
QAlgorithms_Papers_Independent_Intakethird100_P57

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

The objects the formalized statements of Renormalization algorithm with graph enhancement (arXiv:0802.1211) are stated in. Each was checked against the paper by a blind read-back and a moderator.

  • Tensors: Eq.(1), PDF pp.1–2: two arbitrary complex D-by-D site matrices.
  • traceMPS: Eq.(1), PDF p.1: the periodic trace MPS, with matrices multiplied in chain order.
  • PhaseGraph: PDF p.2: symmetric, zero-diagonal graph weights in [0,2π).
  • emptyPhaseGraph: The absent graph (PDF p.2, following Eq.(2)).
  • productOp: PDF p.2: tensor product of local matrices, on arbitrary finite sets of wires.
  • graphAngle: PDF p.2: each unordered edge acts once, with the positive controlled phase.
  • graphOp: PDF p.2: diagonal product of all controlled-phase gates.
  • enhance: Eq.(2), PDF p.2: graph enhancement followed by the local rotations.
  • rage: Eq.(2), PDF p.2: the RAGE raw vector.
  • normalizeRageVector: PDF pp.2–4: normalize a raw nonzero vector before physical uses. At zero this total helper is zero; all physical theorems exclude that input.
  • productVec: PDF p.2, Eq.(3), second line: an arbitrary product vector.
  • plusFactors: PDF p.2: normalized plus factors.
  • productTensors: PDF p.2: bond-one matrices for product vectors.
  • diagonalTensors: Eq.(3), second line, PDF p.2: diagonal tensors for a finite sum of products. The coefficient is placed only at site zero; N≥1 is needed for this construction.
  • etaAmplitude: Eq.(3), PDF p.2: η(d)=|0⟩+exp(d)|1⟩; there is no extra i in this exponent.
  • RageParameters: PDF p.2: all admissible numerical input data; constraints do not remove stored entries.
  • DescriptionIndex: PDF p.2: stored real coordinates: real/imaginary tensor entries, one weight per unordered pair, and real/imaginary entries of each 2-by-2 unitary.
  • describe: PDF p.2: the explicit coordinate description, with the last Boolean selecting Im.
  • joinBits: PDF p.2: glue retained and traced-out bit strings, including empty supports.
  • rawMarginal: PDF p.2: actual partial trace of |v⟩⟨v|, without normalization.
  • rageMarginal: PDF pp.2–4: normalized reduced density matrix, used only for nonzero v.
  • zMean: PDF pp.1,3–4: Z expectation on a unit vector.
  • connectedZ: PDF pp.1,3–4: connected two-point Z correlation on a unit vector.
  • firstBlock: PDF p.2: the first L sites (meaningful also for L=0 and L=N).
  • nextSite: PDF p.2: one cyclic increment. An existing index supplies positivity of N.
  • CyclicInvariant: PDF p.2: exact cyclic invariance of a vector, without a global-phase quotient.
  • transferE: PDF pp.2–3: E[k,a,b]=A[k,a] ⊗ conjugate(A[k,b]); conjugation is entrywise.
  • bitReal: PDF pp.2–3: real bit indicator, to keep a-b signed.
  • transferT: PDF pp.2–3: corrected transfer matrices. The outside phase uses the summed physical index t, not the unbound label in the printed B formula.
  • crossMarginal: PDF pp.2–3: the cross-edge reduced kernel, contracted in chain order.
  • retainedOp: PDF p.2: internal graph gates followed by the rotations on retained sites.
  • rayleighEnergy: PDF p.3, Eq.(4): energy of a raw nonzero vector.
  • SiteCoordinates: PDF p.3: both physical tensors at one site supply 2D² complex coordinates.
  • replaceSite: PDF p.3: replace one site's two tensors, freezing every other entry.
  • siteMap: PDF p.3: the constructed one-site physical linear map, by its coordinate columns.
  • rageSiteQuadratic: PDF p.3: x†Mx, with a complex value until its real part is taken.
  • siteVector: PDF p.3: physical vector from the constructed one-site map.
  • controlledPhaseAction: PDF pp.3–4: apply a phase gate to a distinct pair, using an arbitrary complex label.
  • edgeBackground: PDF p.3: undo one edge from the graph-enhanced vector before the final V layer.
  • edgePart: PDF p.3: the P11 or complementary component of the frozen edge background.
  • edgeTrial: PDF p.3: edge-coordinate trial vector, retaining the entire two-site phase gate.
  • edgeCoefficients: PDF p.3: single-edge energy coefficients, with V undone from H as printed.
  • minimizingPhase: PDF p.3: a minimizing unit-modulus phase for c0+2Re(c1 z).
  • SingleEdgeEnergyLaw: PDF p.3: the single-edge energy form and its constrained minimum. This is not a minimization over unconstrained complex z, and gives no joint global phase optimum.
  • wrapAngle: PDF p.4: reduce any real angle to [0,2π), including negative angles.
  • updatedWeights: PDF p.4: update both symmetric entries, leaving every other pair fixed.
  • overlapObjective: PDF p.4, Eq.(5): normalized squared overlap with a normalized target.
  • localGate: PDF p.4: put one single-qubit unitary at the selected wire.
  • overlapCoefficients: PDF p.4: squared overlap coefficients for the incident-edge coordinate.
  • oppositeWeights: PDF p.2, (i)–(ii): weights of a circulant opposite-site matching on 2L sites.
  • cyclicBlock: PDF p.2, (ii): contiguous blocks on a cyclic chain, including wrapping blocks.
  • mpsTangent: PDF p.3: derivative of the trace product, obtained by inserting one tensor derivative.
  • localTangent: PDF p.3: derivative of the tensor product of local matrices.
  • rawTangent: PDF p.3: explicit differentiated finite tensor/phase product. The ambient formula extends the unitary charts smoothly; no defective unrestricted real-Pauli chart is used.
  • ScalarInstruction: PDF pp.2–3 and p.4 Extensions: ideal scalar instructions, with no matrix-operation primitive. A productCall is reserved for the explicitly supplied base contraction evaluator.
  • ScalarInstruction.eval: PDF pp.2–3: one instruction's exact semantics. Division has a checked denominator.
  • ScalarProgram: PDF pp.2–3: a straight-line scalar program. All registers initially contain zero; each instruction writes the next register. Work includes reads and output-factor formation.
  • ScalarProgram.execute: PDF pp.2–3: execute the instruction list; undefined division fails explicitly.
  • ScalarProgram.calls: PDF p.4: number of calls to the base product-operator evaluator.
  • ScalarProgram.work: PDF pp.2–4: scalar work, charging an oracle call for formation of all 4N factors, in addition to a supplied per-call base-evaluation budget B.
  • ContractionInput: PDF pp.2–3: typed scalar inputs for local contraction. O may be non-Hermitian.
  • contractionData: PDF pp.2–3: numerical input values; no oracle supplies any desired marginal.
  • MarginalProgram: PDF pp.2–3: program outputs include every partial transfer product, so the theorem requires the transfer construction itself, not just an unrelated scalar output.
  • MarginalProgram.Correct: PDF pp.2–3: a program's full transfer-contraction specification. Partial products are in chain order. Both norm division and the final local conjugation must be executed.
  • supportedOp: PDF p.4: embed an operator supported on S, with the identity on its complement.
  • QubitCliffordGate: PDF p.4: a unitary Clifford circuit, with no measurements or postselection. H, S and controlled-X generate the qubit Clifford circuits.
  • hadamardMatrix: PDF p.4: the elementary Hadamard matrix in Boolean basis order 0,1.
  • QubitCliffordGate.matrix: PDF p.4: exact gate action of the three Clifford generators.
  • cliffordMatrix: PDF p.4: circuit order is chronological, so the first gate acts first.
  • EnhancementInput: PDF p.4 Extensions: enhancement inputs, excluding the base state's product evaluator.
  • enhancementData: PDF p.4 Extensions: input data read by the conditional reduction.
  • EnhancementProgram: PDF p.4 Extensions: output register of a product-evaluator reduction.
  • ExactProductEvaluator: PDF p.4 Extensions: exact product expectations, for all complex local matrices. This interface deliberately includes non-Hermitian factors and is uniform in those factors.
  • localTermHamiltonian: PDF pp.2–3: a supplied sum of local Hamiltonian terms. Supports may be long-range.
  • EdgeInput: PDF p.3: scalar inputs for evaluating one-edge energy coefficients term by term.
  • edgeData: PDF p.3: edge coefficient input values, with no precomputed coefficient oracle.
  • EdgeProgram: PDF p.3: executable output registers for c0,c1,Z and the supplied total energy.
Definition code
import Mathlib
import Definitions.Def_QAlgorithms_Defs_Basic
import Definitions.Def_QAlgorithms_Defs_Ensemble

/-!
Statements from Hübener et al., arXiv:0802.1211v1, PDF pp.1–4.
Paper-local definitions use the periodic trace convention of Eq.(1), not open-boundary MPS.
All algebraic vectors are raw; every physical expectation, marginal and entropy is normalized.
Compilation is pending the batch mechanical handoff.
-/

noncomputable section

open scoped ComplexConjugate Matrix

namespace QAlgorithms.Papers.Independent.Intakethird100.P57

attribute [local instance] Classical.propDecidable

/-- Eq.(1), PDF pp.1–2: two arbitrary complex D-by-D site matrices. -/
abbrev Tensors (N D : ℕ) := Fin N → Bool → Matrix (Fin D) (Fin D) ℂ

/-- Eq.(1), PDF p.1: the periodic trace MPS, with matrices multiplied in chain order. -/
def traceMPS {N D : ℕ} (A : Tensors N D) : EuclideanSpace ℂ (Qubits N) :=
  WithLp.toLp 2 fun b => ((List.ofFn fun k => A k (b k)).prod).trace

/-- PDF p.2: symmetric, zero-diagonal graph weights in [0,2π). -/
structure PhaseGraph (N : ℕ) where
  weight : Fin N → Fin N → ℝ
  symmetric : ∀ i j, weight i j = weight j i
  diagonal : ∀ i, weight i i = 0
  nonnegative : ∀ i j, 0 ≤ weight i j
  bounded : ∀ i j, weight i j < 2 * Real.pi

/-- The absent graph (PDF p.2, following Eq.(2)). -/
def emptyPhaseGraph (N : ℕ) : PhaseGraph N where
  weight := fun _ _ => 0
  symmetric := by intros; rfl
  diagonal := by intros; rfl
  nonnegative := by intros; exact le_refl 0
  bounded := by intros; positivity

/-- PDF p.2: tensor product of local matrices, on arbitrary finite sets of wires. -/
def productOp {ι : Type*} [Fintype ι] (V : ι → Matrix Bool Bool ℂ) :
    Matrix (ι → Bool) (ι → Bool) ℂ :=
  Matrix.of fun a b => ∏ k, V k (a k) (b k)

/-- PDF p.2: each unordered edge acts once, with the positive controlled phase. -/
def graphAngle {ι : Type*} [Fintype ι] [LinearOrder ι]
    (w : ι → ι → ℝ) (b : ι → Bool) : ℝ :=
  ∑ i, ∑ j, if i < j ∧ b i = true ∧ b j = true then w i j else 0

/-- PDF p.2: diagonal product of all controlled-phase gates. -/
def graphOp {ι : Type*} [Fintype ι] [LinearOrder ι] (w : ι → ι → ℝ) :
    Matrix (ι → Bool) (ι → Bool) ℂ :=
  Matrix.diagonal fun b => Complex.exp (Complex.I * (graphAngle w b : ℂ))

/-- Eq.(2), PDF p.2: graph enhancement followed by the local rotations. -/
def enhance {N : ℕ} (G : PhaseGraph N) (V : Fin N → Matrix.unitaryGroup Bool ℂ)
    (v : EuclideanSpace ℂ (Qubits N)) : EuclideanSpace ℂ (Qubits N) :=
  act (productOp fun k => (V k : Matrix Bool Bool ℂ)) (act (graphOp G.weight) v)

/-- Eq.(2), PDF p.2: the RAGE raw vector. -/
def rage {N D : ℕ} (A : Tensors N D) (G : PhaseGraph N)
    (V : Fin N → Matrix.unitaryGroup Bool ℂ) : EuclideanSpace ℂ (Qubits N) :=
  enhance G V (traceMPS A)

/-- PDF pp.2–4: normalize a raw nonzero vector before physical uses.
At zero this total helper is zero; all physical theorems exclude that input. -/
def normalizeRageVector {ι : Type*} [Fintype ι] (v : EuclideanSpace ℂ ι) : EuclideanSpace ℂ ι :=
  ((‖v‖ : ℂ)⁻¹) • v

/-- PDF p.2, Eq.(3), second line: an arbitrary product vector. -/
def productVec {N : ℕ} (r : Fin N → Bool → ℂ) : EuclideanSpace ℂ (Qubits N) :=
  WithLp.toLp 2 fun b => ∏ k, r k (b k)

/-- PDF p.2: normalized plus factors. -/
def plusFactors (N : ℕ) : Fin N → Bool → ℂ :=
  fun _ _ => (Real.sqrt 2 : ℂ)⁻¹

/-- PDF p.2: bond-one matrices for product vectors. -/
def productTensors {N : ℕ} (r : Fin N → Bool → ℂ) : Tensors N 1 :=
  fun k b => Matrix.of fun _ _ => r k b

/-- Eq.(3), second line, PDF p.2: diagonal tensors for a finite sum of products.
The coefficient is placed only at site zero; N≥1 is needed for this construction. -/
def diagonalTensors {N m : ℕ} (c : Fin m → ℂ)
    (r : Fin m → Fin N → Bool → ℂ) : Tensors N m :=
  fun k b => Matrix.diagonal fun t => (if k.val = 0 then c t else 1) * r t k b

/-- Eq.(3), PDF p.2: η(d)=|0⟩+exp(d)|1⟩; there is no extra i in this exponent. -/
def etaAmplitude (d : ℂ) (b : Bool) : ℂ := if b then Complex.exp d else 1

/-- Sanity: no spurious phase on a basis string with no occupied pair. -/
example (G : PhaseGraph 1) (b : Qubits 1) : graphAngle G.weight b = 0 := by
  simp [graphAngle]

/-- Sanity: the zero raw vector is not accidentally turned into a physical state. -/
example {ι : Type*} [Fintype ι] : normalizeRageVector (0 : EuclideanSpace ℂ ι) = 0 := by
  simp [normalizeRageVector]

/-- Sanity: the product factors in Eq.(3) have the stated amplitudes. -/
example (d : ℂ) : etaAmplitude d false = 1 ∧ etaAmplitude d true = Complex.exp d := ⟨rfl, rfl⟩

/-- PDF p.2: all admissible numerical input data; constraints do not remove stored entries. -/
structure RageParameters (N D : ℕ) where
  tensors : Tensors N D
  graph : PhaseGraph N
  rotations : Fin N → Matrix.unitaryGroup Bool ℂ

/-- PDF p.2: stored real coordinates: real/imaginary tensor entries, one weight per
unordered pair, and real/imaginary entries of each 2-by-2 unitary. -/
abbrev DescriptionIndex (N D : ℕ) :=
  (Fin N × Bool × Fin D × Fin D × Bool) ⊕
    ({p : Fin N × Fin N // p.1 < p.2} ⊕ (Fin N × Bool × Bool × Bool))

/-- PDF p.2: the explicit coordinate description, with the last Boolean selecting Im. -/
def describe {N D : ℕ} (p : RageParameters N D) : DescriptionIndex N D → ℝ
  | .inl (k,b,i,j,part) => if part then (p.tensors k b i j).im else (p.tensors k b i j).re
  | .inr (.inl e) => p.graph.weight e.val.1 e.val.2
  | .inr (.inr (k,b,c,part)) =>
      if part then ((p.rotations k : Matrix Bool Bool ℂ) b c).im
      else ((p.rotations k : Matrix Bool Bool ℂ) b c).re

/-- PDF p.2: glue retained and traced-out bit strings, including empty supports. -/
def joinBits {N : ℕ} (S : Finset (Fin N)) (a : S → Bool)
    (e : {k : Fin N // k ∉ S} → Bool) : Qubits N :=
  fun k => if h : k ∈ S then a ⟨k,h⟩ else e ⟨k,h⟩

/-- PDF p.2: actual partial trace of |v⟩⟨v|, without normalization. -/
def rawMarginal {N : ℕ} (v : EuclideanSpace ℂ (Qubits N)) (S : Finset (Fin N)) :
    Matrix (S → Bool) (S → Bool) ℂ :=
  Matrix.of fun a b => ∑ e : {k : Fin N // k ∉ S} → Bool,
    v (joinBits S a e) * conj (v (joinBits S b e))

/-- PDF pp.2–4: normalized reduced density matrix, used only for nonzero v. -/
def rageMarginal {N : ℕ} (v : EuclideanSpace ℂ (Qubits N)) (S : Finset (Fin N)) :
    Matrix (S → Bool) (S → Bool) ℂ :=
  (((‖v‖ ^ 2 : ℝ) : ℂ)⁻¹) • rawMarginal v S

/-- PDF pp.1,3–4: Z expectation on a unit vector. -/
def zMean {N : ℕ} (v : EuclideanSpace ℂ (Qubits N)) (i : Fin N) : ℝ :=
  ∑ b, (if b i then -1 else 1) * Complex.normSq (v b)

/-- PDF pp.1,3–4: connected two-point Z correlation on a unit vector. -/
def connectedZ {N : ℕ} (v : EuclideanSpace ℂ (Qubits N)) (i j : Fin N) : ℝ :=
  (∑ b, (if b i then -1 else 1) * (if b j then -1 else 1) * Complex.normSq (v b)) -
    zMean v i * zMean v j

/-- PDF p.2: the first L sites (meaningful also for L=0 and L=N). -/
def firstBlock (N L : ℕ) : Finset (Fin N) := Finset.univ.filter fun i => i.val < L

/-- PDF p.2: one cyclic increment. An existing index supplies positivity of N. -/
def nextSite {N : ℕ} (i : Fin N) : Fin N :=
  ⟨(i.val + 1) % N, Nat.mod_lt _ (Nat.zero_lt_of_lt i.isLt)⟩

/-- PDF p.2: exact cyclic invariance of a vector, without a global-phase quotient. -/
def CyclicInvariant {N : ℕ} (v : EuclideanSpace ℂ (Qubits N)) : Prop :=
  ∀ b, v (fun k => b (nextSite k)) = v b

/-- PDF pp.2–3: E[k,a,b]=A[k,a] ⊗ conjugate(A[k,b]); conjugation is entrywise. -/
def transferE {N D : ℕ} (A : Tensors N D) (k : Fin N) (a b : Bool) :
    Matrix (Fin D × Fin D) (Fin D × Fin D) ℂ :=
  Matrix.kronecker (A k a) (Matrix.of fun i j => conj (A k b i j))

/-- PDF pp.2–3: real bit indicator, to keep a-b signed. -/
def bitReal (b : Bool) : ℝ := if b then 1 else 0

/-- PDF pp.2–3: corrected transfer matrices. The outside phase uses the summed physical
index t, not the unbound label in the printed B formula. -/
def transferT {N D : ℕ} (A : Tensors N D) (G : PhaseGraph N) (S : Finset (Fin N))
    (a b : S → Bool) (k : Fin N) : Matrix (Fin D × Fin D) (Fin D × Fin D) ℂ :=
  if hk : k ∈ S then transferE A k (a ⟨k,hk⟩) (b ⟨k,hk⟩)
  else ∑ t : Bool,
    Complex.exp (Complex.I * ((bitReal t *
      ∑ j : S, G.weight j.val k * (bitReal (a j) - bitReal (b j))) : ℂ)) •
      transferE A k t t

/-- PDF pp.2–3: the cross-edge reduced kernel, contracted in chain order. -/
def crossMarginal {N D : ℕ} (A : Tensors N D) (G : PhaseGraph N) (S : Finset (Fin N)) :
    Matrix (S → Bool) (S → Bool) ℂ :=
  Matrix.of fun a b => ((List.ofFn fun k => transferT A G S a b k).prod).trace

/-- PDF p.2: internal graph gates followed by the rotations on retained sites. -/
def retainedOp {N : ℕ} (G : PhaseGraph N) (V : Fin N → Matrix.unitaryGroup Bool ℂ)
    (S : Finset (Fin N)) : Matrix (S → Bool) (S → Bool) ℂ :=
  productOp (fun k : S => (V k.val : Matrix Bool Bool ℂ)) *
    graphOp (fun i j : S => G.weight i.val j.val)

/-- Sanity: no natural-number subtraction enters the phase difference. -/
example : bitReal false - bitReal true = -1 := by norm_num [bitReal]

/-- PDF p.3, Eq.(4): energy of a raw nonzero vector. -/
def rayleighEnergy {N : ℕ} (H : Matrix (Qubits N) (Qubits N) ℂ)
    (v : EuclideanSpace ℂ (Qubits N)) : ℝ :=
  (inner ℂ v (act H v)).re / ‖v‖ ^ 2

/-- PDF p.3: both physical tensors at one site supply 2D² complex coordinates. -/
abbrev SiteCoordinates (D : ℕ) := Bool × Fin D × Fin D

/-- PDF p.3: replace one site's two tensors, freezing every other entry. -/
def replaceSite {N D : ℕ} (A : Tensors N D) (k : Fin N)
    (x : SiteCoordinates D → ℂ) : Tensors N D :=
  fun j b => if j = k then Matrix.of fun i l => x (b,i,l) else A j b

/-- PDF p.3: the constructed one-site physical linear map, by its coordinate columns. -/
def siteMap {N D : ℕ} (A : Tensors N D) (G : PhaseGraph N)
    (V : Fin N → Matrix.unitaryGroup Bool ℂ) (k : Fin N) :
    Matrix (Qubits N) (SiteCoordinates D) ℂ :=
  Matrix.of fun b c => rage (replaceSite A k (fun e => if e = c then 1 else 0)) G V b

/-- PDF p.3: x†Mx, with a complex value until its real part is taken. -/
def rageSiteQuadratic {ι : Type*} [Fintype ι] (M : Matrix ι ι ℂ) (x : ι → ℂ) : ℂ :=
  ∑ i, ∑ j, conj (x i) * M i j * x j

/-- PDF p.3: physical vector from the constructed one-site map. -/
def siteVector {N D : ℕ} (L : Matrix (Qubits N) (SiteCoordinates D) ℂ)
    (x : SiteCoordinates D → ℂ) : EuclideanSpace ℂ (Qubits N) :=
  WithLp.toLp 2 (L.mulVec x)

/-- PDF pp.3–4: apply a phase gate to a distinct pair, using an arbitrary complex label. -/
def controlledPhaseAction {N : ℕ} (j k : Fin N) (z : ℂ)
    (v : EuclideanSpace ℂ (Qubits N)) : EuclideanSpace ℂ (Qubits N) :=
  WithLp.toLp 2 fun b => (if b j = true ∧ b k = true then z else 1) * v b

/-- PDF p.3: undo one edge from the graph-enhanced vector before the final V layer. -/
def edgeBackground {N D : ℕ} (A : Tensors N D) (G : PhaseGraph N) (j k : Fin N) :
    EuclideanSpace ℂ (Qubits N) :=
  controlledPhaseAction j k (Complex.exp (-Complex.I * (G.weight j k : ℂ)))
    (act (graphOp G.weight) (traceMPS A))

/-- PDF p.3: the P11 or complementary component of the frozen edge background. -/
def edgePart {N : ℕ} (v : EuclideanSpace ℂ (Qubits N)) (j k : Fin N) (on : Bool) :
    EuclideanSpace ℂ (Qubits N) :=
  WithLp.toLp 2 fun b => if (b j && b k) = on then v b else 0

/-- PDF p.3: edge-coordinate trial vector, retaining the entire two-site phase gate. -/
def edgeTrial {N D : ℕ} (A : Tensors N D) (G : PhaseGraph N)
    (V : Fin N → Matrix.unitaryGroup Bool ℂ) (j k : Fin N) (z : ℂ) :
    EuclideanSpace ℂ (Qubits N) :=
  act (productOp fun q => (V q : Matrix Bool Bool ℂ))
    (controlledPhaseAction j k z (edgeBackground A G j k))

/-- PDF p.3: single-edge energy coefficients, with V undone from H as printed. -/
def edgeCoefficients {N D : ℕ} (A : Tensors N D) (G : PhaseGraph N)
    (V : Fin N → Matrix.unitaryGroup Bool ℂ) (j k : Fin N)
    (H : Matrix (Qubits N) (Qubits N) ℂ) : ℝ × ℂ :=
  let W := productOp fun q => (V q : Matrix Bool Bool ℂ)
  let HV := W.conjTranspose * H * W
  let u := edgePart (edgeBackground A G j k) j k false
  let v := edgePart (edgeBackground A G j k) j k true
  ((inner ℂ u (act HV u)).re + (inner ℂ v (act HV v)).re,
    inner ℂ u (act HV v))

/-- PDF p.3: a minimizing unit-modulus phase for c0+2Re(c1 z). -/
def minimizingPhase (c : ℂ) : ℂ := if c = 0 then 1 else -conj c / (‖c‖ : ℂ)

/-- PDF p.3: the single-edge energy form and its constrained minimum. This is not a
minimization over unconstrained complex z, and gives no joint global phase optimum. -/
def SingleEdgeEnergyLaw {N D : ℕ} (hN : 1 ≤ N) (hD : 1 ≤ D)
    (A : Tensors N D) (G : PhaseGraph N) (V : Fin N → Matrix.unitaryGroup Bool ℂ)
    (hv : traceMPS A ≠ 0) (j k : Fin N) (hjk : j ≠ k)
    (H : Matrix (Qubits N) (Qubits N) ℂ) (hH : H.IsHermitian) : Prop :=
    let c := edgeCoefficients A G V j k H
    let Z := ‖traceMPS A‖ ^ 2
    (∀ z : ℂ, ‖z‖ = 1 → ‖edgeTrial A G V j k z‖ ^ 2 = Z ∧
      rayleighEnergy H (edgeTrial A G V j k z) = (c.1 + 2 * (c.2 * z).re) / Z) ∧
    ‖minimizingPhase c.2‖ = 1 ∧
    (∀ z : ℂ, ‖z‖ = 1 → rayleighEnergy H (edgeTrial A G V j k (minimizingPhase c.2)) ≤
      rayleighEnergy H (edgeTrial A G V j k z)) ∧
    (c.2 = 0 → ∀ z : ℂ, ‖z‖ = 1 → rayleighEnergy H (edgeTrial A G V j k z) = c.1 / Z)

/-- PDF p.4: reduce any real angle to [0,2π), including negative angles. -/
def wrapAngle (theta : ℝ) : ℝ :=
  theta - (2 * Real.pi) * (Int.floor (theta / (2 * Real.pi)) : ℝ)

/-- PDF p.4: update both symmetric entries, leaving every other pair fixed. -/
def updatedWeights {N : ℕ} (G : PhaseGraph N) (j k : Fin N) (theta : ℝ) : Fin N → Fin N → ℝ :=
  fun a b => if (a = j ∧ b = k) ∨ (a = k ∧ b = j)
    then wrapAngle (G.weight j k + theta) else G.weight a b

/-- PDF p.4, Eq.(5): normalized squared overlap with a normalized target. -/
def overlapObjective {N : ℕ} (v chi : EuclideanSpace ℂ (Qubits N)) : ℝ :=
  Complex.normSq (inner ℂ v chi) / ‖v‖ ^ 2

/-- PDF p.4: put one single-qubit unitary at the selected wire. -/
def localGate {N : ℕ} (q : Fin N) (U : Matrix.unitaryGroup Bool ℂ) :
    Matrix (Qubits N) (Qubits N) ℂ :=
  productOp fun k => if k = q then (U : Matrix Bool Bool ℂ) else 1

/-- PDF p.4: squared overlap coefficients for the incident-edge coordinate. -/
def overlapCoefficients {N D : ℕ} (A : Tensors N D) (G : PhaseGraph N) (j k : Fin N)
    (chi : EuclideanSpace ℂ (Qubits N)) : ℝ × ℂ :=
  let u := edgePart (edgeBackground A G j k) j k false
  let v := edgePart (edgeBackground A G j k) j k true
  let a := inner ℂ u chi
  let b := inner ℂ v chi
  (Complex.normSq a + Complex.normSq b, a * conj b)

/-- PDF p.2, (i)–(ii): weights of a circulant opposite-site matching on 2L sites. -/
def oppositeWeights (L : ℕ) : Fin (2 * L) → Fin (2 * L) → ℝ :=
  fun i j => if i ≠ j ∧ (i.val + L) % (2 * L) = j.val then Real.pi else 0

/-- PDF p.2, (ii): contiguous blocks on a cyclic chain, including wrapping blocks. -/
def cyclicBlock (N : ℕ) (start : Fin N) (ell : ℕ) : Finset (Fin N) :=
  Finset.univ.filter fun i => ∃ t : ℕ, t < ell ∧ i.val = (start.val + t) % N

/-- PDF p.3: derivative of the trace product, obtained by inserting one tensor derivative. -/
def mpsTangent {N D : ℕ} (A Adot : Tensors N D) : EuclideanSpace ℂ (Qubits N) :=
  WithLp.toLp 2 fun b => ∑ k : Fin N,
    ((List.ofFn fun l => if l = k then Adot l (b l) else A l (b l)).prod).trace

/-- PDF p.3: derivative of the tensor product of local matrices. -/
def localTangent {N : ℕ} (V Vdot : Fin N → Matrix Bool Bool ℂ) :
    Matrix (Qubits N) (Qubits N) ℂ :=
  Matrix.of fun a b => ∑ k : Fin N,
    ∏ l : Fin N, if l = k then Vdot l (a l) (b l) else V l (a l) (b l)

/-- PDF p.3: explicit differentiated finite tensor/phase product. The ambient formula
extends the unitary charts smoothly; no defective unrestricted real-Pauli chart is used. -/
def rawTangent {N D : ℕ} (A Adot : Tensors N D)
    (w wdot : Fin N → Fin N → ℝ) (V Vdot : Fin N → Matrix Bool Bool ℂ) :
    EuclideanSpace ℂ (Qubits N) :=
  act (localTangent V Vdot) (act (graphOp w) (traceMPS A)) +
    act (productOp V) (WithLp.toLp 2 fun b =>
      Complex.exp (Complex.I * (graphAngle w b : ℂ)) *
        (mpsTangent A Adot b + Complex.I * (graphAngle wdot b : ℂ) * traceMPS A b))

/-- PDF pp.2–3 and p.4 Extensions: ideal scalar instructions, with no matrix-operation
primitive. A productCall is reserved for the explicitly supplied base contraction evaluator. -/
inductive ScalarInstruction (N : ℕ) (Input : Type*) where
  | constant (c : ℂ)
  | read (i : Input)
  | add (a b : ℕ)
  | mul (a b : ℕ)
  | divide (a b : ℕ)
  | conjugate (a : ℕ)
  | phase (a : ℕ)
  | productCall (factors : Fin N → Bool → Bool → ℕ)

/-- PDF pp.2–3: one instruction's exact semantics. Division has a checked denominator. -/
def ScalarInstruction.eval {N : ℕ} {Input : Type*}
    (data : Input → ℂ) (base : (Fin N → Matrix Bool Bool ℂ) → ℂ)
    (mem : ℕ → ℂ) : ScalarInstruction N Input → Option ℂ
  | .constant c => some c
  | .read i => some (data i)
  | .add a b => some (mem a + mem b)
  | .mul a b => some (mem a * mem b)
  | .divide a b => if mem b = 0 then none else some (mem a / mem b)
  | .conjugate a => some (conj (mem a))
  | .phase a => some (Complex.exp (Complex.I * (mem a).re))
  | .productCall factors => some (base (fun k => Matrix.of fun a b => mem (factors k a b)))

/-- PDF pp.2–3: a straight-line scalar program. All registers initially contain zero;
each instruction writes the next register. Work includes reads and output-factor formation. -/
structure ScalarProgram (N : ℕ) (Input : Type*) where
  code : List (ScalarInstruction N Input)

/-- PDF pp.2–3: execute the instruction list; undefined division fails explicitly. -/
def ScalarProgram.execute {N : ℕ} {Input : Type*} (p : ScalarProgram N Input)
    (data : Input → ℂ) (base : (Fin N → Matrix Bool Bool ℂ) → ℂ) : Option (ℕ → ℂ) :=
  ((p.code.foldl (fun (st : Option (ℕ × (ℕ → ℂ))) op =>
    st.bind fun s => (op.eval data base s.2).map fun v =>
      (s.1 + 1, Function.update s.2 s.1 v)) (some (0,fun _ => 0))).map Prod.snd)

/-- PDF p.4: number of calls to the base product-operator evaluator. -/
def ScalarProgram.calls {N : ℕ} {Input : Type*} (p : ScalarProgram N Input) : ℕ :=
  p.code.countP fun op => match op with | .productCall _ => true | _ => false

/-- PDF pp.2–4: scalar work, charging an oracle call for formation of all 4N factors,
in addition to a supplied per-call base-evaluation budget B. -/
def ScalarProgram.work {N : ℕ} {Input : Type*} (p : ScalarProgram N Input) (B : ℕ := 0) : ℕ :=
  (p.code.map fun op => match op with
    | .productCall _ => 4 * N + 1 + B
    | _ => 1).sum

/-- Sanity: a real zero denominator is never silently assigned a scalar answer. -/
example {N : ℕ} {Input : Type*} (data : Input → ℂ)
    (base : (Fin N → Matrix Bool Bool ℂ) → ℂ) :
    (ScalarInstruction.divide 0 0 : ScalarInstruction N Input).eval data base (fun _ => 0) = none := by
  simp [ScalarInstruction.eval]

/-- Sanity: the instruction list is charged, including an input read. -/
example {N : ℕ} {Input : Type*} (i : Input) :
    (ScalarProgram.mk [.read i] : ScalarProgram N Input).work 0 = 1 := rfl

/-- PDF pp.2–3: typed scalar inputs for local contraction. O may be non-Hermitian. -/
inductive ContractionInput (N D : ℕ) (S : Finset (Fin N)) where
  | tensor (k : Fin N) (b : Bool) (i j : Fin D)
  | phase (i j : Fin N)
  | rotation (k : Fin N) (a b : Bool)
  | observable (a b : S → Bool)

/-- PDF pp.2–3: numerical input values; no oracle supplies any desired marginal. -/
def contractionData {N D : ℕ} {S : Finset (Fin N)} (A : Tensors N D) (G : PhaseGraph N)
    (V : Fin N → Matrix.unitaryGroup Bool ℂ) (O : Matrix (S → Bool) (S → Bool) ℂ) :
    ContractionInput N D S → ℂ
  | .tensor k b i j => A k b i j
  | .phase i j => (G.weight i j : ℂ)
  | .rotation k a b => (V k : Matrix Bool Bool ℂ) a b
  | .observable a b => O a b

/-- PDF pp.2–3: program outputs include every partial transfer product, so the theorem
requires the transfer construction itself, not just an unrelated scalar output. -/
structure MarginalProgram (N D : ℕ) (S : Finset (Fin N)) where
  scalar : ScalarProgram N (ContractionInput N D S)
  stage : (S → Bool) → (S → Bool) → Fin (N + 1) →
    (Fin D × Fin D) → (Fin D × Fin D) → ℕ
  cross : (S → Bool) → (S → Bool) → ℕ
  norm : ℕ
  entry : (S → Bool) → (S → Bool) → ℕ
  expectation : ℕ

/-- PDF pp.2–3: a program's full transfer-contraction specification. Partial products
are in chain order. Both norm division and the final local conjugation must be executed. -/
def MarginalProgram.Correct {N D : ℕ} {S : Finset (Fin N)} (p : MarginalProgram N D S)
    (A : Tensors N D) (G : PhaseGraph N) (V : Fin N → Matrix.unitaryGroup Bool ℂ)
    (O : Matrix (S → Bool) (S → Bool) ℂ) : Prop :=
  ∃ mem : ℕ → ℂ,
    p.scalar.execute (contractionData A G V O) (fun _ => 0) = some mem ∧
    mem p.norm = (‖traceMPS A‖ ^ 2 : ℝ) ∧
    (∀ a b t i j, p.stage a b t i j < p.scalar.code.length ∧
      mem (p.stage a b t i j) =
        (((List.ofFn fun k => transferT A G S a b k).take t.val).prod) i j) ∧
    (∀ a b, p.cross a b < p.scalar.code.length ∧
      mem (p.cross a b) = crossMarginal A G S a b) ∧
    (∀ a b, p.entry a b < p.scalar.code.length ∧
      mem (p.entry a b) = rageMarginal (rage A G V) S a b) ∧
    p.norm < p.scalar.code.length ∧ p.expectation < p.scalar.code.length ∧
    mem p.expectation = (O * rageMarginal (rage A G V) S).trace

/-- PDF p.4: embed an operator supported on S, with the identity on its complement. -/
def supportedOp {N : ℕ} (S : Finset (Fin N)) (O : Matrix (S → Bool) (S → Bool) ℂ) :
    Matrix (Qubits N) (Qubits N) ℂ :=
  Matrix.of fun a b => if ∀ k : Fin N, k ∉ S → a k = b k
    then O (fun k => a k.val) (fun k => b k.val) else 0

/-- PDF p.4: a unitary Clifford circuit, with no measurements or postselection.
H, S and controlled-X generate the qubit Clifford circuits. -/
inductive QubitCliffordGate (N : ℕ) where
  | hadamard (q : Fin N)
  | phase (q : Fin N)
  | controlledX (control target : Fin N) (distinct : control ≠ target)

/-- PDF p.4: the elementary Hadamard matrix in Boolean basis order 0,1. -/
def hadamardMatrix : Matrix Bool Bool ℂ :=
  Matrix.of fun a b => if a = true ∧ b = true
    then -(Real.sqrt 2 : ℂ)⁻¹ else (Real.sqrt 2 : ℂ)⁻¹

/-- PDF p.4: exact gate action of the three Clifford generators. -/
def QubitCliffordGate.matrix {N : ℕ} : QubitCliffordGate N → Matrix (Qubits N) (Qubits N) ℂ
  | .hadamard q => productOp fun k => if k = q then hadamardMatrix else 1
  | .phase q => productOp fun k => if k = q then
      Matrix.diagonal (fun b : Bool => if b then Complex.I else 1) else 1
  | .controlledX j k _ => Matrix.of fun a b =>
      if a = (fun q => if q = k then Bool.xor (b k) (b j) else b q) then 1 else 0

/-- PDF p.4: circuit order is chronological, so the first gate acts first. -/
def cliffordMatrix {N : ℕ} (circuit : List (QubitCliffordGate N)) : Matrix (Qubits N) (Qubits N) ℂ :=
  (circuit.map QubitCliffordGate.matrix).reverse.prod

/-- Sanity: the empty Clifford circuit acts as the identity. -/
example (N : ℕ) : cliffordMatrix ([] : List (QubitCliffordGate N)) = 1 := rfl

/-- PDF p.4 Extensions: enhancement inputs, excluding the base state's product evaluator. -/
inductive EnhancementInput (N : ℕ) (S : Finset (Fin N)) where
  | phase (i j : Fin N)
  | rotation (k : Fin N) (a b : Bool)
  | observable (a b : S → Bool)

/-- PDF p.4 Extensions: input data read by the conditional reduction. -/
def enhancementData {N : ℕ} {S : Finset (Fin N)} (G : PhaseGraph N)
    (V : Fin N → Matrix.unitaryGroup Bool ℂ) (O : Matrix (S → Bool) (S → Bool) ℂ) :
    EnhancementInput N S → ℂ
  | .phase i j => (G.weight i j : ℂ)
  | .rotation k a b => (V k : Matrix Bool Bool ℂ) a b
  | .observable a b => O a b

/-- PDF p.4 Extensions: output register of a product-evaluator reduction. -/
structure EnhancementProgram (N : ℕ) (S : Finset (Fin N)) where
  scalar : ScalarProgram N (EnhancementInput N S)
  output : ℕ

/-- PDF p.4 Extensions: exact product expectations, for all complex local matrices.
This interface deliberately includes non-Hermitian factors and is uniform in those factors. -/
def ExactProductEvaluator {N : ℕ} (psi : EuclideanSpace ℂ (Qubits N))
    (base : (Fin N → Matrix Bool Bool ℂ) → ℂ) : Prop :=
  ∀ factors, base factors = inner ℂ psi (act (productOp factors) psi)

/-- PDF pp.2–3: a supplied sum of local Hamiltonian terms. Supports may be long-range. -/
def localTermHamiltonian {N m : ℕ} (supports : Fin m → Finset (Fin N))
    (terms : (r : Fin m) → Matrix (supports r → Bool) (supports r → Bool) ℂ) :
    Matrix (Qubits N) (Qubits N) ℂ :=
  ∑ r, supportedOp (supports r) (terms r)

/-- PDF p.3: scalar inputs for evaluating one-edge energy coefficients term by term. -/
inductive EdgeInput (N D m : ℕ) (supports : Fin m → Finset (Fin N)) where
  | tensor (k : Fin N) (b : Bool) (i j : Fin D)
  | phase (i j : Fin N)
  | rotation (k : Fin N) (a b : Bool)
  | term (r : Fin m) (a b : supports r → Bool)

/-- PDF p.3: edge coefficient input values, with no precomputed coefficient oracle. -/
def edgeData {N D m : ℕ} {supports : Fin m → Finset (Fin N)}
    (A : Tensors N D) (G : PhaseGraph N) (V : Fin N → Matrix.unitaryGroup Bool ℂ)
    (terms : (r : Fin m) → Matrix (supports r → Bool) (supports r → Bool) ℂ) :
    EdgeInput N D m supports → ℂ
  | .tensor k b i j => A k b i j
  | .phase i j => (G.weight i j : ℂ)
  | .rotation k a b => (V k : Matrix Bool Bool ℂ) a b
  | .term r a b => terms r a b

/-- PDF p.3: executable output registers for c0,c1,Z and the supplied total energy. -/
structure EdgeProgram (N D m : ℕ) (supports : Fin m → Finset (Fin N)) where
  scalar : ScalarProgram N (EdgeInput N D m supports)
  constantCoefficient : ℕ
  phaseCoefficient : ℕ
  norm : ℕ
  totalEnergy : ℕ

end QAlgorithms.Papers.Independent.Intakethird100.P57
Source
Renormalization algorithm with graph enhancement, arXiv:0802.1211v1, https://arxiv.org/abs/0802.1211v1
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What the Lean code literally says, in plain math · gpt-6.1-sol

QAlgorithms.Papers.Independent.Intakethird100.P57.ContractionInput

For any natural numbers N,DN,DN,D, including zero, and any subset S⊆IN={0,…,N−1}S\subseteq I_N=\{0,\ldots,N-1\}S⊆IN​={0,…,N−1}, this defines a type of input labels with four distinct forms: a tensor label (k,b,i,j)(k,b,i,j)(k,b,i,j), where k∈INk\in I_Nk∈IN​, bbb is Boolean, and i,j∈IDi,j\in I_Di,j∈ID​; a phase label (i,j)(i,j)(i,j), where i,j∈INi,j\in I_Ni,j∈IN​; a rotation label (k,a,b)(k,a,b)(k,a,b), where k∈INk\in I_Nk∈IN​ and a,ba,ba,b are Boolean; and an observable label (a,b)(a,b)(a,b), where a,b:S→{false,true}a,b:S\to\{\mathrm{false},\mathrm{true}\}a,b:S→{false,true}. Phase labels allow equal indices and both orders of each pair. If N=0N=0N=0, only observable labels exist, and there is exactly one such label because SSS is empty; if D=0D=0D=0, no tensor labels exist.

QAlgorithms.Papers.Independent.Intakethird100.P57.CyclicInvariant

For every natural number NNN and every complex vector vvv indexed by {0,1}N\{0,1\}^N{0,1}N, define cyclic invariance to mean that, for every bit string bbb,

v ⁣((b(k+1) mod N)k=0N−1)=v(b).v\!\left((b_{(k+1)\bmod N})_{k=0}^{N-1}\right)=v(b).v((b(k+1)modN​)k=0N−1​)=v(b).

No normalization is required. For N=0N=0N=0, the shifted string is the unique empty string, so the condition holds for every such vector; for N=1N=1N=1, it also holds for every vector because the shift fixes the sole site.

QAlgorithms.Papers.Independent.Intakethird100.P57.DescriptionIndex

For any natural numbers N,DN,DN,D, this abbreviates a disjoint union of three kinds of indices: tuples (k,b,i,j,p)(k,b,i,j,p)(k,b,i,j,p), where k<Nk<Nk<N, b,pb,pb,p are Booleans, and i,j<Di,j<Di,j<D; pairs of sites (j,k)(j,k)(j,k) satisfying j<k<Nj<k<Nj<k<N; and tuples (k,b,c,p)(k,b,c,p)(k,b,c,p), where k<Nk<Nk<N and b,c,pb,c,pb,c,p are Booleans. The three kinds remain distinct even if some of their components coincide. When N=0N=0N=0, this index set is empty; when D=0D=0D=0, the first kind is empty.

QAlgorithms.Papers.Independent.Intakethird100.P57.EdgeInput

For every triple of natural numbers N,D,mN,D,mN,D,m and every family of finite supports Sr⊆{0,…,N−1}S_r\subseteq\{0,\ldots,N-1\}Sr​⊆{0,…,N−1} indexed by r∈{0,…,m−1}r\in\{0,\ldots,m-1\}r∈{0,…,m−1}, this defines a type of input labels with four distinct kinds: a tensor label (k,b,i,j)(k,b,i,j)(k,b,i,j) with site 0≤k<N0\le k<N0≤k<N, Boolean value bbb, and indices 0≤i,j<D0\le i,j<D0≤i,j<D; a phase label (i,j)(i,j)(i,j) with 0≤i,j<N0\le i,j<N0≤i,j<N; a rotation label (k,a,b)(k,a,b)(k,a,b) with 0≤k<N0\le k<N0≤k<N and Boolean values a,ba,ba,b; and a term label (r,a,b)(r,a,b)(r,a,b) with 0≤r<m0\le r<m0≤r<m and Boolean assignments a,b:Sr→{false,true}a,b:S_r\to\{\mathrm{false},\mathrm{true}\}a,b:Sr​→{false,true}. Phase labels include ordered pairs and diagonal pairs without restriction. Zero values of N,D,mN,D,mN,D,m are allowed and remove whichever labels require an index in the corresponding empty range; an empty support still has one Boolean assignment.

QAlgorithms.Papers.Independent.Intakethird100.P57.EdgeProgram

For every triple of natural numbers N,D,mN,D,mN,D,m and family of finite supports Sr⊆{0,…,N−1}S_r\subseteq\{0,\ldots,N-1\}Sr​⊆{0,…,N−1} for 0≤r<m0\le r<m0≤r<m, an edge program consists of a scalar program together with four arbitrary natural-number addresses named the constant coefficient, phase coefficient, norm, and total energy addresses. The scalar program is a finite list with input labels for tensor entries (k,b,i,j)(k,b,i,j)(k,b,i,j), ordered phase pairs (i,j)(i,j)(i,j), rotation entries (k,a,b)(k,a,b)(k,a,b), and term entries (r,a,b)(r,a,b)(r,a,b), where site indices are below NNN, tensor matrix indices are below DDD, Boolean values are arbitrary, and term assignments are Boolean functions on SrS_rSr​. Its instructions may introduce complex constants, read inputs, add, multiply, divide, conjugate, form exp⁡(iRe⁡z)\exp(i\operatorname{Re}z)exp(iRez), or call a supplied function on a family of NNN complex 2×22\times22×2 matrices assembled from memory. Execution begins with all addresses zero and writes successive results at successive addresses starting at zero; unwritten addresses read as zero, and division by zero fails. The structure alone gives no equations for its four designated addresses, no bounds placing them within the instruction list, and no guarantee of successful execution. Zero size parameters and empty supports are permitted.

QAlgorithms.Papers.Independent.Intakethird100.P57.EnhancementInput

For every natural number NNN, including zero, and every subset S⊆IN={0,…,N−1}S\subseteq I_N=\{0,\ldots,N-1\}S⊆IN​={0,…,N−1}, this defines a type of input labels with three distinct forms: a phase label (i,j)(i,j)(i,j) for any i,j∈INi,j\in I_Ni,j∈IN​; a rotation label (k,a,b)(k,a,b)(k,a,b) for any k∈INk\in I_Nk∈IN​ and Boolean a,ba,ba,b; and an observable label (a,b)(a,b)(a,b) for any Boolean assignments a,ba,ba,b on SSS. Phase labels include equal indices and both orders of each pair. If N=0N=0N=0, SSS is empty and the type consists of the single observable label given by the two empty assignments.

QAlgorithms.Papers.Independent.Intakethird100.P57.EnhancementProgram

For every natural number NNN and finite subset S⊆{0,…,N−1}S\subseteq\{0,\ldots,N-1\}S⊆{0,…,N−1}, an enhancement program consists of a scalar program and a natural-number output address. Its scalar program is a finite list of instructions whose input labels are either an ordered pair of sites (i,j)(i,j)(i,j) for a phase, a site and two Boolean values (k,a,b)(k,a,b)(k,a,b) for a rotation entry, or two Boolean assignments (a,b)(a,b)(a,b) on SSS for an observable entry. Instructions may introduce an arbitrary complex constant, read an input, add, multiply, divide, conjugate, form exp⁡(iRe⁡z)\exp(i\operatorname{Re}z)exp(iRez), or call a supplied function on a family of NNN complex 2×22\times22×2 matrices whose entries are taken from memory. Execution starts with every memory address equal to zero and writes successive results at addresses 0,1,…0,1,\ldots0,1,…; division by zero makes execution fail. Operand addresses are unrestricted, so an address not yet written reads as zero. The structure imposes no condition that the output address lies within the instruction list or that execution succeeds. Both N=0N=0N=0 and S=∅S=\varnothingS=∅ are permitted.

QAlgorithms.Papers.Independent.Intakethird100.P57.ExactProductEvaluator

For every natural number NNN, every complex vector ψ\psiψ indexed by Boolean strings of length NNN, and every function base\mathrm{base}base from families of NNN complex 2×22\times22×2 matrices to C\mathbb CC, the predicate says that, for every such family F=(Fk)k=0N−1F=(F_k)_{k=0}^{N-1}F=(Fk​)k=0N−1​, base(F)=⟨ψ,PFψ⟩\mathrm{base}(F)=\langle\psi,P_F\psi\ranglebase(F)=⟨ψ,PF​ψ⟩, where matrix action is ordinary matrix–vector multiplication and (PF)a,b=∏k=0N−1(Fk)ak,bk(P_F)_{a,b}=\prod_{k=0}^{N-1}(F_k)_{a_k,b_k}(PF​)a,b​=∏k=0N−1​(Fk​)ak​,bk​​ for Boolean strings a,ba,ba,b. There is no normalization assumption on ψ\psiψ and no restriction on the matrices FkF_kFk​. For N=0N=0N=0, the product is empty and equals 111, so the required value is the squared modulus of the sole coordinate of ψ\psiψ.

QAlgorithms.Papers.Independent.Intakethird100.P57.MarginalProgram.Correct

For any natural numbers N,DN,DN,D, subset S⊆IN={0,…,N−1}S\subseteq I_N=\{0,\ldots,N-1\}S⊆IN​={0,…,N−1}, program record ppp with scalar code and addresses stage⁡,cross⁡,norm⁡,entry⁡,expectation⁡\operatorname{stage},\operatorname{cross},\operatorname{norm},\operatorname{entry},\operatorname{expectation}stage,cross,norm,entry,expectation, arbitrary complex D×DD\times DD×D matrices Ak(b)A_k(b)Ak​(b), real weights wijw_{ij}wij​ satisfying symmetry, zero diagonal, and 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π, unitary complex 2×22\times22×2 matrices VkV_kVk​, and arbitrary complex matrix OOO indexed by Boolean assignments on SSS, this defines the following predicate. Write BN={false,true}IN\mathcal B_N=\{\mathrm{false},\mathrm{true}\}^{I_N}BN​={false,true}IN​, let ϵ(false)=0\epsilon(\mathrm{false})=0ϵ(false)=0 and ϵ(true)=1\epsilon(\mathrm{true})=1ϵ(true)=1, and define

ϕc=tr⁡ ⁣(A0(c0)⋯AN−1(cN−1)),Z=∑c∈BN∣ϕc∣2,\phi_c=\operatorname{tr}\!\left(A_0(c_0)\cdots A_{N-1}(c_{N-1})\right),\qquad Z=\sum_{c\in\mathcal B_N}|\phi_c|^2,ϕc​=tr(A0​(c0​)⋯AN−1​(cN−1​)),Z=c∈BN​∑​∣ϕc​∣2, rb=∑c∈BN(∏k∈IN(Vk)bkck)exp⁡ ⁣(i∑i,j∈INi<jwijϵ(ci)ϵ(cj))ϕc.r_b=\sum_{c\in\mathcal B_N} \left(\prod_{k\in I_N}(V_k)_{b_kc_k}\right) \exp\!\left(i\sum_{\substack{i,j\in I_N\\i<j}} w_{ij}\epsilon(c_i)\epsilon(c_j)\right)\phi_c.rb​=c∈BN​∑​(k∈IN​∏​(Vk​)bk​ck​​)exp​ii,j∈IN​i<j​∑​wij​ϵ(ci​)ϵ(cj​)​ϕc​.

For assignments a,ba,ba,b on SSS, let a⊔ea\sqcup ea⊔e denote the full assignment equal to aaa on SSS and to eee on its complement, and set

Rab=(∑c∈BN∣rc∣2)−1∑e:IN∖S→{false,true}ra⊔e rb⊔e‾.R_{ab}= \left(\sum_{c\in\mathcal B_N}|r_c|^2\right)^{-1} \sum_{e:I_N\setminus S\to\{\mathrm{false},\mathrm{true}\}} r_{a\sqcup e}\,\overline{r_{b\sqcup e}}.Rab​=(c∈BN​∑​∣rc​∣2)−1e:IN​∖S→{false,true}∑​ra⊔e​rb⊔e​​.

Define matrices indexed by ID×IDI_D\times I_DID​×ID​ by

Ek(u,v)=Ak(u)⊗Ak(v)‾,Tk(a,b)={Ek(ak,bk),k∈S,∑u∈{false,true}exp⁡ ⁣(iϵ(u)∑j∈Swjk(ϵ(aj)−ϵ(bj)))Ek(u,u),k∉S,E_k(u,v)=A_k(u)\otimes\overline{A_k(v)},\qquad T_k(a,b)= \begin{cases} E_k(a_k,b_k),&k\in S,\\[2mm] \displaystyle\sum_{u\in\{\mathrm{false},\mathrm{true}\}} \exp\!\left(i\epsilon(u)\sum_{j\in S} w_{jk}\bigl(\epsilon(a_j)-\epsilon(b_j)\bigr)\right)E_k(u,u), &k\notin S, \end{cases}Ek​(u,v)=Ak​(u)⊗Ak​(v)​,Tk​(a,b)=⎩⎨⎧​Ek​(ak​,bk​),u∈{false,true}∑​exp​iϵ(u)j∈S∑​wjk​(ϵ(aj​)−ϵ(bj​))​Ek​(u,u),​k∈S,k∈/S,​

where the bar on a matrix means entrywise conjugation, and put Pt(a,b)=T0(a,b)⋯Tt−1(a,b)P_t(a,b)=T_0(a,b)\cdots T_{t-1}(a,b)Pt​(a,b)=T0​(a,b)⋯Tt−1​(a,b), with P0(a,b)P_0(a,b)P0​(a,b) the identity. The predicate holds exactly when there exists a memory function m:N→Cm:\mathbb N\to\mathbb Cm:N→C obtained by successfully executing all scalar instructions, starting with every address zero and writing the result of instruction number qqq to address qqq, such that, writing LLL for the code length,

m(norm⁡)=Z,norm⁡<L,expectation⁡<L,m(expectation⁡)=tr⁡(OR),m(\operatorname{norm})=Z,\qquad \operatorname{norm}<L,\qquad \operatorname{expectation}<L,\qquad m(\operatorname{expectation})=\operatorname{tr}(OR),m(norm)=Z,norm<L,expectation<L,m(expectation)=tr(OR),

and, for every a,ba,ba,b, every 0≤t≤N0\le t\le N0≤t≤N, and every i,j∈ID×IDi,j\in I_D\times I_Di,j∈ID​×ID​,

stage⁡(a,b,t,i,j)<L,m(stage⁡(a,b,t,i,j))=(Pt(a,b))ij,\operatorname{stage}(a,b,t,i,j)<L,\qquad m(\operatorname{stage}(a,b,t,i,j))=(P_t(a,b))_{ij},stage(a,b,t,i,j)<L,m(stage(a,b,t,i,j))=(Pt​(a,b))ij​,

while, for every a,ba,ba,b,

cross⁡(a,b)<L,m(cross⁡(a,b))=tr⁡(PN(a,b)),entry⁡(a,b)<L,m(entry⁡(a,b))=Rab.\operatorname{cross}(a,b)<L,\qquad m(\operatorname{cross}(a,b))=\operatorname{tr}(P_N(a,b)),\qquad \operatorname{entry}(a,b)<L,\qquad m(\operatorname{entry}(a,b))=R_{ab}.cross(a,b)<L,m(cross(a,b))=tr(PN​(a,b)),entry(a,b)<L,m(entry(a,b))=Rab​.

Execution reads tensor entries, complex embeddings of wijw_{ij}wij​, entries of VkV_kVk​, and entries of OOO; constants, addition, multiplication, conjugation, and the operation z↦eiRe⁡zz\mapsto e^{i\operatorname{Re}z}z↦eiRez have their usual meanings; division fails if its denominator is zero; and every external product call returns zero. Operand addresses need not refer to earlier instructions, so an address not yet written still contains zero. No nonzero-vector hypothesis is part of this predicate: the inverse in RRR is defined to be zero when its denominator is zero. Zero dimensions and empty SSS are allowed; empty products are identities, and empty sums are zero.

QAlgorithms.Papers.Independent.Intakethird100.P57.MarginalProgram

For natural numbers N,DN,DN,D, including zero, and a subset S⊆IN={0,…,N−1}S\subseteq I_N=\{0,\ldots,N-1\}S⊆IN​={0,…,N−1}, this defines a record containing a scalar program and several natural-number addresses. The scalar program is a finite list of instructions that may supply a complex constant, read a tensor, phase, rotation, or observable input label, add or multiply values at two natural-number addresses, divide values at two addresses, conjugate a value, form eiRe⁡ze^{i\operatorname{Re}z}eiRez from a value zzz, or call an external function on a family of complex 2×22\times22×2 matrices whose entries are specified by addresses indexed by IN×{false,true}2I_N\times\{\mathrm{false},\mathrm{true}\}^2IN​×{false,true}2. Tensor input labels have indices (k,b,i,j)∈IN×{false,true}×ID2(k,b,i,j)\in I_N\times\{\mathrm{false},\mathrm{true}\}\times I_D^2(k,b,i,j)∈IN​×{false,true}×ID2​; phase labels have two indices in INI_NIN​; rotation labels have one site index and two Boolean indices; observable labels have two Boolean assignments on SSS. The record additionally supplies an address stage⁡(a,b,t,i,j)\operatorname{stage}(a,b,t,i,j)stage(a,b,t,i,j) for every two Boolean assignments a,ba,ba,b on SSS, every integer 0≤t≤N0\le t\le N0≤t≤N, and every i,j∈ID×IDi,j\in I_D\times I_Di,j∈ID​×ID​; addresses cross⁡(a,b)\operatorname{cross}(a,b)cross(a,b) and entry⁡(a,b)\operatorname{entry}(a,b)entry(a,b); and addresses norm⁡\operatorname{norm}norm and expectation⁡\operatorname{expectation}expectation. The record itself imposes no bounds or semantic requirements on these addresses or on instruction operands.

QAlgorithms.Papers.Independent.Intakethird100.P57.PhaseGraph

For any natural number NNN, this defines a structure consisting of real weights wijw_{ij}wij​ for 0≤i,j<N0\le i,j<N0≤i,j<N, together with the requirements that, for every such pair, wij=wjiw_{ij}=w_{ji}wij​=wji​, 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π, and, for every iii, wii=0w_{ii}=0wii​=0. Zero weights are permitted. When N=0N=0N=0, there are no weights and all these requirements are vacuous.

QAlgorithms.Papers.Independent.Intakethird100.P57.QubitCliffordGate.matrix

For every natural number NNN, this maps each gate description—Hadamard at a site, phase at a site, or controlled-XXX on distinct control and target sites—to a complex matrix indexed by Boolean assignments a,b:IN→{false,true}a,b:I_N\to\{\mathrm{false},\mathrm{true}\}a,b:IN​→{false,true}. Writing δuv=1\delta_{uv}=1δuv​=1 when u=vu=vu=v and 000 otherwise, a Hadamard description at qqq has entry

Haqbq∏k≠qδakbk,Huv={−1/2,u=v=true,1/2,otherwise;H_{a_qb_q}\prod_{k\ne q}\delta_{a_kb_k}, \qquad H_{uv}= \begin{cases} -1/\sqrt2,&u=v=\mathrm{true},\\ 1/\sqrt2,&\text{otherwise}; \end{cases}Haq​bq​​k=q∏​δak​bk​​,Huv​={−1/2​,1/2​,​u=v=true,otherwise;​

a phase description at qqq has entry

Saqbq∏k≠qδakbk,S=(100i)S_{a_qb_q}\prod_{k\ne q}\delta_{a_kb_k}, \qquad S= \begin{pmatrix}1&0\\0&i\end{pmatrix}Saq​bq​​k=q∏​δak​bk​​,S=(10​0i​)

in the Boolean ordering false, true; and a controlled-XXX description with control jjj and distinct target kkk has entry 111 exactly when ak=bkxorbja_k=b_k\mathbin{\mathrm{xor}}b_jak​=bk​xorbj​ and aq=bqa_q=b_qaq​=bq​ for every q≠kq\ne kq=k, and entry 000 otherwise. The definition covers N=0N=0N=0, although there are then no gate descriptions to which it can be applied.

QAlgorithms.Papers.Independent.Intakethird100.P57.QubitCliffordGate

For every natural number NNN, this defines a type of gate descriptions with three forms: a Hadamard description carrying a site q∈IN={0,…,N−1}q\in I_N=\{0,\ldots,N-1\}q∈IN​={0,…,N−1}; a phase description carrying a site q∈INq\in I_Nq∈IN​; and a controlled-XXX description carrying control and target sites in INI_NIN​, together with a proof that they are distinct. Thus the controlled-XXX form cannot use the same site twice. For N=0N=0N=0 there are no gate descriptions, and for N=1N=1N=1 there are no controlled-XXX descriptions.

QAlgorithms.Papers.Independent.Intakethird100.P57.RageParameters

For any natural numbers N,DN,DN,D, this defines a parameter record consisting of three fields: a family Ak,bA_{k,b}Ak,b​ of arbitrary complex D×DD\times DD×D matrices indexed by k<Nk<Nk<N and Boolean bbb; a real weight function wjkw_{jk}wjk​ on pairs of sites satisfying symmetry wjk=wkjw_{jk}=w_{kj}wjk​=wkj​, zero diagonal wjj=0w_{jj}=0wjj​=0, and 0≤wjk<2π0\le w_{jk}<2\pi0≤wjk​<2π; and a unitary 2×22\times22×2 complex matrix VkV_kVk​, with Boolean row and column indices, for every site k<Nk<Nk<N. No normalization or nonzero condition is imposed on the matrix family. Zero values of NNN and DDD are permitted: when N=0N=0N=0, all three fields have empty site index sets, and when D=0D=0D=0, the tensor matrices have empty row and column index sets.

QAlgorithms.Papers.Independent.Intakethird100.P57.ScalarInstruction.eval

For every natural number NNN, arbitrary input-label type III, input-data function d:I→Cd:I\to\mathbb Cd:I→C, arbitrary function BBB from families of NNN complex 2×22\times22×2 matrices to C\mathbb CC, and total memory function m:N→Cm:\mathbb N\to\mathbb Cm:N→C, this defines instruction evaluation with an optional complex result. A constant returns its specified value; an input read at iii returns d(i)d(i)d(i); addition and multiplication at addresses a,ba,ba,b return m(a)+m(b)m(a)+m(b)m(a)+m(b) and m(a)m(b)m(a)m(b)m(a)m(b); division returns no result if m(b)=0m(b)=0m(b)=0, and otherwise returns m(a)/m(b)m(a)/m(b)m(a)/m(b); conjugation at aaa returns m(a)‾\overline{m(a)}m(a)​; phase formation at aaa returns eiRe⁡m(a)e^{i\operatorname{Re}m(a)}eiRem(a); and a product call with address function FFF returns B((Mk)k<N)B((M_k)_{k<N})B((Mk​)k<N​), where (Mk)ab=m(F(k,a,b))(M_k)_{ab}=m(F(k,a,b))(Mk​)ab​=m(F(k,a,b)). Every form except division by zero returns a value. Addresses are unrestricted natural numbers, and no property of BBB is assumed; when N=0N=0N=0, a product call applies BBB to the empty matrix family.

QAlgorithms.Papers.Independent.Intakethird100.P57.ScalarInstruction

For every natural number NNN and arbitrary type of input labels III, this defines a type of instructions with nine forms: a complex constant ccc; a read of an input label i∈Ii\in Ii∈I; addition, multiplication, or division specified by two natural-number memory addresses; conjugation or phase formation specified by one natural-number memory address; and a product call specified by a function assigning a natural-number memory address to each triple (k,a,b)(k,a,b)(k,a,b), where k<Nk<Nk<N and a,ba,ba,b are Boolean values. These constructors impose no bounds on memory addresses or requirement that referenced addresses have already been written. The definition allows N=0N=0N=0 and allows the input-label type to be empty.

QAlgorithms.Papers.Independent.Intakethird100.P57.ScalarProgram.calls

For every natural number NNN, arbitrary input-label type III, and scalar program ppp, this defines the number of entries in its instruction list that are product-call instructions, each carrying an address function on triples consisting of a site k<Nk<Nk<N and two Boolean values. All other instruction forms contribute zero. This counts occurrences in the list without executing the program, including occurrences after an instruction that would fail; an empty program has count zero, and N=0N=0N=0 is allowed.

QAlgorithms.Papers.Independent.Intakethird100.P57.ScalarProgram.execute

For every natural number NNN, arbitrary input-label type III, program ppp containing a finite list of scalar instructions, data function d:I→Cd:I\to\mathbb Cd:I→C, and arbitrary function BBB from families of NNN complex 2×22\times22×2 matrices to C\mathbb CC, this defines execution returning either no result or a total memory function N→C\mathbb N\to\mathbb CN→C. Execution starts with instruction counter 000 and every memory address equal to zero, and processes the list in order. At each instruction, using the current memory mmm, constants and input reads yield their specified constant and d(i)d(i)d(i); addition, multiplication, division, and conjugation yield the corresponding operations on the addressed values; phase formation at address aaa yields eiRe⁡m(a)e^{i\operatorname{Re}m(a)}eiRem(a); and a product call with address function FFF yields B((Mk)k<N)B((M_k)_{k<N})B((Mk​)k<N​), where (Mk)ab=m(F(k,a,b))(M_k)_{ab}=m(F(k,a,b))(Mk​)ab​=m(F(k,a,b)). Division fails precisely when its denominator memory value is zero. A successful instruction stores its result at the current counter address and increments the counter; a failure makes the entire execution return no result. On success, only the final memory function is returned. Memory references need not point to earlier instructions: addresses not yet written read as zero. An empty program succeeds with the all-zero memory, and after a successful program of length qqq, every address at least qqq remains zero.

QAlgorithms.Papers.Independent.Intakethird100.P57.ScalarProgram

For every natural number NNN and arbitrary input-label type III, this defines a program as a structure containing a single field: a finite list of scalar instructions. Each instruction is a complex constant, an input read, addition, multiplication, division, conjugation, phase formation, or a call carrying memory addresses for the entries of NNN complex 2×22\times22×2 matrices. The structure imposes no validity conditions, memory-address bounds, designated output address, or requirement that operands refer to earlier instructions. An empty instruction list is permitted, including when N=0N=0N=0 or III is empty.

QAlgorithms.Papers.Independent.Intakethird100.P57.ScalarProgram.work

For every natural number NNN, arbitrary input-label type III, scalar program ppp, and natural number BBB, whose default value is 000, this defines work by summing a cost of 4N+1+B4N+1+B4N+1+B for every product-call instruction and a cost of 111 for every other instruction. Equivalently, if the instruction list has length qqq and contains ccc product-call instructions, the result is q+c(4N+B)q+c(4N+B)q+c(4N+B). The definition counts the entire list without executing it or checking whether execution succeeds. An empty program has work zero; when N=0N=0N=0 and B=0B=0B=0, every instruction has cost 111.

QAlgorithms.Papers.Independent.Intakethird100.P57.SingleEdgeEnergyLaw

For natural numbers N,DN,DN,D supplied with 1≤N1\le N1≤N and 1≤D1\le D1≤D, choose complex D×DD\times DD×D matrices ArsA_r^sArs​, a graph with real weights wrs=wsrw_{rs}=w_{sr}wrs​=wsr​, wrr=0w_{rr}=0wrr​=0, and 0≤wrs<2π0\le w_{rs}<2\pi0≤wrs​<2π, unitary complex 2×22\times22×2 matrices VrV_rVr​, distinct sites j,k<Nj,k<Nj,k<N, and a Hermitian matrix HHH indexed by NNN-bit strings, and assume the vector T(b)=tr⁡(∏r=0N−1Arbr)T(b)=\operatorname{tr}(\prod_{r=0}^{N-1}A_r^{b_r})T(b)=tr(∏r=0N−1​Arbr​​), with increasing site order, is nonzero. Put

Φ(b)=∑r<sbr=bs=1wrs,B(b)=eiΦ(b)−iwjk1{bj=bk=1}T(b),W(b,a)=∏rVr(br,ar).\Phi(b)=\sum_{\substack{r<s\\b_r=b_s=1}}w_{rs},\qquad B(b)=e^{i\Phi(b)-iw_{jk}\mathbf1_{\{b_j=b_k=1\}}}T(b),\qquad W(b,a)=\prod_rV_r(b_r,a_r).Φ(b)=r<sbr​=bs​=1​∑​wrs​,B(b)=eiΦ(b)−iwjk​1{bj​=bk​=1}​T(b),W(b,a)=r∏​Vr​(br​,ar​).

Let uuu equal BBB on strings for which the two selected bits are not both 111, and zero elsewhere, and let vvv equal BBB on the complementary strings and zero elsewhere. Define

c0=Re⁡⟨u,W†HWu⟩+Re⁡⟨v,W†HWv⟩,c1=⟨u,W†HWv⟩,Z=∥T∥2,Ez=W(u+zv),c_0=\operatorname{Re}\langle u,W^\dagger HWu\rangle+ \operatorname{Re}\langle v,W^\dagger HWv\rangle,\quad c_1=\langle u,W^\dagger HWv\rangle,\quad Z=\|T\|^2,\quad E_z=W(u+zv),c0​=Re⟨u,W†HWu⟩+Re⟨v,W†HWv⟩,c1​=⟨u,W†HWv⟩,Z=∥T∥2,Ez​=W(u+zv),

and write RH(ξ)=Re⁡⟨ξ,Hξ⟩/∥ξ∥2R_H(\xi)=\operatorname{Re}\langle\xi,H\xi\rangle/\|\xi\|^2RH​(ξ)=Re⟨ξ,Hξ⟩/∥ξ∥2 and m(c)=1m(c)=1m(c)=1 if c=0c=0c=0, otherwise m(c)=−c‾/∣c∣m(c)=-\overline c/|c|m(c)=−c/∣c∣. The definition is the proposition consisting of the following conjunction:

∀z∈C,∣z∣=1 ⟹ (∥Ez∥2=Z  and  RH(Ez)=c0+2Re⁡(c1z)Z),∣m(c1)∣=1,∀z∈C,∣z∣=1 ⟹ RH(Em(c1))≤RH(Ez),c1=0 ⟹ ∀z∈C,∣z∣=1 ⟹ RH(Ez)=c0Z.\begin{gathered} \forall z\in\mathbb C,\quad |z|=1\ \Longrightarrow\ \left(\|E_z\|^2=Z\ \text{ and }\ R_H(E_z)=\frac{c_0+2\operatorname{Re}(c_1z)}{Z}\right),\\ |m(c_1)|=1,\\ \forall z\in\mathbb C,\quad |z|=1\ \Longrightarrow\ R_H(E_{m(c_1)})\le R_H(E_z),\\ c_1=0\ \Longrightarrow\ \forall z\in\mathbb C,\quad |z|=1\ \Longrightarrow\ R_H(E_z)=\frac{c_0}{Z}. \end{gathered}∀z∈C,∣z∣=1 ⟹ (∥Ez​∥2=Z  and  RH​(Ez​)=Zc0​+2Re(c1​z)​),∣m(c1​)∣=1,∀z∈C,∣z∣=1 ⟹ RH​(Em(c1​)​)≤RH​(Ez​),c1​=0 ⟹ ∀z∈C,∣z∣=1 ⟹ RH​(Ez​)=Zc0​​.​

Here Z>0Z>0Z>0 follows from the supplied nonzero assumption. This declaration defines a proposition; it does not itself assert that the proposition holds. Although the dimension hypothesis states only N≥1N\ge1N≥1, the required distinct sites cannot be supplied when N=1N=1N=1.

QAlgorithms.Papers.Independent.Intakethird100.P57.SiteCoordinates

For every natural number DDD, the abbreviation denotes the set of triples (b,i,j)(b,i,j)(b,i,j), where bbb is Boolean and i,j∈{0,…,D−1}i,j\in\{0,\ldots,D-1\}i,j∈{0,…,D−1}. It has 2D22D^22D2 elements and is empty when D=0D=0D=0.

QAlgorithms.Papers.Independent.Intakethird100.P57.Tensors

For any natural numbers N,DN,DN,D, including zero, this abbreviates the type of families A=(Ak(s))A=(A_k(s))A=(Ak​(s)), where k∈{0,…,N−1}k\in\{0,\ldots,N-1\}k∈{0,…,N−1}, s∈{false,true}s\in\{\mathrm{false},\mathrm{true}\}s∈{false,true}, and each Ak(s)A_k(s)Ak​(s) is a complex D×DD\times DD×D matrix. No conditions are imposed on these matrices. When N=0N=0N=0, the family has no sites; when D=0D=0D=0, each matrix has no entries.

QAlgorithms.Papers.Independent.Intakethird100.P57.bitReal

For every Boolean value bbb, define its real-valued representative by

bitReal⁡(b)={1,b=true,0,b=false.\operatorname{bitReal}(b)= \begin{cases} 1,&b=\mathrm{true},\\ 0,&b=\mathrm{false}. \end{cases}bitReal(b)={1,0,​b=true,b=false.​

QAlgorithms.Papers.Independent.Intakethird100.P57.cliffordMatrix

For every natural number NNN and finite list of gate descriptions [g0,…,gℓ−1][g_0,\ldots,g_{\ell-1}][g0​,…,gℓ−1​], this defines the complex matrix on Boolean assignments to IN={0,…,N−1}I_N=\{0,\ldots,N-1\}IN​={0,…,N−1} to be

Mgℓ−1⋯Mg1Mg0.M_{g_{\ell-1}}\cdots M_{g_1}M_{g_0}.Mgℓ−1​​⋯Mg1​​Mg0​​.

Here a Hadamard gate at qqq applies 12(111−1)\frac1{\sqrt2}\begin{pmatrix}1&1\\1&-1\end{pmatrix}2​1​(11​1−1​) at qqq and identities elsewhere; a phase gate at qqq applies diag⁡(1,i)\operatorname{diag}(1,i)diag(1,i) at qqq and identities elsewhere; and a controlled-XXX gate on distinct control jjj and target kkk is the permutation matrix sending an input assignment bbb to the assignment with target bit bkxorbjb_k\mathbin{\mathrm{xor}}b_jbk​xorbj​ and all other bits unchanged. Boolean matrix indices are ordered false, true. An empty list gives the identity matrix, including when N=0N=0N=0, when the assignment space has one element and every such list is empty.

QAlgorithms.Papers.Independent.Intakethird100.P57.connectedZ

For every natural number NNN, every complex vector vvv indexed by bit strings b∈{0,1}Nb\in\{0,1\}^Nb∈{0,1}N, and any sites i,j∈{0,…,N−1}i,j\in\{0,\ldots,N-1\}i,j∈{0,…,N−1}, define

connectedZ⁡(v,i,j)=∑b(−1)bi+bj∣v(b)∣2−(∑b(−1)bi∣v(b)∣2)(∑b(−1)bj∣v(b)∣2).\operatorname{connectedZ}(v,i,j) = \sum_b(-1)^{b_i+b_j}|v(b)|^2 - \left(\sum_b(-1)^{b_i}|v(b)|^2\right) \left(\sum_b(-1)^{b_j}|v(b)|^2\right).connectedZ(v,i,j)=b∑​(−1)bi​+bj​∣v(b)∣2−(b∑​(−1)bi​∣v(b)∣2)(b∑​(−1)bj​∣v(b)∣2).

There is no normalization assumption on vvv, and iii and jjj may coincide; when i=ji=ji=j, this expression is ∑b∣v(b)∣2−(∑b(−1)bi∣v(b)∣2)2\sum_b|v(b)|^2-\bigl(\sum_b(-1)^{b_i}|v(b)|^2\bigr)^2∑b​∣v(b)∣2−(∑b​(−1)bi​∣v(b)∣2)2. For N=0N=0N=0, there are no choices of iii or jjj.

QAlgorithms.Papers.Independent.Intakethird100.P57.contractionData

For natural numbers N,DN,DN,D, a subset S⊆IN={0,…,N−1}S\subseteq I_N=\{0,\ldots,N-1\}S⊆IN​={0,…,N−1}, arbitrary complex D×DD\times DD×D matrices Ak(b)A_k(b)Ak​(b) for each site k∈INk\in I_Nk∈IN​ and Boolean bbb, a real weight function w:IN×IN→Rw:I_N\times I_N\to\mathbb Rw:IN​×IN​→R satisfying wij=wjiw_{ij}=w_{ji}wij​=wji​, wii=0w_{ii}=0wii​=0, and 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π, a unitary complex 2×22\times22×2 matrix VkV_kVk​ at each site, and an arbitrary complex matrix OOO indexed by Boolean assignments on SSS, this defines a complex-valued function on four kinds of input labels: a tensor label (k,b,i,j)(k,b,i,j)(k,b,i,j) returns (Ak(b))ij(A_k(b))_{ij}(Ak​(b))ij​; a phase label (i,j)(i,j)(i,j) returns the real number wijw_{ij}wij​, regarded as complex; a rotation label (k,a,b)(k,a,b)(k,a,b) returns (Vk)ab(V_k)_{ab}(Vk​)ab​; and an observable label (a,b)(a,b)(a,b) returns OabO_{ab}Oab​. No normalization of the tensors or Hermiticity of OOO is required, and N,DN,DN,D may be zero.

QAlgorithms.Papers.Independent.Intakethird100.P57.controlledPhaseAction

For every natural number NNN, any two sites j,k∈{0,…,N−1}j,k\in\{0,\ldots,N-1\}j,k∈{0,…,N−1}, any complex number zzz, and any complex Euclidean vector vvv indexed by Boolean assignments on the sites, the definition gives a vector uuu with amplitudes

ub={z vb,bj=bk=1,vb,otherwise.u_b= \begin{cases} z\,v_b,&b_j=b_k=1,\\ v_b,&\text{otherwise}. \end{cases}ub​={zvb​,vb​,​bj​=bk​=1,otherwise.​

There is no requirement that j≠kj\ne kj=k, that ∣z∣=1|z|=1∣z∣=1, or that vvv be normalized or nonzero. When j=kj=kj=k, the condition is simply bj=1b_j=1bj​=1; when N=0N=0N=0, no sites j,kj,kj,k can be supplied.

QAlgorithms.Papers.Independent.Intakethird100.P57.crossMarginal

For any natural numbers N,DN,DN,D, complex D×DD\times DD×D matrices Ak(t)A_k(t)Ak​(t) indexed by sites and bits, real weights wjkw_{j k}wjk​ satisfying symmetry, zero diagonal, and 0≤wjk<2π0\le w_{j k}<2\pi0≤wjk​<2π, and a finite subset S⊆{0,…,N−1}S\subseteq\{0,\ldots,N-1\}S⊆{0,…,N−1}, define a complex matrix CCC whose rows and columns are bit assignments a,b:S→{0,1}a,b:S\to\{0,1\}a,b:S→{0,1} by

Ca,b=tr⁡ ⁣(T0a,b⋯TN−1a,b),Tka,b={Ak(ak)⊗Ak(bk)‾,k∈S,∑t∈{0,1}e it∑j∈Swjk(aj−bj)(Ak(t)⊗Ak(t)‾),k∉S.C_{a,b}=\operatorname{tr}\!\left(T_0^{a,b}\cdots T_{N-1}^{a,b}\right), \qquad T_k^{a,b}= \begin{cases} A_k(a_k)\otimes\overline{A_k(b_k)},&k\in S,\\[2mm] \displaystyle\sum_{t\in\{0,1\}} e^{\,\mathrm{i}t\sum_{j\in S}w_{j k}(a_j-b_j)} \bigl(A_k(t)\otimes\overline{A_k(t)}\bigr),&k\notin S. \end{cases}Ca,b​=tr(T0a,b​⋯TN−1a,b​),Tka,b​=⎩⎨⎧​Ak​(ak​)⊗Ak​(bk​)​,t∈{0,1}∑​eit∑j∈S​wjk​(aj​−bj​)(Ak​(t)⊗Ak​(t)​),​k∈S,k∈/S.​

Bits in the exponential mean 000 or 111, conjugation is entrywise, (B⊗C‾)(p,q),(r,s)=Bp,rCq,s‾(B\otimes\overline C)_{(p,q),(r,s)}=B_{p,r}\overline{C_{q,s}}(B⊗C)(p,q),(r,s)​=Bp,r​Cq,s​​, and the product is taken in increasing site order. This definition includes S=∅S=\varnothingS=∅, when there is one row and one column. For N=0N=0N=0, the product is the identity on the D2D^2D2 pair indices, so that sole entry is D2D^2D2; for D=0D=0D=0, every entry is 000.

QAlgorithms.Papers.Independent.Intakethird100.P57.cyclicBlock

For natural numbers N,ℓN,\ellN,ℓ and a starting index s∈{0,…,N−1}s\in\{0,\ldots,N-1\}s∈{0,…,N−1}, this defines the finite set

{i∈{0,…,N−1}:∃t∈N, t<ℓ and i=(s+t) mod N}.\left\{i\in\{0,\ldots,N-1\}:\exists t\in\mathbb N,\ t<\ell\ \text{and}\ i=(s+t)\bmod N\right\}.{i∈{0,…,N−1}:∃t∈N, t<ℓ and i=(s+t)modN}.

Repeated visits contribute only one element. In particular, the set is empty when ℓ=0\ell=0ℓ=0, and it contains all NNN indices when ℓ≥N\ell\ge Nℓ≥N. Supplying a starting index requires N>0N>0N>0; there is no starting index when N=0N=0N=0.

QAlgorithms.Papers.Independent.Intakethird100.P57.describe

For any natural numbers N,DN,DN,D and any parameter record p=(A,w,V)p=(A,w,V)p=(A,w,V), where Ak,bA_{k,b}Ak,b​ are complex D×DD\times DD×D matrices, www is a symmetric real weight function with zero diagonal and 0≤wjk<2π0\le w_{jk}<2\pi0≤wjk​<2π, and each VkV_kVk​ is a unitary Boolean-indexed 2×22\times22×2 complex matrix, this defines a real-valued function on a disjoint union of tensor-entry indices, strictly ordered site pairs, and rotation-entry indices. At a tensor-entry index (k,b,i,j,part)(k,b,i,j,\mathrm{part})(k,b,i,j,part), its value is Re⁡(Ak,b)ij\operatorname{Re}(A_{k,b})_{ij}Re(Ak,b​)ij​ if part=false\mathrm{part}=\mathrm{false}part=false, and Im⁡(Ak,b)ij\operatorname{Im}(A_{k,b})_{ij}Im(Ak,b​)ij​ if part=true\mathrm{part}=\mathrm{true}part=true. At a site-pair index (j,k)(j,k)(j,k) with j<kj<kj<k, its value is wjkw_{jk}wjk​. At a rotation-entry index (k,b,c,part)(k,b,c,\mathrm{part})(k,b,c,part), its value is Re⁡(Vk)bc\operatorname{Re}(V_k)_{bc}Re(Vk​)bc​ if part=false\mathrm{part}=\mathrm{false}part=false, and Im⁡(Vk)bc\operatorname{Im}(V_k)_{bc}Im(Vk​)bc​ if part=true\mathrm{part}=\mathrm{true}part=true. All sites lie below NNN, tensor row and column indices lie below DDD, and the remaining indices are Booleans. Zero dimensions are allowed; the function has an empty domain when N=0N=0N=0, and has no tensor-entry coordinates when D=0D=0D=0.

QAlgorithms.Papers.Independent.Intakethird100.P57.diagonalTensors

For arbitrary natural numbers N,mN,mN,m, coefficients ct∈Cc_t\in\mathbb Cct​∈C indexed by t<mt<mt<m, and complex numbers r(t,k,b)r(t,k,b)r(t,k,b) indexed by t<mt<mt<m, k<Nk<Nk<N, and Boolean bbb, this defines a family of m×mm\times mm×m matrices Ak,bA_{k,b}Ak,b​ whose entries are

(Ak,b)s,t={ct r(t,k,b),s=t and k=0,r(t,k,b),s=t and k≠0,0,s≠t.(A_{k,b})_{s,t}= \begin{cases} c_t\,r(t,k,b),&s=t\text{ and }k=0,\\ r(t,k,b),&s=t\text{ and }k\ne0,\\ 0,&s\ne t. \end{cases}(Ak,b​)s,t​=⎩⎨⎧​ct​r(t,k,b),r(t,k,b),0,​s=t and k=0,s=t and k=0,s=t.​

No positivity or normalization is required. When N=0N=0N=0, there are no site matrices; when m=0m=0m=0, every site matrix has an empty row and column index set.

QAlgorithms.Papers.Independent.Intakethird100.P57.edgeBackground

For all natural numbers N,DN,DN,D, let Ai(t)A_i(t)Ai​(t) be arbitrary complex D×DD\times DD×D matrices indexed by sites and Boolean values, and let GGG specify real weights wiℓw_{i\ell}wiℓ​ satisfying wiℓ=wℓiw_{i\ell}=w_{\ell i}wiℓ​=wℓi​, wii=0w_{ii}=0wii​=0, and 0≤wiℓ<2π0\le w_{i\ell}<2\pi0≤wiℓ​<2π. Given any sites j,kj,kj,k, the definition gives the complex Euclidean vector uuu, indexed by Boolean assignments bbb on all sites, with amplitudes

ub=exp⁡ ⁣(i[∑i<ℓwiℓbibℓ−wjkbjbk])tr⁡ ⁣(A0(b0)⋯AN−1(bN−1)),u_b= \exp\!\left( \mathrm i\left[\sum_{i<\ell}w_{i\ell}b_i b_\ell-w_{jk}b_jb_k\right] \right) \operatorname{tr}\!\left(A_0(b_0)\cdots A_{N-1}(b_{N-1})\right),ub​=exp(i[i<ℓ∑​wiℓ​bi​bℓ​−wjk​bj​bk​])tr(A0​(b0​)⋯AN−1​(bN−1​)),

where Boolean values are identified with 0,10,10,1. No local rotation matrices, normalization, or nonzero hypothesis occur. The sites need not be distinct; when j=kj=kj=k, wjj=0w_{jj}=0wjj​=0, so the subtracted term is zero. The definition permits D=0D=0D=0, in which case the traces and vector are zero; when N=0N=0N=0, no sites j,kj,kj,k exist.

QAlgorithms.Papers.Independent.Intakethird100.P57.edgeCoefficients

For natural numbers N,DN,DN,D, choose complex D×DD\times DD×D matrices ArsA_r^sArs​ for every site r<Nr<Nr<N and bit sss, real graph weights wrs=wsrw_{rs}=w_{sr}wrs​=wsr​ with wrr=0w_{rr}=0wrr​=0 and 0≤wrs<2π0\le w_{rs}<2\pi0≤wrs​<2π, unitary complex 2×22\times22×2 matrices VrV_rVr​, sites j,k<Nj,k<Nj,k<N, and an arbitrary complex matrix HHH indexed by NNN-bit strings. Set

T(b)=tr⁡ ⁣(∏r=0N−1Arbr),Φ(b)=∑r<sbr=bs=1wrs,B(b)=eiΦ(b)−iwjk1{bj=bk=1}T(b),T(b)=\operatorname{tr}\!\left(\prod_{r=0}^{N-1}A_r^{b_r}\right),\qquad \Phi(b)=\sum_{\substack{r<s\\b_r=b_s=1}}w_{rs},\qquad B(b)=e^{i\Phi(b)-iw_{jk}\mathbf1_{\{b_j=b_k=1\}}}T(b),T(b)=tr(r=0∏N−1​Arbr​​),Φ(b)=r<sbr​=bs​=1​∑​wrs​,B(b)=eiΦ(b)−iwjk​1{bj​=bk​=1}​T(b),

where the matrix product is in increasing site order. Define W(b,a)=∏rVr(br,ar)W(b,a)=\prod_rV_r(b_r,a_r)W(b,a)=∏r​Vr​(br​,ar​), HV=W†HWH_V=W^\dagger HWHV​=W†HW, and vectors u,vu,vu,v by u(b)=B(b)u(b)=B(b)u(b)=B(b) when bj,bkb_j,b_kbj​,bk​ are not both 111, and u(b)=0u(b)=0u(b)=0 otherwise, while v(b)=B(b)v(b)=B(b)v(b)=B(b) when both bits are 111, and v(b)=0v(b)=0v(b)=0 otherwise. The definition returns the real–complex pair

(Re⁡⟨u,HVu⟩+Re⁡⟨v,HVv⟩,  ⟨u,HVv⟩).\left( \operatorname{Re}\langle u,H_Vu\rangle+ \operatorname{Re}\langle v,H_Vv\rangle,\; \langle u,H_Vv\rangle \right).(Re⟨u,HV​u⟩+Re⟨v,HV​v⟩,⟨u,HV​v⟩).

No Hermitian assumption on HHH, distinctness assumption on j,kj,kj,k, or normalization or nonzero assumption on TTT is imposed; D=0D=0D=0 is included, whereas N=0N=0N=0 supplies no required sites.

QAlgorithms.Papers.Independent.Intakethird100.P57.edgeData

For arbitrary natural numbers N,D,mN,D,mN,D,m, finite supports Sr⊆{0,…,N−1}S_r\subseteq\{0,\ldots,N-1\}Sr​⊆{0,…,N−1} for 0≤r<m0\le r<m0≤r<m, a family Ak,bA_{k,b}Ak,b​ of complex D×DD\times DD×D matrices for sites 0≤k<N0\le k<N0≤k<N and Boolean values bbb, a real weight array www satisfying wij=wjiw_{ij}=w_{ji}wij​=wji​, wii=0w_{ii}=0wii​=0, and 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π, a family of unitary complex 2×22\times22×2 matrices VkV_kVk​, and arbitrary complex matrices TrT_rTr​ indexed by Boolean assignments on SrS_rSr​, this defines a complex-valued function on the four kinds of edge-input labels: a tensor label (k,b,i,j)(k,b,i,j)(k,b,i,j) returns (Ak,b)i,j(A_{k,b})_{i,j}(Ak,b​)i,j​; a phase label (i,j)(i,j)(i,j) returns wijw_{ij}wij​ viewed as a complex number; a rotation label (k,a,b)(k,a,b)(k,a,b) returns (Vk)a,b(V_k)_{a,b}(Vk​)a,b​; and a term label (r,a,b)(r,a,b)(r,a,b) returns (Tr)a,b(T_r)_{a,b}(Tr​)a,b​. No nonzero or normalization condition is imposed on AAA, and no Hermitian condition is imposed on the terms. All three size parameters may be zero, with labels requiring an unavailable index absent.

QAlgorithms.Papers.Independent.Intakethird100.P57.edgePart

For every natural number NNN, any complex Euclidean vector vvv indexed by Boolean assignments on NNN sites, any sites j,kj,kj,k, and any Boolean value on\mathrm{on}on, the definition gives the vector uuu with amplitudes

ub={vb,(bj∧bk)=on,0,(bj∧bk)≠on.u_b= \begin{cases} v_b,&(b_j\land b_k)=\mathrm{on},\\ 0,&(b_j\land b_k)\ne\mathrm{on}. \end{cases}ub​={vb​,0,​(bj​∧bk​)=on,(bj​∧bk​)=on.​

Thus on=1\mathrm{on}=1on=1 retains precisely assignments with both selected bits equal to 111, while on=0\mathrm{on}=0on=0 retains precisely assignments where at least one selected bit is 000. No normalization or nonzero assumption is imposed, and the retained vector is not rescaled. The sites may coincide, in which case the retained condition is bj=onb_j=\mathrm{on}bj​=on; for N=0N=0N=0, no sites j,kj,kj,k can be supplied.

QAlgorithms.Papers.Independent.Intakethird100.P57.edgeTrial

For natural numbers N,DN,DN,D, let ArsA_r^sArs​ be a complex D×DD\times DD×D matrix for each site r∈{0,…,N−1}r\in\{0,\ldots,N-1\}r∈{0,…,N−1} and bit s∈{0,1}s\in\{0,1\}s∈{0,1}; let GGG have real weights wrsw_{rs}wrs​ satisfying wrs=wsrw_{rs}=w_{sr}wrs​=wsr​, wrr=0w_{rr}=0wrr​=0, and 0≤wrs<2π0\le w_{rs}<2\pi0≤wrs​<2π; and let VrV_rVr​ be a unitary complex 2×22\times22×2 matrix at every site. For sites j,kj,kj,k and any z∈Cz\in\mathbb Cz∈C, define

T(b)=tr⁡ ⁣(A0b0⋯AN−1bN−1),Φ(b)=∑r<sbr=bs=1wrs,B(b)=eiΦ(b){e−iwjkT(b),bj=bk=1,T(b),otherwise.T(b)=\operatorname{tr}\!\left(A_0^{b_0}\cdots A_{N-1}^{b_{N-1}}\right),\qquad \Phi(b)=\sum_{\substack{r<s\\b_r=b_s=1}}w_{rs},\qquad B(b)=e^{i\Phi(b)} \begin{cases} e^{-iw_{jk}}T(b),&b_j=b_k=1,\\ T(b),&\text{otherwise}. \end{cases}T(b)=tr(A0b0​​⋯AN−1bN−1​​),Φ(b)=r<sbr​=bs​=1​∑​wrs​,B(b)=eiΦ(b){e−iwjk​T(b),T(b),​bj​=bk​=1,otherwise.​

The defined vector, indexed by bit strings b∈{0,1}Nb\in\{0,1\}^Nb∈{0,1}N, has amplitudes

edgeTrial⁡(b)=∑a∈{0,1}N(∏r=0N−1Vr(br,ar)){zB(a),aj=ak=1,B(a),otherwise.\operatorname{edgeTrial}(b)= \sum_{a\in\{0,1\}^N} \left(\prod_{r=0}^{N-1}V_r(b_r,a_r)\right) \begin{cases} zB(a),&a_j=a_k=1,\\ B(a),&\text{otherwise}. \end{cases}edgeTrial(b)=a∈{0,1}N∑​(r=0∏N−1​Vr​(br​,ar​)){zB(a),B(a),​aj​=ak​=1,otherwise.​

There is no requirement that j≠kj\ne kj=k, that ∣z∣=1|z|=1∣z∣=1, or that TTT be normalized or nonzero. The dimension D=0D=0D=0 is allowed; N=0N=0N=0 admits no choices of the required sites j,kj,kj,k.

QAlgorithms.Papers.Independent.Intakethird100.P57.emptyPhaseGraph

For every natural number NNN, including zero, this defines real weights wij=0w_{ij}=0wij​=0 for all 0≤i,j<N0\le i,j<N0≤i,j<N, together with proofs that the weights are symmetric, have zero diagonal, and satisfy 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π. When N=0N=0N=0, the weight function has no arguments and these requirements are vacuous.

QAlgorithms.Papers.Independent.Intakethird100.P57.enhance

For any natural number NNN, real weights wrsw_{rs}wrs​ on the sites 0,…,N−10,\ldots,N-10,…,N−1 satisfying wrs=wsrw_{rs}=w_{sr}wrs​=wsr​, wrr=0w_{rr}=0wrr​=0, and 0≤wrs<2π0\le w_{rs}<2\pi0≤wrs​<2π, any family of unitary complex Boolean-indexed matrices VkV_kVk​, and any vector vvv in the complex Euclidean space indexed by NNN-bit strings, this defines a vector with coordinates

(enhance⁡(w,V,v))a=∑b:{0,…,N−1}→{false,true}(∏k=0N−1(Vk)ak,bk)exp⁡ ⁣(i ⁣∑0≤r<s<Nbr=true, bs=truewrs)vb.(\operatorname{enhance}(w,V,v))_a =\sum_{b:\{0,\ldots,N-1\}\to\{\mathrm{false},\mathrm{true}\}} \left(\prod_{k=0}^{N-1}(V_k)_{a_k,b_k}\right) \exp\!\left(\mathrm{i}\! \sum_{\substack{0\le r<s<N\\ b_r=\mathrm{true},\ b_s=\mathrm{true}}}w_{rs}\right)v_b.(enhance(w,V,v))a​=b:{0,…,N−1}→{false,true}∑​(k=0∏N−1​(Vk​)ak​,bk​​)exp​i0≤r<s<Nbr​=true, bs​=true​∑​wrs​​vb​.

No normalization or nonzero condition is imposed on vvv. For N=0N=0N=0, the sole coordinate is unchanged.

QAlgorithms.Papers.Independent.Intakethird100.P57.enhancementData

For any natural number NNN, subset S⊆IN={0,…,N−1}S\subseteq I_N=\{0,\ldots,N-1\}S⊆IN​={0,…,N−1}, real weight function w:IN×IN→Rw:I_N\times I_N\to\mathbb Rw:IN​×IN​→R satisfying wij=wjiw_{ij}=w_{ji}wij​=wji​, wii=0w_{ii}=0wii​=0, and 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π, unitary complex 2×22\times22×2 matrices VkV_kVk​ for k∈INk\in I_Nk∈IN​, and arbitrary complex matrix OOO indexed by Boolean assignments on SSS, this defines a complex-valued function on input labels: a phase label (i,j)(i,j)(i,j) returns wijw_{ij}wij​, regarded as a complex number; a rotation label (k,a,b)(k,a,b)(k,a,b) returns (Vk)ab(V_k)_{ab}(Vk​)ab​; and an observable label (a,b)(a,b)(a,b) returns OabO_{ab}Oab​. No Hermiticity or positivity of OOO is assumed. Empty SSS and N=0N=0N=0 are allowed; when N=0N=0N=0, the function has only the single observable input label.

QAlgorithms.Papers.Independent.Intakethird100.P57.etaAmplitude

For every complex number ddd and Boolean bbb, this defines the complex number

η(d,b)={ed,b=true,1,b=false.\eta(d,b)= \begin{cases} e^d,&b=\mathrm{true},\\ 1,&b=\mathrm{false}. \end{cases}η(d,b)={ed,1,​b=true,b=false.​

There is no restriction on ddd.

QAlgorithms.Papers.Independent.Intakethird100.P57.firstBlock

For any natural numbers N,LN,LN,L, define the finite set

firstBlock⁡(N,L)={i∈{0,…,N−1}:i<L}.\operatorname{firstBlock}(N,L)=\{i\in\{0,\ldots,N-1\}:i<L\}.firstBlock(N,L)={i∈{0,…,N−1}:i<L}.

Thus it contains the first min⁡(N,L)\min(N,L)min(N,L) sites; it is empty if N=0N=0N=0 or L=0L=0L=0, and it contains every site if L≥NL\ge NL≥N.

QAlgorithms.Papers.Independent.Intakethird100.P57.graphAngle

For any type ι\iotaι equipped with a finite enumeration and a linear order, any real function w:ι×ι→Rw:\iota\times\iota\to\mathbb Rw:ι×ι→R, and any Boolean assignment b:ι→{false,true}b:\iota\to\{\mathrm{false},\mathrm{true}\}b:ι→{false,true}, this defines the real number

∑i,j∈ιi<j, bi=true, bj=truewij.\sum_{\substack{i,j\in\iota\\ i<j,\ b_i=\mathrm{true},\ b_j=\mathrm{true}}}w_{ij}.i,j∈ιi<j, bi​=true, bj​=true​∑​wij​.

Only strictly ordered pairs contribute; no symmetry, sign, diagonal, or boundedness conditions are imposed on www. If there are no contributing pairs, including when ι\iotaι is empty, the value is zero.

QAlgorithms.Papers.Independent.Intakethird100.P57.graphOp

For any type ι\iotaι equipped with a finite enumeration and a linear order, and any real function w:ι×ι→Rw:\iota\times\iota\to\mathbb Rw:ι×ι→R, this defines the complex diagonal matrix indexed by Boolean assignments a,b:ι→{false,true}a,b:\iota\to\{\mathrm{false},\mathrm{true}\}a,b:ι→{false,true}, whose entries are

Ga,b={exp⁡ ⁣(i ⁣∑r,s∈ιr<s, br=true, bs=truewrs),a=b,0,a≠b.G_{a,b}= \begin{cases} \displaystyle \exp\!\left(\mathrm{i}\! \sum_{\substack{r,s\in\iota\\ r<s,\ b_r=\mathrm{true},\ b_s=\mathrm{true}}}w_{rs}\right),&a=b,\\ 0,&a\ne b. \end{cases}Ga,b​=⎩⎨⎧​exp​ir,s∈ιr<s, br​=true, bs​=true​∑​wrs​​,0,​a=b,a=b.​

No symmetry, sign, or boundedness condition is required of www. If ι\iotaι is empty, this is the one-entry matrix with entry 111.

QAlgorithms.Papers.Independent.Intakethird100.P57.hadamardMatrix

This defines a complex matrix with rows and columns indexed by Booleans whose (a,b)(a,b)(a,b)-entry is −1/2-1/\sqrt2−1/2​ if both aaa and bbb are true, and 1/21/\sqrt21/2​ otherwise. In the ordering false, true, it is

12(111−1).\frac1{\sqrt2} \begin{pmatrix} 1&1\\ 1&-1 \end{pmatrix}.2​1​(11​1−1​).

QAlgorithms.Papers.Independent.Intakethird100.P57.joinBits

For every natural number NNN, every finite set S⊆{0,…,N−1}S\subseteq\{0,\ldots,N-1\}S⊆{0,…,N−1}, every Boolean assignment aaa on SSS, and every Boolean assignment eee on its complement, this defines the full NNN-bit string JS(a,e)J_S(a,e)JS​(a,e) by

JS(a,e)k={ak,k∈S,ek,k∉S.J_S(a,e)_k= \begin{cases} a_k,&k\in S,\\ e_k,&k\notin S. \end{cases}JS​(a,e)k​={ak​,ek​,​k∈S,k∈/S.​

The empty set and the full site set are allowed: in those cases the result uses only eee or only aaa, respectively. When N=0N=0N=0, the result is the unique empty bit string.

QAlgorithms.Papers.Independent.Intakethird100.P57.localGate

For a natural number NNN, a site q<Nq<Nq<N, and a unitary complex 2×22\times22×2 matrix UUU, this defines the matrix indexed by NNN-bit strings a,ba,ba,b with entries

localGate⁡(b,a)=U(bq,aq)∏r<Nr≠q{1,br=ar,0,br≠ar.\operatorname{localGate}(b,a) = U(b_q,a_q)\prod_{\substack{r<N\\r\ne q}} \begin{cases} 1,&b_r=a_r,\\ 0,&b_r\ne a_r. \end{cases}localGate(b,a)=U(bq​,aq​)r<Nr=q​∏​{1,0,​br​=ar​,br​=ar​.​

Thus it is the product of the matrix UUU at site qqq and identity matrices at every other site. The required site qqq cannot be supplied when N=0N=0N=0.

QAlgorithms.Papers.Independent.Intakethird100.P57.localTangent

For every natural number NNN and arbitrary families V,V˙V,\dot VV,V˙ of complex 2×22\times22×2 matrices indexed by sites k<Nk<Nk<N, this defines a matrix indexed by bit strings a,b∈{0,1}Na,b\in\{0,1\}^Na,b∈{0,1}N, with entries

∑k=0N−1∏l=0N−1{(V˙l)albl,l=k,(Vl)albl,l≠k.\sum_{k=0}^{N-1}\prod_{l=0}^{N-1} \begin{cases} (\dot V_l)_{a_l b_l},&l=k,\\ (V_l)_{a_l b_l},&l\ne k. \end{cases}k=0∑N−1​l=0∏N−1​{(V˙l​)al​bl​​,(Vl​)al​bl​​,​l=k,l=k.​

Neither unitarity nor a derivative relation between the two families is assumed. When N=0N=0N=0, the sum is empty, so this is the zero matrix on the singleton set of empty bit strings.

QAlgorithms.Papers.Independent.Intakethird100.P57.localTermHamiltonian

For arbitrary natural numbers N,mN,mN,m, a family of finite site sets Sr⊆{0,…,N−1}S_r\subseteq\{0,\ldots,N-1\}Sr​⊆{0,…,N−1} indexed by r∈{0,…,m−1}r\in\{0,\ldots,m-1\}r∈{0,…,m−1}, and arbitrary complex matrices TrT_rTr​ indexed by pairs of Boolean assignments on SrS_rSr​, this definition gives the complex matrix HHH indexed by Boolean strings of length NNN whose entries are Ha,b=∑r=0m−1T~r;a,bH_{a,b}=\sum_{r=0}^{m-1}\widetilde T_{r;a,b}Ha,b​=∑r=0m−1​Tr;a,b​, where T~r;a,b=(Tr)a∣Sr,b∣Sr\widetilde T_{r;a,b}=(T_r)_{a|_{S_r},b|_{S_r}}Tr;a,b​=(Tr​)a∣Sr​​,b∣Sr​​​ if aaa and bbb agree at every site outside SrS_rSr​, and T~r;a,b=0\widetilde T_{r;a,b}=0Tr;a,b​=0 otherwise. There are no Hermitian, positivity, normalization, or support-size assumptions. When m=0m=0m=0, the sum is the zero matrix; when Sr=∅S_r=\varnothingSr​=∅, its matrix has one entry and its extension is that entry times the identity. The definition also permits N=0N=0N=0.

QAlgorithms.Papers.Independent.Intakethird100.P57.minimizingPhase

For every complex number ccc, this defines the complex number

minimizingPhase⁡(c)={1,c=0,−c‾∣c∣,c≠0,\operatorname{minimizingPhase}(c)= \begin{cases} 1,&c=0,\\[2pt] -\dfrac{\overline c}{|c|},&c\ne0, \end{cases}minimizingPhase(c)=⎩⎨⎧​1,−∣c∣c​,​c=0,c=0,​

where the real modulus in the denominator is regarded as a complex number. The zero case is explicitly assigned the value 111.

QAlgorithms.Papers.Independent.Intakethird100.P57.mpsTangent

For arbitrary natural numbers N,DN,DN,D and two families A,A˙A,\dot AA,A˙ assigning a complex D×DD\times DD×D matrix to each site k<Nk<Nk<N and Boolean value, this defines a vector indexed by bit strings b∈{0,1}Nb\in\{0,1\}^Nb∈{0,1}N, with amplitudes

∑k=0N−1tr⁡ ⁣(∏l=0N−1{A˙l(bl),l=k,Al(bl),l≠k),\sum_{k=0}^{N-1}\operatorname{tr}\!\left( \prod_{l=0}^{N-1} \begin{cases} \dot A_l(b_l),&l=k,\\ A_l(b_l),&l\ne k \end{cases}\right),k=0∑N−1​tr(l=0∏N−1​{A˙l​(bl​),Al​(bl​),​l=k,l=k​),

where matrix factors occur in increasing site order. No relation between AAA and A˙\dot AA˙, such as being values and derivatives of a path, is required. For N=0N=0N=0 the sum is empty and the vector is zero; for D=0D=0D=0 every trace is zero, so the vector is also zero.

QAlgorithms.Papers.Independent.Intakethird100.P57.nextSite

For every natural number NNN and every site i∈{0,…,N−1}i\in\{0,\ldots,N-1\}i∈{0,…,N−1}, define nextSite⁡(i)\operatorname{nextSite}(i)nextSite(i) to be the site whose index is

(i+1) mod N.(i+1)\bmod N.(i+1)modN.

The existence of iii ensures N>0N>0N>0, so the remainder is a valid site. This sends N−1N-1N−1 to 000; for N=1N=1N=1, it fixes the sole site, and for N=0N=0N=0, there are no inputs.

QAlgorithms.Papers.Independent.Intakethird100.P57.normalizeRageVector

For any type ι\iotaι equipped with a finite enumeration and any vector v∈Cιv\in\mathbb C^\iotav∈Cι with its Euclidean norm, this defines

(∥v∥:C)−1v.(\|v\|:\mathbb C)^{-1}v.(∥v∥:C)−1v.

There is no assumption that v≠0v\ne0v=0. For nonzero vvv, the expression divides vvv by its norm; for v=0v=0v=0, it is zero because the inverse of zero is defined to be zero. In particular, an empty index type yields the zero vector.

QAlgorithms.Papers.Independent.Intakethird100.P57.oppositeWeights

For every natural number LLL, this defines a real-valued function on ordered pairs i,j∈{0,…,2L−1}i,j\in\{0,\ldots,2L-1\}i,j∈{0,…,2L−1} by

oppositeWeights⁡(L)(i,j)={π,i≠j and (i+L) mod (2L)=j,0,otherwise.\operatorname{oppositeWeights}(L)(i,j)= \begin{cases} \pi,&i\ne j\text{ and }(i+L)\bmod(2L)=j,\\ 0,&\text{otherwise}. \end{cases}oppositeWeights(L)(i,j)={π,0,​i=j and (i+L)mod(2L)=j,otherwise.​

In particular, diagonal entries receive 000. The case L=0L=0L=0 is included as a function on an empty set of pairs, so there are no entries at which the remainder expression is evaluated.

QAlgorithms.Papers.Independent.Intakethird100.P57.overlapCoefficients

For natural numbers N,DN,DN,D, choose complex D×DD\times DD×D matrices ArsA_r^sArs​, a graph with real weights wrs=wsrw_{rs}=w_{sr}wrs​=wsr​, wrr=0w_{rr}=0wrr​=0, and 0≤wrs<2π0\le w_{rs}<2\pi0≤wrs​<2π, sites j,k<Nj,k<Nj,k<N, and an arbitrary complex vector χ\chiχ indexed by NNN-bit strings. Set

T(b)=tr⁡ ⁣(∏r=0N−1Arbr),Φ(b)=∑r<sbr=bs=1wrs,B(b)=eiΦ(b)−iwjk1{bj=bk=1}T(b),T(b)=\operatorname{tr}\!\left(\prod_{r=0}^{N-1}A_r^{b_r}\right),\qquad \Phi(b)=\sum_{\substack{r<s\\b_r=b_s=1}}w_{rs},\qquad B(b)=e^{i\Phi(b)-iw_{jk}\mathbf1_{\{b_j=b_k=1\}}}T(b),T(b)=tr(r=0∏N−1​Arbr​​),Φ(b)=r<sbr​=bs​=1​∑​wrs​,B(b)=eiΦ(b)−iwjk​1{bj​=bk​=1}​T(b),

using increasing site order in the matrix product. Let u(b)=B(b)u(b)=B(b)u(b)=B(b) when bj,bkb_j,b_kbj​,bk​ are not both 111, and u(b)=0u(b)=0u(b)=0 otherwise, and let v(b)=B(b)v(b)=B(b)v(b)=B(b) when both bits are 111, and v(b)=0v(b)=0v(b)=0 otherwise. Writing a=⟨u,χ⟩a=\langle u,\chi\ranglea=⟨u,χ⟩ and b′=⟨v,χ⟩b'=\langle v,\chi\rangleb′=⟨v,χ⟩, the definition returns

(∣a∣2+∣b′∣2,  a b′‾)∈R×C.\left(|a|^2+|b'|^2,\;a\,\overline{b'}\right)\in\mathbb R\times\mathbb C.(∣a∣2+∣b′∣2,ab′)∈R×C.

There is no distinctness requirement on j,kj,kj,k, no normalization or nonzero requirement on either vector, and no positivity requirement on DDD; N=0N=0N=0 admits no choices of the required sites.

QAlgorithms.Papers.Independent.Intakethird100.P57.overlapObjective

For every natural number NNN and arbitrary complex vectors v,χv,\chiv,χ indexed by bit strings in {0,1}N\{0,1\}^N{0,1}N, this defines the real number

overlapObjective⁡(v,χ)=∣⟨v,χ⟩∣2∥v∥2.\operatorname{overlapObjective}(v,\chi) =\frac{|\langle v,\chi\rangle|^2}{\|v\|^2}.overlapObjective(v,χ)=∥v∥2∣⟨v,χ⟩∣2​.

Neither vector is assumed normalized or nonzero. In particular, the value is 000 when v=0v=0v=0, because division by zero in the real numbers is assigned the value 000. The case N=0N=0N=0 is included, with a single empty bit string indexing the vectors.

QAlgorithms.Papers.Independent.Intakethird100.P57.plusFactors

For every natural number NNN, this defines the complex-valued function on a site 0≤k<N0\le k<N0≤k<N and a Boolean value sss by

rk(s)=12.r_k(s)=\frac{1}{\sqrt2}.rk​(s)=2​1​.

The value is independent of both arguments. When N=0N=0N=0, the function has no site arguments.

QAlgorithms.Papers.Independent.Intakethird100.P57.productOp

For any type ι\iotaι equipped with a finite enumeration, and any family VkV_kVk​ of complex matrices whose rows and columns are indexed by Boolean values, this defines a complex matrix PPP indexed by Boolean assignments a,b:ι→{false,true}a,b:\iota\to\{\mathrm{false},\mathrm{true}\}a,b:ι→{false,true}, with entries

Pa,b=∏k∈ι(Vk)ak,bk.P_{a,b}=\prod_{k\in\iota}(V_k)_{a_k,b_k}.Pa,b​=k∈ι∏​(Vk​)ak​,bk​​.

No unitarity or other condition is imposed on VkV_kVk​. If ι\iotaι is empty, there is one Boolean assignment and the sole matrix entry is the empty product 111.

QAlgorithms.Papers.Independent.Intakethird100.P57.productTensors

For every natural number NNN and every function r:{0,…,N−1}×{false,true}→Cr:\{0,\ldots,N-1\}\times\{\mathrm{false},\mathrm{true}\}\to\mathbb Cr:{0,…,N−1}×{false,true}→C, this defines a family of 1×11\times11×1 complex matrices Ak,bA_{k,b}Ak,b​, one for each site k<Nk<Nk<N and Boolean bbb, by

(Ak,b)0,0=r(k,b).(A_{k,b})_{0,0}=r(k,b).(Ak,b​)0,0​=r(k,b).

There is no normalization condition on rrr. When N=0N=0N=0, the family has no sites.

QAlgorithms.Papers.Independent.Intakethird100.P57.productVec

For any natural number NNN and any complex values rk(s)r_k(s)rk​(s), indexed by 0≤k<N0\le k<N0≤k<N and Boolean sss, this defines a vector in the complex Euclidean space indexed by NNN-bit strings, with coordinates

vb=∏k=0N−1rk(bk).v_b=\prod_{k=0}^{N-1}r_k(b_k).vb​=k=0∏N−1​rk​(bk​).

No normalization or nonzero condition is imposed on the factors. When N=0N=0N=0, there is one bit string and its coordinate is the empty product 111.

QAlgorithms.Papers.Independent.Intakethird100.P57.rage

For any natural numbers N,DN,DN,D, any family of complex D×DD\times DD×D matrices Ak(s)A_k(s)Ak​(s) indexed by 0≤k<N0\le k<N0≤k<N and Boolean sss, any real weights wrsw_{rs}wrs​ satisfying symmetry, zero diagonal, and 0≤wrs<2π0\le w_{rs}<2\pi0≤wrs​<2π, and any family of unitary complex Boolean-indexed matrices VkV_kVk​, this defines a vector indexed by NNN-bit strings with coordinates

va=∑b:{0,…,N−1}→{false,true}(∏k=0N−1(Vk)ak,bk)exp⁡ ⁣(i ⁣∑0≤r<s<Nbr=true, bs=truewrs)tr⁡ ⁣(A0(b0)⋯AN−1(bN−1)).v_a=\sum_{b:\{0,\ldots,N-1\}\to\{\mathrm{false},\mathrm{true}\}} \left(\prod_{k=0}^{N-1}(V_k)_{a_k,b_k}\right) \exp\!\left(\mathrm{i}\! \sum_{\substack{0\le r<s<N\\ b_r=\mathrm{true},\ b_s=\mathrm{true}}}w_{rs}\right) \operatorname{tr}\!\left(A_0(b_0)\cdots A_{N-1}(b_{N-1})\right).va​=b:{0,…,N−1}→{false,true}∑​(k=0∏N−1​(Vk​)ak​,bk​​)exp​i0≤r<s<Nbr​=true, bs​=true​∑​wrs​​tr(A0​(b0​)⋯AN−1​(bN−1​)).

The matrix product inside the trace follows increasing site order. No normalization or nonzero condition is imposed. For N=0N=0N=0, the sole coordinate is DDD; for D=0D=0D=0, the vector is zero.

QAlgorithms.Papers.Independent.Intakethird100.P57.rageMarginal

For every natural number NNN, every complex vector vvv indexed by NNN-bit strings, and every finite site set S⊆{0,…,N−1}S\subseteq\{0,\ldots,N-1\}S⊆{0,…,N−1}, this defines a matrix indexed by Boolean assignments a,ba,ba,b on SSS, with entries

ρa,b=(∥v∥2)−1∑e:{0,…,N−1}∖S→{false,true}v ⁣(JS(a,e))v ⁣(JS(b,e))‾,\rho_{a,b}= \bigl(\|v\|^2\bigr)^{-1} \sum_{e:\{0,\ldots,N-1\}\setminus S\to\{\mathrm{false},\mathrm{true}\}} v\!\left(J_S(a,e)\right) \overline{v\!\left(J_S(b,e)\right)},ρa,b​=(∥v∥2)−1e:{0,…,N−1}∖S→{false,true}∑​v(JS​(a,e))v(JS​(b,e))​,

where JS(a,e)J_S(a,e)JS​(a,e) equals aaa on SSS and eee outside SSS, and the real number ∥v∥2\|v\|^2∥v∥2 is regarded as complex before taking its inverse. There is no assumption that vvv is nonzero or normalized; the inverse of zero is defined to be zero, so v=0v=0v=0 produces the zero matrix. Empty and full site sets, including N=0N=0N=0, are allowed, with a sum over an empty assignment domain containing its single empty assignment.

QAlgorithms.Papers.Independent.Intakethird100.P57.rageSiteQuadratic

For any type ι\iotaι equipped with a finite enumeration of all its elements, any complex matrix MMM with rows and columns indexed by ι\iotaι, and any function x:ι→Cx:\iota\to\mathbb Cx:ι→C, the definition gives the complex number

qM(x)=∑i∈ι∑j∈ιxi‾ Mijxj.q_M(x)=\sum_{i\in\iota}\sum_{j\in\iota}\overline{x_i}\,M_{ij}x_j.qM​(x)=i∈ι∑​j∈ι∑​xi​​Mij​xj​.

There is no Hermitian or positivity assumption on MMM, and no normalization requirement on xxx. If ι\iotaι is empty, the value is 000.

QAlgorithms.Papers.Independent.Intakethird100.P57.rawMarginal

For every natural number NNN, every complex vector vvv indexed by NNN-bit strings, and every finite site set S⊆{0,…,N−1}S\subseteq\{0,\ldots,N-1\}S⊆{0,…,N−1}, this defines a complex matrix indexed by Boolean assignments a,ba,ba,b on SSS, with entries

Ra,b=∑e:{0,…,N−1}∖S→{false,true}v ⁣(JS(a,e))v ⁣(JS(b,e))‾,R_{a,b}= \sum_{e:\{0,\ldots,N-1\}\setminus S\to\{\mathrm{false},\mathrm{true}\}} v\!\left(J_S(a,e)\right) \overline{v\!\left(J_S(b,e)\right)},Ra,b​=e:{0,…,N−1}∖S→{false,true}∑​v(JS​(a,e))v(JS​(b,e))​,

where JS(a,e)J_S(a,e)JS​(a,e) is the full bit string equal to aaa on SSS and to eee outside SSS. No normalization or nonzero condition is required on vvv. If SSS is empty, this is a 1×11\times11×1 matrix with entry ∑z∣v(z)∣2=∥v∥2\sum_z|v(z)|^2=\|v\|^2∑z​∣v(z)∣2=∥v∥2; if SSS contains all sites, the complement has one empty assignment and the entries are v(a)v(b)‾v(a)\overline{v(b)}v(a)v(b)​. These conventions also apply when N=0N=0N=0.

QAlgorithms.Papers.Independent.Intakethird100.P57.rawTangent

For arbitrary natural numbers N,DN,DN,D, complex D×DD\times DD×D matrix families A,A˙A,\dot AA,A˙ indexed by a site and a Boolean value, real arrays w,w˙w,\dot ww,w˙ indexed by two sites, and arbitrary complex 2×22\times22×2 matrix families V,V˙V,\dot VV,V˙, define

Tb=tr⁡ ⁣(∏l=0N−1Al(bl)),T˙b=∑k=0N−1tr⁡ ⁣(∏l=0N−1{A˙l(bl),l=k,Al(bl),l≠k,),T_b=\operatorname{tr}\!\left(\prod_{l=0}^{N-1}A_l(b_l)\right),\qquad \dot T_b=\sum_{k=0}^{N-1}\operatorname{tr}\!\left( \prod_{l=0}^{N-1} \begin{cases}\dot A_l(b_l),&l=k,\\A_l(b_l),&l\ne k,\end{cases}\right),Tb​=tr(l=0∏N−1​Al​(bl​)),T˙b​=k=0∑N−1​tr(l=0∏N−1​{A˙l​(bl​),Al​(bl​),​l=k,l=k,​),

with matrix products in increasing site order, and define

Γw(b)=∑i<jbi=bj=1wij,Pab=∏l=0N−1(Vl)albl,P˙ab=∑k=0N−1∏l=0N−1{(V˙l)albl,l=k,$Vl)albl,l≠k.\Gamma_w(b)=\sum_{\substack{i<j\\b_i=b_j=1}}w_{ij},\qquad P_{ab}=\prod_{l=0}^{N-1}(V_l)_{a_l b_l},\qquad \dot P_{ab}=\sum_{k=0}^{N-1}\prod_{l=0}^{N-1} \begin{cases}(\dot V_l)_{a_l b_l},&l=k,\$V_l)_{a_l b_l},&l\ne k.\end{cases}Γw​(b)=i<jbi​=bj​=1​∑​wij​,Pab​=l=0∏N−1​(Vl​)al​bl​​,P˙ab​=k=0∑N−1​l=0∏N−1​{(V˙l​)al​bl​​,​l=k,$Vl​)al​bl​​,​l=k.​

The definition returns the vector whose amplitude at (a\in{0,1}^N$ is

∑b∈{0,1}N[P˙abeiΓw(b)Tb+PabeiΓw(b)(T˙b+iΓw˙(b)Tb)].\sum_{b\in\{0,1\}^N} \left[ \dot P_{ab}e^{i\Gamma_w(b)}T_b+ P_{ab}e^{i\Gamma_w(b)} \bigl(\dot T_b+i\Gamma_{\dot w}(b)T_b\bigr) \right].b∈{0,1}N∑​[P˙ab​eiΓw​(b)Tb​+Pab​eiΓw​(b)(T˙b​+iΓw˙​(b)Tb​)].

No symmetry or bounds on w,w˙w,\dot ww,w˙, unitarity of V,V˙V,\dot VV,V˙, or derivative relationships between any of the paired inputs are required. The resulting vector is zero if N=0N=0N=0 or D=0D=0D=0.

QAlgorithms.Papers.Independent.Intakethird100.P57.rayleighEnergy

For every natural number NNN, every complex matrix HHH indexed by Boolean assignments on NNN sites, and every complex Euclidean vector vvv with the same index set, the definition assigns the real number

EH(v)=Re⁡⟨v,Hv⟩∥v∥2=Re⁡∑b,cvb‾ Hbcvc∑b∣vb∣2.E_H(v)=\frac{\operatorname{Re}\langle v,Hv\rangle}{\|v\|^2} = \frac{\operatorname{Re}\displaystyle\sum_{b,c}\overline{v_b}\,H_{bc}v_c} {\displaystyle\sum_b|v_b|^2}.EH​(v)=∥v∥2Re⟨v,Hv⟩​=b∑​∣vb​∣2Reb,c∑​vb​​Hbc​vc​​.

No Hermitian assumption on HHH or normalization or nonzero assumption on vvv is imposed. Division is total, so EH(0)=0E_H(0)=0EH​(0)=0. The definition also includes N=0N=0N=0, when the index set consists of the unique empty Boolean assignment.

QAlgorithms.Papers.Independent.Intakethird100.P57.replaceSite

For all natural numbers N,DN,DN,D, let Aj(b)A_j(b)Aj​(b) be arbitrary complex D×DD\times DD×D matrices indexed by a site j∈{0,…,N−1}j\in\{0,\ldots,N-1\}j∈{0,…,N−1} and a Boolean value bbb. Given a site kkk and any complex-valued function xxx on triples (b,i,ℓ)(b,i,\ell)(b,i,ℓ) with Boolean bbb and 0≤i,ℓ<D0\le i,\ell<D0≤i,ℓ<D, the definition gives a new family A′A'A′ with entries

Aj′(b)iℓ={x(b,i,ℓ),j=k,Aj(b)iℓ,j≠k.A'_j(b)_{i\ell} = \begin{cases} x(b,i,\ell),&j=k,\\ A_j(b)_{i\ell},&j\ne k. \end{cases}Aj′​(b)iℓ​={x(b,i,ℓ),Aj​(b)iℓ​,​j=k,j=k.​

There are no normalization or nonzero requirements. When D=0D=0D=0, the matrices and the coordinate domain are empty; when N=0N=0N=0, no site kkk can be supplied.

QAlgorithms.Papers.Independent.Intakethird100.P57.retainedOp

For every natural number NNN, let GGG specify real weights wijw_{ij}wij​ on the sites 0,…,N−10,\ldots,N-10,…,N−1, with wij=wjiw_{ij}=w_{ji}wij​=wji​, wii=0w_{ii}=0wii​=0, and 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π; let ViV_iVi​ be a unitary complex 2×22\times22×2 matrix for each site; and let SSS be any finite subset of the sites. Identifying Boolean values with 0,10,10,1, the definition gives a complex matrix RRR, indexed by assignments a,b:S→{0,1}a,b:S\to\{0,1\}a,b:S→{0,1}, whose entries are

Rab=(∏i∈S(Vi)aibi)exp⁡ ⁣(i∑i,j∈Si<jwijbibj).R_{ab} = \left(\prod_{i\in S}(V_i)_{a_i b_i}\right) \exp\!\left(\mathrm i\sum_{\substack{i,j\in S\\i<j}}w_{ij}b_i b_j\right).Rab​=(i∈S∏​(Vi​)ai​bi​​)exp​ii,j∈Si<j​∑​wij​bi​bj​​.

Thus the diagonal phase matrix on the retained sites acts first, followed by the product of their individual unitary matrices. The definition includes N=0N=0N=0 and S=∅S=\varnothingS=∅; for empty SSS, there is one assignment and RRR is the 1×11\times11×1 matrix with entry 111.

QAlgorithms.Papers.Independent.Intakethird100.P57.siteMap

For all natural numbers N,DN,DN,D, let Ai(t)A_i(t)Ai​(t) be arbitrary complex D×DD\times DD×D matrices for sites iii and Boolean values ttt; let wijw_{ij}wij​ be real weights satisfying wij=wjiw_{ij}=w_{ji}wij​=wji​, wii=0w_{ii}=0wii​=0, and 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π; let each ViV_iVi​ be a unitary complex 2×22\times22×2 matrix; and choose a site kkk. For each coordinate c=(t,r,s)c=(t,r,s)c=(t,r,s), where ttt is Boolean and 0≤r,s<D0\le r,s<D0≤r,s<D, define matrices A(c)A^{(c)}A(c) by retaining Ai(u)A_i(u)Ai​(u) when i≠ki\ne ki=k and setting

Ak(c)(u)pq={1,(u,p,q)=c,0,(u,p,q)≠c.A^{(c)}_k(u)_{pq} = \begin{cases} 1,&(u,p,q)=c,\\ 0,&(u,p,q)\ne c. \end{cases}Ak(c)​(u)pq​={1,0,​(u,p,q)=c,(u,p,q)=c.​

The definition gives the matrix LLL, with rows indexed by Boolean assignments bbb on all NNN sites and columns indexed by these coordinates ccc, whose entries are

Lbc=∑a:{0,…,N−1}→{0,1}(∏i(Vi)biai)e i∑i<jwijaiajtr⁡ ⁣(A0(c)(a0)⋯AN−1(c)(aN−1)).L_{bc} = \sum_{a:\{0,\ldots,N-1\}\to\{0,1\}} \left(\prod_i(V_i)_{b_i a_i}\right) e^{\,\mathrm i\sum_{i<j}w_{ij}a_i a_j} \operatorname{tr}\!\left(A^{(c)}_0(a_0)\cdots A^{(c)}_{N-1}(a_{N-1})\right).Lbc​=a:{0,…,N−1}→{0,1}∑​(i∏​(Vi​)bi​ai​​)ei∑i<j​wij​ai​aj​tr(A0(c)​(a0​)⋯AN−1(c)​(aN−1​)).

No nonzero or normalization assumption is required. For D=0D=0D=0, this matrix has no columns; for N=0N=0N=0, no site kkk exists.

QAlgorithms.Papers.Independent.Intakethird100.P57.siteVector

For all natural numbers N,DN,DN,D, let CDC_DCD​ be the set of triples (t,i,j)(t,i,j)(t,i,j) with Boolean ttt and 0≤i,j<D0\le i,j<D0≤i,j<D. Given any complex matrix LLL whose rows are indexed by Boolean assignments bbb on NNN sites and whose columns are indexed by CDC_DCD​, and any function x:CD→Cx:C_D\to\mathbb Cx:CD​→C, the definition gives the complex Euclidean vector with amplitudes

(siteVector⁡(L,x))b=∑c∈CDLbcxc.(\operatorname{siteVector}(L,x))_b=\sum_{c\in C_D}L_{bc}x_c.(siteVector(L,x))b​=c∈CD​∑​Lbc​xc​.

There are no normalization or nonzero requirements. For D=0D=0D=0, the sum is empty and the vector is zero; for N=0N=0N=0, there is a single row indexed by the empty assignment.

QAlgorithms.Papers.Independent.Intakethird100.P57.supportedOp

For any natural number NNN, subset S⊆IN={0,…,N−1}S\subseteq I_N=\{0,\ldots,N-1\}S⊆IN​={0,…,N−1}, and arbitrary complex matrix OOO indexed by Boolean assignments on SSS, this defines a complex matrix indexed by full Boolean assignments a,b:IN→{false,true}a,b:I_N\to\{\mathrm{false},\mathrm{true}\}a,b:IN​→{false,true}, with entries

O~ab={Oa∣S,b∣S,ak=bk for every k∉S,0,otherwise.\widetilde O_{ab}= \begin{cases} O_{a|_S,b|_S},&a_k=b_k\text{ for every }k\notin S,\\ 0,&\text{otherwise}. \end{cases}Oab​={Oa∣S​,b∣S​​,0,​ak​=bk​ for every k∈/S,otherwise.​

No Hermiticity or positivity of OOO is assumed. Empty SSS is allowed: then OOO has one entry and O~\widetilde OO is that scalar times the identity. If S=INS=I_NS=IN​, the agreement condition outside SSS is vacuous. For N=0N=0N=0, the resulting matrix has one row and one column.

QAlgorithms.Papers.Independent.Intakethird100.P57.traceMPS

For any natural numbers N,DN,DN,D and any family of complex D×DD\times DD×D matrices Ak(s)A_k(s)Ak​(s), indexed by sites 0≤k<N0\le k<N0≤k<N and Boolean values sss, this defines a vector vvv in the complex Euclidean space indexed by Boolean strings b:{0,…,N−1}→{false,true}b:\{0,\ldots,N-1\}\to\{\mathrm{false},\mathrm{true}\}b:{0,…,N−1}→{false,true}, with coordinates

vb=tr⁡ ⁣(A0(b0)A1(b1)⋯AN−1(bN−1)).v_b=\operatorname{tr}\!\left(A_0(b_0)A_1(b_1)\cdots A_{N-1}(b_{N-1})\right).vb​=tr(A0​(b0​)A1​(b1​)⋯AN−1​(bN−1​)).

The factors occur in increasing site order. No normalization is required. For N=0N=0N=0, the product is the D×DD\times DD×D identity, so the sole coordinate is DDD, regarded as a complex number; for D=0D=0D=0, every coordinate is zero.

QAlgorithms.Papers.Independent.Intakethird100.P57.transferE

For any natural numbers N,DN,DN,D, any collection of complex D×DD\times DD×D matrices Ak(t)A_k(t)Ak​(t) indexed by sites k∈{0,…,N−1}k\in\{0,\ldots,N-1\}k∈{0,…,N−1} and bits ttt, any site kkk, and any bits a,ba,ba,b, define

Eka,b=Ak(a)⊗Ak(b)‾,(Eka,b)(p,q),(r,s)=Ak(a)p,r Ak(b)q,s‾,E_k^{a,b}=A_k(a)\otimes\overline{A_k(b)}, \qquad (E_k^{a,b})_{(p,q),(r,s)} = A_k(a)_{p,r}\,\overline{A_k(b)_{q,s}},Eka,b​=Ak​(a)⊗Ak​(b)​,(Eka,b​)(p,q),(r,s)​=Ak​(a)p,r​Ak​(b)q,s​​,

where p,q,r,s∈{0,…,D−1}p,q,r,s\in\{0,\ldots,D-1\}p,q,r,s∈{0,…,D−1} and the bar denotes entrywise complex conjugation. This is a matrix indexed by pairs of bond indices. If D=0D=0D=0, it is the empty matrix; if N=0N=0N=0, no site kkk can be supplied.

QAlgorithms.Papers.Independent.Intakethird100.P57.transferT

For any natural numbers N,DN,DN,D, complex D×DD\times DD×D matrices Ak(t)A_k(t)Ak​(t) indexed by sites k∈{0,…,N−1}k\in\{0,\ldots,N-1\}k∈{0,…,N−1} and bits ttt, real weights wjkw_{j k}wjk​ satisfying wjk=wkjw_{j k}=w_{k j}wjk​=wkj​, wkk=0w_{kk}=0wkk​=0, and 0≤wjk<2π0\le w_{j k}<2\pi0≤wjk​<2π, a finite set of sites SSS, bit assignments a,b:S→{0,1}a,b:S\to\{0,1\}a,b:S→{0,1}, and a site kkk, define the matrix

Tka,b={Ak(ak)⊗Ak(bk)‾,k∈S,∑t∈{0,1}exp⁡ ⁣(i t∑j∈Swjk(aj−bj))(Ak(t)⊗Ak(t)‾),k∉S.T_k^{a,b}= \begin{cases} A_k(a_k)\otimes\overline{A_k(b_k)},&k\in S,\\[2mm] \displaystyle\sum_{t\in\{0,1\}} \exp\!\left(\mathrm{i}\,t\sum_{j\in S}w_{j k}(a_j-b_j)\right) \bigl(A_k(t)\otimes\overline{A_k(t)}\bigr),&k\notin S. \end{cases}Tka,b​=⎩⎨⎧​Ak​(ak​)⊗Ak​(bk​)​,t∈{0,1}∑​exp​itj∈S∑​wjk​(aj​−bj​)​(Ak​(t)⊗Ak​(t)​),​k∈S,k∈/S.​

Here bits in the exponential are interpreted as real numbers 000 or 111, conjugation is entrywise, and the tensor product has entries (B⊗C‾)(p,q),(r,s)=Bp,rCq,s‾(B\otimes\overline C)_{(p,q),(r,s)}=B_{p,r}\overline{C_{q,s}}(B⊗C)(p,q),(r,s)​=Bp,r​Cq,s​​. If SSS is empty, every site uses the second branch with exponential factor 111. If D=0D=0D=0, the resulting matrix is empty; if N=0N=0N=0, no site kkk can be supplied.

QAlgorithms.Papers.Independent.Intakethird100.P57.updatedWeights

For a natural number NNN, a graph with real weights wab=wbaw_{ab}=w_{ba}wab​=wba​, waa=0w_{aa}=0waa​=0, and 0≤wab<2π0\le w_{ab}<2\pi0≤wab​<2π, sites j,k<Nj,k<Nj,k<N, and any real θ\thetaθ, this defines a real-valued function on ordered pairs of sites by

wab′={wjk+θ−2π⌊wjk+θ2π⌋,(a=j and b=k) or (a=k and b=j),wab,otherwise.w'_{ab}= \begin{cases} w_{jk}+\theta- 2\pi\left\lfloor\dfrac{w_{jk}+\theta}{2\pi}\right\rfloor, &(a=j\text{ and }b=k)\text{ or }(a=k\text{ and }b=j),\\[5pt] w_{ab},&\text{otherwise}. \end{cases}wab′​=⎩⎨⎧​wjk​+θ−2π⌊2πwjk​+θ​⌋,wab​,​(a=j and b=k) or (a=k and b=j),otherwise.​

The sites are not required to be distinct: if j=kj=kj=k, the selected entry is the diagonal entry (j,j)(j,j)(j,j). The output is a weight function, without an accompanying assertion that it satisfies the graph conditions. For N=0N=0N=0, the required sites cannot be supplied.

QAlgorithms.Papers.Independent.Intakethird100.P57.wrapAngle

For every real number θ\thetaθ, this defines

wrapAngle⁡(θ)=θ−2π⌊θ2π⌋,\operatorname{wrapAngle}(\theta) =\theta-2\pi\left\lfloor\frac{\theta}{2\pi}\right\rfloor,wrapAngle(θ)=θ−2π⌊2πθ​⌋,

where the floor is an integer regarded as a real number in the product. The definition applies to all real inputs, including negative values and exact integer multiples of 2π2\pi2π.

QAlgorithms.Papers.Independent.Intakethird100.P57.zMean

For every natural number NNN, every complex vector vvv indexed by NNN-bit strings, and every site i<Ni<Ni<N, this defines the real number

Zi(v)=∑b∈{false,true}N{−∣v(b)∣2,bi=true,∣v(b)∣2,bi=false.Z_i(v)= \sum_{b\in\{\mathrm{false},\mathrm{true}\}^N} \begin{cases} -|v(b)|^2,&b_i=\mathrm{true},\\ |v(b)|^2,&b_i=\mathrm{false}. \end{cases}Zi​(v)=b∈{false,true}N∑​{−∣v(b)∣2,∣v(b)∣2,​bi​=true,bi​=false.​

Here ∣v(b)∣2|v(b)|^2∣v(b)∣2 is the complex squared modulus. No normalization or nonzero condition is imposed on vvv, and there is no division by its squared norm; the zero vector gives zero. Although NNN ranges over all natural numbers, no site i<Ni<Ni<N exists when N=0N=0N=0.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

    Confirmed by the mission captain (proposal self-audit).

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