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Definitions for Universal Quantum Emulator

Definition
QAlgorithms_Papers_Independent_Intakethird100_P67

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

prove2quantum

The objects the formalized statements of Universal Quantum Emulator (arXiv:1606.02734) are stated in. Each was checked against the paper by a blind read-back and a moderator.

  • densityConjugation: PDF p.2: unitary conjugation, also for subnormalized branches.
  • sampleAlgebra: PDF p.2: complex span of all nonempty sample words (supported nonunital algebra).
  • samplePi: PDF p.2: the support projector of the sum of PSD sample densities is the projector onto the span of their supports. CFC is evaluated on a finite spectrum.
  • Generates: PDF p.2, Eq.(6): equality with the full supported matrix algebra.
  • InSampleSupport: PDF p.2: density support contained in the input span.
  • sampleDimension: PDF p.2, Eq.(2): dimension of the sample support.
  • pureSamples: PDF p.2: pure sample density records.
  • sampleReflection: PDF p.3, Eq.(9): the sample reflection sign is I-2P.
  • systemControlled: PDF p.3, Eq.(10): frozen control-first gate reindexed into system-first order.
  • erasureGate: PDF p.3, Eq.(11), R(k) H R(anchor), with the rightmost gate first.
  • minusRegister: PDF p.4: |minus> tensor T, including the empty tensor.
  • minusVector: PDF p.3: the normalized one-qubit |minus>.
  • onAncilla: PDF p.4: a system/one-qubit operator placed on ancilla j.
  • historyUnitary: PDF p.13: ordered forward history, recalled unchanged in the reverse circuit.
  • historyWeight: PDF p.14: iid history weight.
  • coherentErasureChannel: PDF p.14, A5: the generalized averaged erasure channel.
  • nonanchorProbability: PDF pp.4–5: fixed anchor excluded from the uniform random indices.
  • jointBranchHistory: PDF pp.13–16: a Fig.5 branch, including measurement, replacement of the system by the output anchor, then reverse output history. False means b=0.
  • jointBranch: PDF p.14: averaged subnormalized joint branch.
  • jointEmulator: PDF p.14, A10: nonselective joint output in the Appendix A convention.
  • transportedGate: PDF pp.6,15, Eq.(18)/A12: covariance has U-dagger on the right, correcting printed A1's U. This does not impose U squared equal to the identity.
  • eraseProbability: PDF p.6, Eq.(20): actual erasure success probability.
  • emulate: PDF p.6: pure-sample main-system emulator, Appendix A output convention.
  • compressedReflection: PDF p.7, Eq.(25): compression to H_in intersect anchor-perp.
  • compressedReflectionChannel: PDF p.7, Eq.(24): compressed sampleReflection channel.
  • lambdaPerp: PDF p.7, Eq.(26): norm of the vectorized compressed channel.
  • residual: PDF p.8, Eq.(35): exact, unnormalized residual.
  • unaryWord: PDF p.8: unary address, including residual t=T.
  • coordinateExpansion: PDF p.8, Eq.(34): the full expansion retains its residual term.
  • meanSampleDensity: PDF p.32, H3: average sample density.
  • projectionBranch: PDF pp.31–32: actual Fig.7 branch. Same history is used forward and backward; false is span detection, true is the all-minus outcome.
  • projectionChannel: PDF p.32: channel discarding the Fig.7 label.
  • gentleChannel: PDF p.33, H19: randomized conjugated projective measurement.
  • gentleProbability: PDF p.34, H21: actual expected outcome probability.
  • ProjectiveFamily: PDF p.33: complete orthogonal projectors; zero projectors are allowed.
  • positivePhaseEvolution: PDF p.20: positive-sign matrix exponential, e^(i theta H).
  • pureFisherInformation: PDF pp.7–8, Eq.(31): quantum Fisher information of a differentiable normalized pure-state family. The theorem uses the actual analytic exp(i alpha P) family, so no nondifferentiability default of deriv is involved.
  • referenceVector: PDF p.24: n independently prepared pure reference registers.
  • swapReference: PDF p.24, E1: SWAP of system with reference j, identity on other references.
  • swapHamiltonian: PDF p.24, E1: full continuous interaction.
  • swapJoint: PDF p.24, E2: actual joint positivePhaseEvolution.
  • effectiveHamiltonian: PDF p.24, E3: effective Hamiltonian with the n+1 coefficient.
  • wireBranch: PDF p.4, Fig.2: unsuccessful output is the old system wire from the SWAP. The successful wire is reconstructed. These differ from Appendix A on failure.
  • mixedGate: PDF p.28, G1: systemControlled density-matrix translations.
  • mixedSampleErasureChannel: PDF p.28: entrywise Lebesgue integration of the continuous one-round body. For density samples the matrix exponential body is continuous on the compact interval.
  • mixedHistory: PDF p.28: history unitary for fixed mixed-sample indices and real times.
  • mixedHistoryOutput: PDF p.28: fixed mixed-history output after system replacement and reconstruction.
  • mixedEmulate: PDF p.28: actual mixed-sample emulator, with independent uniform times and indices. Entrywise integrals are over a compact cube of a continuous finite-matrix body.
  • bridgeSamples: PDF p.28, G2: tagged sample densities plus a pure bridge (none).
  • conjugateBasis: PDF p.29, G3: positive-sign Fourier-densityConjugation basis.
  • uniformAddress: PDF pp.29–30: normalized uniform address state.
  • negativeFourier: PDF p.30, G7: negative-sign normalized DFT. This corrects G7's missing normalization and ket index; G6 and G11 determine this sign.
  • basisPhase: PDF pp.29–30, G4/G8: full spectral exponential, hence identity on H_in-perp.
  • increment: PDF p.22, D5: cyclic increment on the binary address.
  • binaryMeasure: PDF p.22, D6: Fig.6 effective operation on system/address, with the helper returned to |minus>. The address is initialized at zero, correcting D8's printed |t>.
  • addressedReflection: PDF p.23, D7: address-selective sampleReflection; t is a natural address.
  • binaryHistory: PDF pp.22–23: actual binary history F(t+1,k) V, using addresses 1 through T.
  • encodeUnary: PDF pp.22–23: linear reencoding of the unary subspace, extended by zero elsewhere.
  • registerSwap: PDF p.11: SWAP between two equal-dimensional registers.
  • doubleControlledSwap: PDF p.11: double-systemControlled full-register SWAP, with both controls ancillary.
  • ElementaryGate: PDF pp.19–21: source elementary gate set, one-qubit unitaries and two-control SWAPs acting on four distinct qubit wires.
  • elementaryMatrix: PDF pp.19–21: complete matrix semantics of the counted elementary gates.
  • SampleCircuit: PDF pp.19–21: a circuit using supplied indexed density copies and fixed ancillary bits. Ports are disjoint by one injection; gates do not receive the unknown U or samples. The output is the main system and all other wires are traced out.
  • SampleCircuit.initial: PDF pp.19–21: product input with actual independent supplied sample copies.
  • SampleCircuit.output: PDF pp.19–21: source circuit channel; gate cost is literally gates.length.
  • inputOutputRecords: PDF p.19: actual supplied input/output records, with no coherent phase reference.
  • EmulatorFamily: PDF pp.19–21: one uniform family of sample circuits, fixed before the unknown sample vectors, U, and the new input. T and m are precision controls; history is classical.
  • precisionRounds: PDF p.19: fixed ideal-error allocation eps/2 and at most eps/2 for all DME calls. For rank one no erasure rounds are needed. This corrects the printed allocation after B21, whose substitution into B19 gives more than eps. Constants only are rescaled.
  • slowFactor: PDF pp.7,19: explicit polylogarithmic multiplier used to spell out O-tilde.
  • BinaryEmulatorFamily: PDF p.22: binary circuits also accept the number of address qubits q.
Definition code
import Mathlib
import Definitions.Def_QAlgorithms_Defs_QuantumOutputMetrics
import Definitions.Def_QAlgorithms_Defs_Measurement
import Definitions.Def_QAlgorithms_Defs_Gates
import Definitions.Def_QAlgorithms_Defs_Learning

/-! Universal Quantum Emulator, arXiv:1606.02734v2. Page numbers are PDF pages.
All new constructions are paper-local. Tensor factors put the system first.
Generated algebras use nonempty words: the ambient identity is not silently adjoined. -/

noncomputable section
open scoped ComplexConjugate Matrix Matrix.Norms.L2Operator
attribute [local instance] Classical.propDecidable
open MeasureTheory Filter

namespace QAlgorithms.Papers.Independent.Intakethird100.P67

variable {I J K L A : Type*} [Fintype I] [DecidableEq I]
  [Fintype J] [DecidableEq J] [Fintype K] [DecidableEq K]
  [Fintype L] [DecidableEq L] [Fintype A] [DecidableEq A]

/-- PDF p.2: unitary conjugation, also for subnormalized branches. -/
def densityConjugation (V : Matrix I I ℂ) (rho : Matrix I I ℂ) : Matrix I I ℂ := V * rho * Vᴴ

/-- PDF p.2: complex span of all nonempty sample words (supported nonunital algebra). -/
def sampleAlgebra (S : K → Matrix I I ℂ) : Submodule ℂ (Matrix I I ℂ) :=
  Submodule.span ℂ {X | ∃ w : List K, w ≠ [] ∧ X = (w.map S).prod}

/-- PDF p.2: the support projector of the sum of PSD sample densities is the projector
onto the span of their supports. CFC is evaluated on a finite spectrum. -/
def samplePi (S : K → Matrix I I ℂ) : Matrix I I ℂ :=
  cfc (fun x : ℝ => if x = 0 then 0 else 1) (∑ k, S k)

/-- PDF p.2, Eq.(6): equality with the full supported matrix algebra. -/
def Generates (S : K → Matrix I I ℂ) : Prop :=
  ∀ X : Matrix I I ℂ, X ∈ sampleAlgebra S ↔ samplePi S * X * samplePi S = X

/-- PDF p.2: density support contained in the input span. -/
def InSampleSupport (S : K → Matrix I I ℂ) (rho : Matrix I I ℂ) : Prop :=
  samplePi S * rho * samplePi S = rho

/-- PDF p.2, Eq.(2): dimension of the sample support. -/
def sampleDimension (S : K → Matrix I I ℂ) : ℕ :=
  Module.finrank ℂ (LinearMap.range (Matrix.toEuclideanLin (samplePi S)))

/-- PDF p.2: pure sample density records. -/
def pureSamples (phi : K → EuclideanSpace ℂ I) : K → Matrix I I ℂ := fun k => pureDensity (phi k)

/-- PDF p.3, Eq.(9): the sample reflection sign is I-2P. -/
def sampleReflection (phi : EuclideanSpace ℂ I) : Matrix I I ℂ := 1 - 2 • pureDensity phi

/-- PDF p.3, Eq.(10): frozen control-first gate reindexed into system-first order. -/
def systemControlled (V : Matrix I I ℂ) : Matrix (I × Bool) (I × Bool) ℂ :=
  (QAlgorithms.controlled V).submatrix Prod.swap Prod.swap

/-- PDF p.3, Eq.(11), R(k) H R(anchor), with the rightmost gate first. -/
def erasureGate (phi : K → EuclideanSpace ℂ I) (a k : K) : Matrix (I × Bool) (I × Bool) ℂ :=
  systemControlled (sampleReflection (phi k)) * Matrix.kronecker (1 : Matrix I I ℂ) hadamard *
    systemControlled (sampleReflection (phi a))

/-- PDF p.4: |minus> tensor T, including the empty tensor. -/
def minusRegister (T : ℕ) : EuclideanSpace ℂ (Qubits T) :=
  WithLp.toLp 2 fun z => ∏ j : Fin T,
    if z j then -((Real.sqrt 2)⁻¹ : ℂ) else ((Real.sqrt 2)⁻¹ : ℂ)

/-- PDF p.3: the normalized one-qubit |minus>. -/
def minusVector : EuclideanSpace ℂ Bool :=
  WithLp.toLp 2 fun b => if b then -((Real.sqrt 2)⁻¹ : ℂ) else ((Real.sqrt 2)⁻¹ : ℂ)

/-- PDF p.4: a system/one-qubit operator placed on ancilla j. -/
def onAncilla {T : ℕ} (V : Matrix (I × Bool) (I × Bool) ℂ) (j : Fin T) : Matrix (I × Qubits T) (I × Qubits T) ℂ :=
  fun x y => if ∀ l, l ≠ j → x.2 l = y.2 l then V (x.1,x.2 j) (y.1,y.2 j) else 0

/-- PDF p.13: ordered forward history, recalled unchanged in the reverse circuit. -/
def historyUnitary {T : ℕ} (W : L → Matrix (I × Bool) (I × Bool) ℂ) (h : Fin T → L) : Matrix (I × Qubits T) (I × Qubits T) ℂ :=
  (List.ofFn fun j : Fin T => onAncilla (W (h j)) j).foldl (fun V G => G * V) 1

/-- PDF p.14: iid history weight. -/
def historyWeight {T : ℕ} (p : L → ℝ) (h : Fin T → L) : ℝ := ∏ j, p (h j)

/-- PDF p.14, A5: the generalized averaged erasure channel. -/
def coherentErasureChannel (p : L → ℝ) (W : L → Matrix (I × Bool) (I × Bool) ℂ) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  ∑ l, (p l : ℂ) • traceRight (densityConjugation (W l) (Matrix.kronecker rho (pureDensity minusVector)))

/-- PDF pp.4–5: fixed anchor excluded from the uniform random indices. -/
def nonanchorProbability (a k : K) : ℝ :=
  if k = a then 0 else ((Fintype.card K - 1 : ℕ) : ℝ)⁻¹

/-- PDF pp.13–16: a Fig.5 branch, including measurement, replacement of the system
by the output anchor, then reverse output history. False means b=0. -/
def jointBranchHistory {T : ℕ} (Win : L → Matrix (I × Bool) (I × Bool) ℂ)
    (Wout : L → Matrix (J × Bool) (J × Bool) ℂ) (phi : EuclideanSpace ℂ I) (phiout : EuclideanSpace ℂ J)
    (h : Fin T → L) (b : Bool) (rho : Matrix I I ℂ) : Matrix (J × Qubits T) (J × Qubits T) ℂ :=
  let X := densityConjugation (historyUnitary Win h) (Matrix.kronecker rho (pureDensity (minusRegister T)))
  let P := if b then 1 - pureDensity phi else pureDensity phi
  let measured := densityConjugation (Matrix.kronecker P (1 : Matrix (Qubits T) (Qubits T) ℂ)) X
  densityConjugation (historyUnitary Wout h)ᴴ
    (Matrix.kronecker (pureDensity phiout) (traceLeft measured))

/-- PDF p.14: averaged subnormalized joint branch. -/
def jointBranch (p : L → ℝ) (Win : L → Matrix (I × Bool) (I × Bool) ℂ)
    (Wout : L → Matrix (J × Bool) (J × Bool) ℂ) (phi : EuclideanSpace ℂ I) (phiout : EuclideanSpace ℂ J)
    (T : ℕ) (b : Bool) (rho : Matrix I I ℂ) : Matrix (J × Qubits T) (J × Qubits T) ℂ :=
  ∑ h : Fin T → L, (historyWeight p h : ℂ) • jointBranchHistory Win Wout phi phiout h b rho

/-- PDF p.14, A10: nonselective joint output in the Appendix A convention. -/
def jointEmulator (p : L → ℝ) (Win : L → Matrix (I × Bool) (I × Bool) ℂ)
    (Wout : L → Matrix (J × Bool) (J × Bool) ℂ) (phi : EuclideanSpace ℂ I) (phiout : EuclideanSpace ℂ J)
    (T : ℕ) (rho : Matrix I I ℂ) : Matrix (J × Qubits T) (J × Qubits T) ℂ :=
  jointBranch p Win Wout phi phiout T false rho + jointBranch p Win Wout phi phiout T true rho

/-- PDF pp.6,15, Eq.(18)/A12: covariance has U-dagger on the right, correcting
printed A1's U. This does not impose U squared equal to the identity. -/
def transportedGate (U : Matrix I I ℂ) (W : L → Matrix (I × Bool) (I × Bool) ℂ) : L → Matrix (I × Bool) (I × Bool) ℂ :=
  fun l => densityConjugation (Matrix.kronecker U (1 : Matrix Bool Bool ℂ)) (W l)

/-- PDF p.6, Eq.(20): actual erasure success probability. -/
def eraseProbability (p : L → ℝ) (W : L → Matrix (I × Bool) (I × Bool) ℂ)
    (phi : EuclideanSpace ℂ I) (T : ℕ) (rho : Matrix I I ℂ) : ℝ :=
  effectProb (pureDensity phi) ((coherentErasureChannel p W)^[T] rho)

/-- PDF p.6: pure-sample main-system emulator, Appendix A output convention. -/
def emulate (phi : K → EuclideanSpace ℂ I) (a : K) (U : Matrix I I ℂ) (T : ℕ) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  traceRight (jointEmulator (nonanchorProbability a) (erasureGate phi a)
    (transportedGate U (erasureGate phi a)) (phi a) (act U (phi a)) T rho)

/-- PDF p.7, Eq.(25): compression to H_in intersect anchor-perp. -/
def compressedReflection (phi : K → EuclideanSpace ℂ I) (a k : K) : Matrix I I ℂ :=
  let Q := samplePi (pureSamples phi) - pureDensity (phi a)
  Q * sampleReflection (phi k) * Q

/-- PDF p.7, Eq.(24): compressed sampleReflection channel. -/
def compressedReflectionChannel (phi : K → EuclideanSpace ℂ I) (a : K) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  ∑ k, (nonanchorProbability a k : ℂ) •
    (compressedReflection phi a k * rho * compressedReflection phi a k)

/-- PDF p.7, Eq.(26): norm of the vectorized compressed channel. -/
def lambdaPerp (phi : K → EuclideanSpace ℂ I) (a : K) : ℝ :=
  QAlgorithms.specNorm (∑ k, (nonanchorProbability a k : ℂ) • Matrix.kronecker
    (compressedReflection phi a k) (fun i j => conj (compressedReflection phi a k i j)))

/-- PDF p.8, Eq.(35): exact, unnormalized residual. -/
def residual (phi : K → EuclideanSpace ℂ I) (a : K) (psi : EuclideanSpace ℂ I) (h : List K) : EuclideanSpace ℂ I :=
  h.foldl (fun v k => act (sampleReflection (phi k) * (1 - pureDensity (phi a))) v) psi

/-- PDF p.8: unary address, including residual t=T. -/
def unaryWord (T t : ℕ) : Qubits T := fun j => decide ((j : ℕ) < t)

/-- PDF p.8, Eq.(34): the full expansion retains its residual term. -/
def coordinateExpansion {T : ℕ} (phi : K → EuclideanSpace ℂ I) (a : K)
    (h : Fin T → K) (psi : EuclideanSpace ℂ I) : EuclideanSpace ℂ (I × Qubits T) :=
  (∑ t : Fin T, (inner ℂ (phi a) (residual phi a psi ((List.ofFn h).take t.val))) •
    tensorVec (phi a) (ket (unaryWord T t.val))) +
    tensorVec (residual phi a psi (List.ofFn h)) (ket (unaryWord T T))

/-- PDF p.32, H3: average sample density. -/
def meanSampleDensity (phi : K → EuclideanSpace ℂ I) : Matrix I I ℂ := (Fintype.card K : ℂ)⁻¹ • ∑ k, pureDensity (phi k)

/-- PDF pp.31–32: actual Fig.7 branch. Same history is used forward and backward;
false is span detection, true is the all-minus outcome. -/
def projectionBranch (phi : K → EuclideanSpace ℂ I) (T : ℕ) (b : Bool) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  ((Fintype.card K : ℂ) ^ T)⁻¹ • ∑ h : Fin T → K,
    let V := historyUnitary (fun k => systemControlled (sampleReflection (phi k))) h
    let P := Matrix.kronecker (1 : Matrix I I ℂ) (pureDensity (minusRegister T))
    let Q := if b then P else 1 - P
    traceRight (densityConjugation Vᴴ (densityConjugation Q
      (densityConjugation V (Matrix.kronecker rho (pureDensity (minusRegister T))))))

/-- PDF p.32: channel discarding the Fig.7 label. -/
def projectionChannel (phi : K → EuclideanSpace ℂ I) (T : ℕ) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  projectionBranch phi T false rho + projectionBranch phi T true rho

/-- PDF p.33, H19: randomized conjugated projective measurement. -/
def gentleChannel (p : L → ℝ) (V : L → Matrix I I ℂ) (P : A → Matrix I I ℂ) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  ∑ l, (p l : ℂ) • ∑ a, densityConjugation ((V l)ᴴ * P a * V l) rho

/-- PDF p.34, H21: actual expected outcome probability. -/
def gentleProbability (p : L → ℝ) (V : L → Matrix I I ℂ) (P : A → Matrix I I ℂ)
    (rho : Matrix I I ℂ) (a : A) : ℝ := ∑ l, p l * effectProb (P a) (densityConjugation (V l) rho)

/-- PDF p.33: complete orthogonal projectors; zero projectors are allowed. -/
def ProjectiveFamily (P : A → Matrix I I ℂ) : Prop :=
  (∀ a, (P a).IsHermitian ∧ P a * P a = P a) ∧
    (∀ a b, a ≠ b → P a * P b = 0) ∧ ∑ a, P a = 1

/-- PDF p.20: positive-sign matrix exponential, e^(i theta H). -/
def positivePhaseEvolution (H : Matrix I I ℂ) (theta : ℝ) : Matrix I I ℂ := NormedSpace.exp ((Complex.I * theta) • H)

/-- PDF pp.7–8, Eq.(31): quantum Fisher information of a differentiable normalized
pure-state family. The theorem uses the actual analytic exp(i alpha P) family, so no
nondifferentiability default of deriv is involved. -/
def pureFisherInformation (v : ℝ → EuclideanSpace ℂ I) (alpha : ℝ) : ℝ :=
  4 * (‖deriv v alpha‖ ^ 2 - ‖inner ℂ (v alpha) (deriv v alpha)‖ ^ 2)

/-- PDF p.24: n independently prepared pure reference registers. -/
def referenceVector (phi : EuclideanSpace ℂ I) (n : ℕ) : EuclideanSpace ℂ (Fin n → I) :=
  WithLp.toLp 2 fun x => ∏ j, phi (x j)

/-- PDF p.24, E1: SWAP of system with reference j, identity on other references. -/
def swapReference {n : ℕ} (j : Fin n) : Matrix (I × (Fin n → I)) (I × (Fin n → I)) ℂ :=
  fun x y => if x.1 = y.2 j ∧ x.2 = Function.update y.2 j y.1 then 1 else 0

/-- PDF p.24, E1: full continuous interaction. -/
def swapHamiltonian (n : ℕ) (coupling : ℝ) : Matrix (I × (Fin n → I)) (I × (Fin n → I)) ℂ :=
  (coupling : ℂ) • ∑ j : Fin n, swapReference j

/-- PDF p.24, E2: actual joint positivePhaseEvolution. -/
def swapJoint (phi : EuclideanSpace ℂ I) (n : ℕ) (coupling t : ℝ) (rho : Matrix I I ℂ) : Matrix (I × (Fin n → I)) (I × (Fin n → I)) ℂ :=
  densityConjugation (positivePhaseEvolution (swapHamiltonian n coupling) (-t))
    (Matrix.kronecker rho (pureDensity (referenceVector phi n)))

/-- PDF p.24, E3: effective Hamiltonian with the n+1 coefficient. -/
def effectiveHamiltonian (phi : EuclideanSpace ℂ I) (n : ℕ) (coupling : ℝ) : Matrix I I ℂ :=
  ((coupling * (n + 1) : ℝ) : ℂ) • pureDensity phi

/-! Construction sanity checks. -/

example (v : EuclideanSpace ℂ I) (alpha : ℝ) : pureFisherInformation (fun _ : ℝ => v) alpha = 0 := by
  simp [pureFisherInformation]

example (phi : K → EuclideanSpace ℂ I) (a : K) (psi : EuclideanSpace ℂ I) : residual phi a psi [] = psi := rfl

example (W : L → Matrix (I × Bool) (I × Bool) ℂ) (h : Fin 0 → L) : historyUnitary W h = 1 := by
  simp [historyUnitary]

example (x : Qubits 0) : minusRegister 0 x = 1 := by simp [minusRegister]

example (T : ℕ) (j : Fin T) : unaryWord T 0 j = false := by simp [unaryWord]

example (T : ℕ) (j : Fin T) : unaryWord T T j = true := by simp [unaryWord, j.isLt]

example (V : Matrix I I ℂ) (i j : I) : systemControlled V (i,false) (j,true) = 0 := rfl

example (phi : K → EuclideanSpace ℂ I) (a : K) : nonanchorProbability a a = 0 := by simp [nonanchorProbability]

example (phi : EuclideanSpace ℂ I) (n : ℕ) (t : ℝ) (rho : Matrix I I ℂ) :
    swapJoint phi n 0 t rho = Matrix.kronecker rho (pureDensity (referenceVector phi n)) := by
  simp [swapJoint, swapHamiltonian, positivePhaseEvolution, densityConjugation]

/-- PDF p.4, Fig.2: unsuccessful output is the old system wire from the SWAP.
The successful wire is reconstructed. These differ from Appendix A on failure. -/
def wireBranch (phi : K → EuclideanSpace ℂ I) (a : K) (U : Matrix I I ℂ) (T : ℕ) (b : Bool) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  if b then
    ∑ h : Fin T → K, (historyWeight (nonanchorProbability a) h : ℂ) •
      traceRight (densityConjugation (Matrix.kronecker (1 - pureDensity (phi a)) (1 : Matrix (Qubits T) (Qubits T) ℂ))
        (densityConjugation (historyUnitary (erasureGate phi a) h)
          (Matrix.kronecker rho (pureDensity (minusRegister T)))))
  else traceRight (jointBranch (nonanchorProbability a) (erasureGate phi a)
    (transportedGate U (erasureGate phi a)) (phi a) (act U (phi a)) T false rho)

/-- PDF p.28, G1: systemControlled density-matrix translations. -/
def mixedGate (S : K → Matrix I I ℂ) (a k : K) (t : ℝ) : Matrix (I × Bool) (I × Bool) ℂ :=
  systemControlled (positivePhaseEvolution (S k) (-t)) * Matrix.kronecker (1 : Matrix I I ℂ) hadamard *
    systemControlled (positivePhaseEvolution (S a) (-Real.pi))

/-- PDF p.28: entrywise Lebesgue integration of the continuous one-round body.
For density samples the matrix exponential body is continuous on the compact interval. -/
def mixedSampleErasureChannel (S : K → Matrix I I ℂ) (a : K) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  (Fintype.card K : ℂ)⁻¹ • ∑ k,
    fun i j => ∫ t in Set.Icc (0 : ℝ) 1,
      traceRight (densityConjugation (mixedGate S a k t) (Matrix.kronecker rho (pureDensity minusVector))) i j

/-- PDF p.28: history unitary for fixed mixed-sample indices and real times. -/
def mixedHistory {T : ℕ} (S : K → Matrix I I ℂ) (a : K) (h : Fin T → K) (ts : Fin T → ℝ) :
    Matrix (I × Qubits T) (I × Qubits T) ℂ :=
  (List.ofFn fun j : Fin T => onAncilla (mixedGate S a (h j) (ts j)) j).foldl (fun V G => G * V) 1

/-- PDF p.28: fixed mixed-history output after system replacement and reconstruction. -/
def mixedHistoryOutput {T : ℕ} (S : K → Matrix I I ℂ) (a : K) (phi : EuclideanSpace ℂ I)
    (U : Matrix I I ℂ) (rho : Matrix I I ℂ) (h : Fin T → K) (ts : Fin T → ℝ) : Matrix I I ℂ :=
  let Vin := mixedHistory S a h ts
  let Vout := Matrix.kronecker U (1 : Matrix (Qubits T) (Qubits T) ℂ) * Vin *
    Matrix.kronecker Uᴴ (1 : Matrix (Qubits T) (Qubits T) ℂ)
  traceRight (densityConjugation Voutᴴ (Matrix.kronecker (pureDensity (act U phi))
    (traceLeft (densityConjugation Vin (Matrix.kronecker rho (pureDensity (minusRegister T)))))))

/-- PDF p.28: actual mixed-sample emulator, with independent uniform times and indices.
Entrywise integrals are over a compact cube of a continuous finite-matrix body. -/
def mixedEmulate (S : K → Matrix I I ℂ) (a : K) (phi : EuclideanSpace ℂ I) (U : Matrix I I ℂ)
    (T : ℕ) (rho : Matrix I I ℂ) : Matrix I I ℂ :=
  ((Fintype.card K : ℂ) ^ T)⁻¹ • ∑ h : Fin T → K,
    fun i j => ∫ ts in Set.pi Set.univ (fun _ : Fin T => Set.Icc (0 : ℝ) 1),
      mixedHistoryOutput S a phi U rho h ts i j

/-- PDF p.28, G2: tagged sample densities plus a pure bridge (none). -/
def bridgeSamples (S : K → Matrix I I ℂ) (phi : EuclideanSpace ℂ I) (alpha beta : ℂ) : Option (Bool × K) → Matrix (I × Bool) (I × Bool) ℂ
  | none => pureDensity (tensorVec phi (WithLp.toLp 2 fun b => if b then beta else alpha))
  | some (b,k) => Matrix.kronecker (S k) (pureDensity (ket b))

/-- PDF p.29, G3: positive-sign Fourier-densityConjugation basis. -/
def conjugateBasis {d : ℕ} (theta : Fin d → EuclideanSpace ℂ I) (j : Fin d) : EuclideanSpace ℂ I :=
  ∑ k, ((((Real.sqrt d)⁻¹ : ℝ) : ℂ) *
    Complex.exp (Complex.I * (2 * Real.pi * k.val * j.val / d : ℝ))) • theta k

/-- PDF pp.29–30: normalized uniform address state. -/
def uniformAddress (d : ℕ) : EuclideanSpace ℂ (Fin d) := WithLp.toLp 2 fun _ => ((Real.sqrt d)⁻¹ : ℂ)

/-- PDF p.30, G7: negative-sign normalized DFT. This corrects G7's missing
normalization and ket index; G6 and G11 determine this sign. -/
def negativeFourier (d : ℕ) : Matrix (Fin d) (Fin d) ℂ :=
  fun j k => ((Real.sqrt d)⁻¹ : ℂ) *
    Complex.exp (-Complex.I * (2 * Real.pi * j.val * k.val / d : ℝ))

/-- PDF pp.29–30, G4/G8: full spectral exponential, hence identity on H_in-perp. -/
def basisPhase {d : ℕ} (theta : Fin d → EuclideanSpace ℂ I) : Matrix (I × Fin d) (I × Fin d) ℂ :=
  fun x y => if x.2 = y.2 then
    positivePhaseEvolution (∑ k : Fin d, (k.val : ℂ) • pureDensity (theta k))
      (2 * Real.pi * x.2.val / d) x.1 y.1 else 0

/-- PDF p.22, D5: cyclic increment on the binary address. -/
def increment (q : ℕ) : Matrix (Fin (2 ^ q)) (Fin (2 ^ q)) ℂ :=
  fun x y => if x.val = (y.val + 1) % (2 ^ q) then 1 else 0

/-- PDF p.22, D6: Fig.6 effective operation on system/address, with the helper
returned to |minus>. The address is initialized at zero, correcting D8's printed |t>. -/
def binaryMeasure (phi : EuclideanSpace ℂ I) (q : ℕ) : Matrix (I × Fin (2 ^ q)) (I × Fin (2 ^ q)) ℂ :=
  Matrix.kronecker (pureDensity phi) 1 + Matrix.kronecker (1 - pureDensity phi) (increment q)

/-- PDF p.23, D7: address-selective sampleReflection; t is a natural address. -/
def addressedReflection (phi : EuclideanSpace ℂ I) (q t : ℕ) : Matrix (I × Fin (2 ^ q)) (I × Fin (2 ^ q)) ℂ :=
  fun x y => if x.2 = y.2 then
    (if x.2.val = t then sampleReflection phi else 1) x.1 y.1 else 0

/-- PDF pp.22–23: actual binary history F(t+1,k) V, using addresses 1 through T. -/
def binaryHistory {T : ℕ} (phi : K → EuclideanSpace ℂ I) (a : K) (q : ℕ) (h : Fin T → K) :
    Matrix (I × Fin (2 ^ q)) (I × Fin (2 ^ q)) ℂ :=
  (List.ofFn fun j : Fin T => addressedReflection (phi (h j)) q (j.val+1) * binaryMeasure (phi a) q).foldl (fun V G => G * V) 1

/-- PDF pp.22–23: linear reencoding of the unary subspace, extended by zero elsewhere. -/
def encodeUnary (q T : ℕ) (v : EuclideanSpace ℂ (I × Qubits T)) : EuclideanSpace ℂ (I × Fin (2 ^ q)) :=
  WithLp.toLp 2 fun x => ∑ t : Fin (T+1),
    if x.2.val = t.val then v (x.1, unaryWord T t.val) else 0

/-- PDF p.11: SWAP between two equal-dimensional registers. -/
def registerSwap : Matrix (I × I) (I × I) ℂ := fun x y => if x.1 = y.2 ∧ x.2 = y.1 then 1 else 0

/-- PDF p.11: double-systemControlled full-register SWAP, with both controls ancillary. -/
def doubleControlledSwap : Matrix ((I × I) × (Bool × Bool)) ((I × I) × (Bool × Bool)) ℂ :=
  fun x y => if x.2 = y.2 then
    (if x.2.1 && x.2.2 then registerSwap else 1) x.1 y.1 else 0

/-- PDF pp.19–21: source elementary gate set, one-qubit unitaries and two-control
SWAPs acting on four distinct qubit wires. -/
inductive ElementaryGate (N : ℕ) where
  | one (wire : Fin N) (U : Matrix.unitaryGroup Bool ℂ)
  | ccswap (wires : Fin 4 ↪ Fin N)

/-- PDF pp.19–21: complete matrix semantics of the counted elementary gates. -/
def elementaryMatrix {N : ℕ} : ElementaryGate N → Matrix (Qubits N) (Qubits N) ℂ
  | .one q U => fun x y =>
      if ∀ l, l ≠ q → x l = y l then (U : Matrix Bool Bool ℂ) (x q) (y q) else 0
  | .ccswap w => fun x y =>
      if x = (if y (w 0) && y (w 1) then
        Function.update (Function.update y (w 2) (y (w 3))) (w 3) (y (w 2)) else y)
      then 1 else 0

/-- PDF pp.19–21: a circuit using supplied indexed density copies and fixed ancillary
bits. Ports are disjoint by one injection; gates do not receive the unknown U or samples.
The output is the main system and all other wires are traced out. -/
structure SampleCircuit (n : ℕ) (K : Type*) where
  N : ℕ
  copies : ℕ
  ports : (Fin n ⊕ (Fin copies × Fin n)) ↪ Fin N
  labels : Fin copies → Bool × K
  auxiliaryBits : Qubits N
  gates : List (ElementaryGate N)

/-- PDF pp.19–21: product input with actual independent supplied sample copies. -/
def SampleCircuit.initial {n : ℕ} (C : SampleCircuit n K)
    (records : Bool × K → Matrix (Qubits n) (Qubits n) ℂ) (rho : Matrix (Qubits n) (Qubits n) ℂ) : Matrix (Qubits C.N) (Qubits C.N) ℂ :=
  fun x y => rho (fun j => x (C.ports (.inl j))) (fun j => y (C.ports (.inl j))) *
    (∏ r, records (C.labels r)
      (fun j => x (C.ports (.inr (r,j)))) (fun j => y (C.ports (.inr (r,j))))) *
    (if ∀ q, q ∉ Set.range C.ports → x q = C.auxiliaryBits q ∧ y q = C.auxiliaryBits q then 1 else 0)

/-- PDF pp.19–21: source circuit channel; gate cost is literally gates.length. -/
def SampleCircuit.output {n : ℕ} (C : SampleCircuit n K)
    (records : Bool × K → Matrix (Qubits n) (Qubits n) ℂ) (rho : Matrix (Qubits n) (Qubits n) ℂ) : Matrix (Qubits n) (Qubits n) ℂ :=
  let V := (C.gates.map elementaryMatrix).foldl (fun V G => G * V) 1
  let X := densityConjugation V (C.initial records rho)
  fun i j => ∑ x : Qubits C.N, ∑ y : Qubits C.N,
    if (∀ l, x (C.ports (.inl l)) = i l ∧ y (C.ports (.inl l)) = j l) ∧
      (∀ q, q ∉ Set.range (fun l => C.ports (.inl l)) → x q = y q) then X x y else 0

/-- PDF p.19: actual supplied input/output records, with no coherent phase reference. -/
def inputOutputRecords (phi : K → EuclideanSpace ℂ I) (U : Matrix I I ℂ) : Bool × K → Matrix I I ℂ :=
  fun bk => if bk.1 then densityConjugation U (pureDensity (phi bk.2)) else pureDensity (phi bk.2)

/-- PDF pp.19–21: one uniform family of sample circuits, fixed before the unknown
sample vectors, U, and the new input. T and m are precision controls; history is classical. -/
abbrev EmulatorFamily := ∀ n k : ℕ, Fin k → (T m : ℕ) → (Fin T → Fin k) → SampleCircuit n (Fin k)

example (phi : EuclideanSpace ℂ I) (x : Fin 0 → I) : referenceVector phi 0 x = 1 := by
  simp [referenceVector]

/-- PDF p.19: fixed ideal-error allocation eps/2 and at most eps/2 for all DME calls.
For rank one no erasure rounds are needed. This corrects the printed allocation after B21,
whose substitution into B19 gives more than eps. Constants only are rescaled. -/
def precisionRounds (d : ℕ) (lam eps : ℝ) : ℕ :=
  if d ≤ 1 then 0 else max 1 ⌈Real.log (8 * eps⁻¹ ^ 2 * (d - 1 : ℝ)) / (1-lam)⌉₊

/-- PDF pp.7,19: explicit polylogarithmic multiplier used to spell out O-tilde. -/
def slowFactor (d : ℕ) (eps : ℝ) (power : ℕ) : ℝ :=
  (1 + Real.log (d+1) + Real.log (1+eps⁻¹)) ^ power

/-- PDF p.22: binary circuits also accept the number of address qubits q. -/
abbrev BinaryEmulatorFamily := ∀ n k : ℕ, Fin k → (q T m : ℕ) →
  (Fin T → Fin k) → SampleCircuit n (Fin k)

end QAlgorithms.Papers.Independent.Intakethird100.P67
Source
Universal Quantum Emulator, arXiv:1606.02734v2, https://arxiv.org/abs/1606.02734v2
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What the Lean code literally says, in plain math · gpt-6.1-sol

QAlgorithms.Papers.Independent.Intakethird100.P67.BinaryEmulatorFamily

This abbreviates the type of all families BBB that, for every pair of natural numbers n,kn,kn,k, every anchor a∈{0,…,k−1}a\in\{0,\ldots,k-1\}a∈{0,…,k−1}, every three natural numbers q,T,mq,T,mq,T,m, and every history h:{0,…,T−1}→{0,…,k−1}h:\{0,\ldots,T-1\}\to\{0,\ldots,k-1\}h:{0,…,T−1}→{0,…,k−1}, return a sample circuit on nnn-qubit registers with sample labels in Bool×{0,…,k−1}\mathrm{Bool}\times\{0,\ldots,k-1\}Bool×{0,…,k−1}. Such a circuit consists of a natural number NNN of physical qubits, a natural number sss of sample copies, an injective map placing the nnn input wires and the snsnsn sample wires into the NNN physical wires, a Boolean-and-index label for each sample copy, a fixed Boolean value for every physical wire, and a list of elementary gates. An elementary gate is either an arbitrary one-qubit unitary or a gate on four distinct wires that swaps the last two wires exactly when the first two are both true. Given input and sample matrices, initialization places them on their respective ports and puts all remaining wires in their designated computational-basis states; the output applies the gates in list order and traces out every wire except the input ports. This abbreviation imposes no resource, correctness, or computability condition. All natural parameters may be zero; when k=0k=0k=0, there is no anchor argument to supply.

QAlgorithms.Papers.Independent.Intakethird100.P67.ElementaryGate

For every natural number NNN, an elementary gate on NNN wires is one of two kinds: a choice of a wire q∈{0,…,N−1}q\in\{0,\ldots,N-1\}q∈{0,…,N−1} together with a unitary complex matrix UUU indexed by the two Boolean values, or an injective assignment w:{0,1,2,3}↪{0,…,N−1}w:\{0,1,2,3\}\hookrightarrow\{0,\ldots,N-1\}w:{0,1,2,3}↪{0,…,N−1} of four distinct wires. The second kind carries no additional matrix parameter. The definition permits N=0N=0N=0, when there are no elementary gates; the four-wire kind is available only when N≥4N\ge4N≥4.

QAlgorithms.Papers.Independent.Intakethird100.P67.EmulatorFamily

An emulator family is a function that, for every pair of natural numbers n,kn,kn,k, every anchor a∈{0,…,k−1}a\in\{0,\ldots,k-1\}a∈{0,…,k−1}, every pair of natural numbers T,mT,mT,m, and every sequence h:{0,…,T−1}→{0,…,k−1}h:\{0,\ldots,T-1\}\to\{0,\ldots,k-1\}h:{0,…,T−1}→{0,…,k−1}, returns a sample circuit on nnn-wire registers whose labels belong to {0,…,k−1}\{0,\ldots,k-1\}{0,…,k−1}. Such a circuit specifies its own physical wire count, number of record registers, injective allocation of the input and record ports, Boolean-label pairs for its records, auxiliary Boolean assignment, and finite list of one-wire unitary or four-wire controlled-swap gates. There are no resource bounds or correctness conditions and no required relationship between T,m,hT,m,hT,m,h and the returned circuit. The case T=0T=0T=0 uses the unique empty sequence; n=0n=0n=0 and m=0m=0m=0 are allowed. When k=0k=0k=0, there is no anchor argument, so no circuit is required for that value of kkk.

QAlgorithms.Papers.Independent.Intakethird100.P67.Generates

For a finite index type III with decidable equality, a finite label type KKK, and arbitrary complex I×II\times II×I matrices SkS_kSk​, let AS\mathcal A_SAS​ be the complex linear span of all nonempty finite ordered products of the SkS_kSk​, allowing repeated labels, and let ΠS=f(∑kSk)\Pi_S=f(\sum_k S_k)ΠS​=f(∑k​Sk​) in real continuous functional calculus, with f(0)=0f(0)=0f(0)=0 and f(x)=1f(x)=1f(x)=1 for x≠0x\neq0x=0. This defines the assertion that, for every complex I×II\times II×I matrix XXX, X∈ASX\in\mathcal A_SX∈AS​ if and only if ΠSXΠS=X\Pi_S X\Pi_S=XΠS​XΠS​=X. For a Hermitian sum, ΠS\Pi_SΠS​ projects onto its nonzero eigenspaces; for a non-Hermitian sum it is zero, so the assertion then requires AS={0}\mathcal A_S=\{0\}AS​={0}. An empty label type satisfies this assertion.

QAlgorithms.Papers.Independent.Intakethird100.P67.InSampleSupport

For a finite index type III with decidable equality, a finite label type KKK, arbitrary complex I×II\times II×I matrices SkS_kSk​, and an arbitrary complex I×II\times II×I matrix ρ\rhoρ, this defines the assertion ΠSρΠS=ρ\Pi_S\rho\Pi_S=\rhoΠS​ρΠS​=ρ, where ΠS=f(∑kSk)\Pi_S=f(\sum_kS_k)ΠS​=f(∑k​Sk​) in real continuous functional calculus, with f(0)=0f(0)=0f(0)=0 and f(x)=1f(x)=1f(x)=1 for nonzero real xxx. If the sum is Hermitian, ΠS\Pi_SΠS​ projects onto its nonzero eigenspaces; if it is not Hermitian, ΠS=0\Pi_S=0ΠS​=0. No positivity or trace condition is imposed on ρ\rhoρ. In particular, when KKK is empty or the sum is non-Hermitian, the assertion is equivalent to ρ=0\rho=0ρ=0.

QAlgorithms.Papers.Independent.Intakethird100.P67.ProjectiveFamily

For finite index types I,AI,AI,A, with decidable equality on III, and any family P:A→CI×IP:A\to\mathbb C^{I\times I}P:A→CI×I, this predicate means that every PaP_aPa​ is Hermitian and satisfies Pa2=PaP_a^2=P_aPa2​=Pa​, every two distinct labels a,b∈Aa,b\in Aa,b∈A satisfy PaPb=0P_aP_b=0Pa​Pb​=0, and

∑a∈APa=Id.\sum_{a\in A}P_a=\mathrm{Id}.a∈A∑​Pa​=Id.

Zero projectors are allowed. If AAA is empty, the individual and pairwise conditions are vacuous and the final condition is 0=Id0=\mathrm{Id}0=Id, which holds precisely when III is empty.

QAlgorithms.Papers.Independent.Intakethird100.P67.SampleCircuit.initial

For any natural number nnn, label type KKK, sample circuit CCC with NNN physical wires and ccc additional registers, arbitrary matrices ρ\rhoρ and Rb,kR_{b,k}Rb,k​ on nnn-bit strings, this definition constructs a matrix on NNN-bit strings as follows. Write xinx_{\mathrm{in}}xin​ for the restriction of xxx to the distinguished input ports and xrx_rxr​ for its restriction to additional register rrr, and similarly for yyy; write uuu for the circuit’s specified auxiliary Boolean assignment. Then

Cinitial(x,y)=ρ(xin,yin)∏r<cRC.labels(r)(xr,yr){1,xq=uq and yq=uq for every wire q outside all ports,0,otherwise.C_{\mathrm{initial}}(x,y) =\rho(x_{\mathrm{in}},y_{\mathrm{in}}) \prod_{r<c}R_{C.\mathrm{labels}(r)}(x_r,y_r) \begin{cases} 1,&x_q=u_q\ \text{and}\ y_q=u_q \text{ for every wire }q\text{ outside all ports},\\ 0,&\text{otherwise}. \end{cases}Cinitial​(x,y)=ρ(xin​,yin​)r<c∏​RC.labels(r)​(xr​,yr​){1,0,​xq​=uq​ and yq​=uq​ for every wire q outside all ports,otherwise.​

No positivity or trace assumptions are imposed on the supplied matrices. The auxiliary assignment on port wires does not enter this expression, and when c=0c=0c=0 the product is 111; when n=0n=0n=0, the supplied register matrices are 1×11\times11×1 matrices.

QAlgorithms.Papers.Independent.Intakethird100.P67.SampleCircuit

For a natural number nnn and an arbitrary label type KKK, a sample circuit consists of natural numbers NNN and ccc, an injection from the disjoint union {0,…,n−1}⊔({0,…,c−1}×{0,…,n−1})\{0,\ldots,n-1\}\sqcup(\{0,\ldots,c-1\}\times\{0,\ldots,n-1\}){0,…,n−1}⊔({0,…,c−1}×{0,…,n−1}) into the NNN physical wires, a label (br,kr)∈{false,true}×K(b_r,k_r)\in\{\mathrm{false},\mathrm{true}\}\times K(br​,kr​)∈{false,true}×K for each r<cr<cr<c, a Boolean assignment to all NNN wires, and a finite ordered list of elementary gates on those wires. The injection allocates mutually distinct wires to one distinguished nnn-wire register and to each of the ccc additional nnn-wire registers, so (c+1)n≤N(c+1)n\le N(c+1)n≤N. Labels may repeat. Zero values of nnn, NNN, or ccc, and an empty gate list, are allowed whenever the specified injection and labels exist; no normalization or correctness conditions are included.

QAlgorithms.Papers.Independent.Intakethird100.P67.SampleCircuit.output

For any natural number nnn, label type KKK, sample circuit CCC, arbitrary record matrices Rb,kR_{b,k}Rb,k​, and arbitrary input matrix ρ\rhoρ, let G1,…,GsG_1,\ldots,G_sG1​,…,Gs​ be the matrices of its elementary gates in list order: a one-wire gate applies its specified unitary on that wire and preserves every other bit, while a four-wire gate swaps its last two specified wires exactly when its first two specified bits are true. Set V=Gs⋯G1V=G_s\cdots G_1V=Gs​⋯G1​, with V=1V=1V=1 for an empty list, and set X=VAV†X=VAV^\daggerX=VAV†, where

A(x,y)=ρ(xin,yin)∏r<C.copiesRC.labels(r)(xr,yr)A(x,y)=\rho(x_{\mathrm{in}},y_{\mathrm{in}}) \prod_{r<C.\mathrm{copies}} R_{C.\mathrm{labels}(r)}(x_r,y_r)A(x,y)=ρ(xin​,yin​)r<C.copies∏​RC.labels(r)​(xr​,yr​)

when both xxx and yyy equal the prescribed auxiliary assignment outside all ports, and A(x,y)=0A(x,y)=0A(x,y)=0 otherwise. Here the restrictions refer to the distinguished input ports and the additional register ports of CCC. The output entry at nnn-bit strings i,ji,ji,j is

∑x,y on the physical wiresxin=i, yin=jxq=yq on every non-input wireX(x,y).\sum_{\substack{x,y\text{ on the physical wires}\\ x_{\mathrm{in}}=i,\ y_{\mathrm{in}}=j\\ x_q=y_q\text{ on every non-input wire}}}X(x,y).x,y on the physical wiresxin​=i, yin​=jxq​=yq​ on every non-input wire​∑​X(x,y).

Thus the definition traces out every physical wire outside the distinguished input register, including the record registers. It requires no positivity or normalization of the supplied matrices and includes zero-sized registers and empty gate lists.

QAlgorithms.Papers.Independent.Intakethird100.P67.addressedReflection

For an index type III with decidable equality, any vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, and natural numbers q,tq,tq,t, put N=2qN=2^qN=2q. This defines a matrix on I×{0,…,N−1}I\times\{0,\ldots,N-1\}I×{0,…,N−1} with zero entries between different address values; its block at address rrr is II−2ϕϕ∗I_I-2\phi\phi^\astII​−2ϕϕ∗ if r=tr=tr=t, and III_III​ otherwise, where (ϕϕ∗)ij=ϕiϕj‾(\phi\phi^\ast)_{ij}=\phi_i\overline{\phi_j}(ϕϕ∗)ij​=ϕi​ϕj​​. No normalization of ϕ\phiϕ is required. If t≥Nt\ge Nt≥N, the whole matrix is the identity; for q=0q=0q=0, its sole address block is II−2ϕϕ∗I_I-2\phi\phi^\astII​−2ϕϕ∗ when t=0t=0t=0, and the identity otherwise.

QAlgorithms.Papers.Independent.Intakethird100.P67.basisPhase

For a finite index type III with decidable equality, a natural number ddd, and any family θk∈CI\theta_k\in\mathbb C^Iθk​∈CI indexed by 0≤k<d0\le k<d0≤k<d, put Hij=∑k=0d−1k (θk)i(θk)j‾H_{ij}=\sum_{k=0}^{d-1}k\,(\theta_k)_i\overline{(\theta_k)_j}Hij​=∑k=0d−1​k(θk​)i​(θk​)j​​. This defines the matrix on I×{0,…,d−1}I\times\{0,\ldots,d-1\}I×{0,…,d−1} whose entry at row (i,r)(i,r)(i,r) and column (j,s)(j,s)(j,s) is [exp⁡(i(2πr/d)H)]ij[\exp(\mathrm{i}(2\pi r/d)H)]_{ij}[exp(i(2πr/d)H)]ij​ when r=sr=sr=s, and zero otherwise, where the exponential is the matrix exponential. No normalization or orthogonality of the θk\theta_kθk​ is assumed. When d=0d=0d=0, the matrix has an empty index set.

QAlgorithms.Papers.Independent.Intakethird100.P67.binaryHistory

For a finite index type III with decidable equality, an index type KKK, natural numbers T,qT,qT,q, any family ϕk∈CI\phi_k\in\mathbb C^Iϕk​∈CI, an anchor a∈Ka\in Ka∈K, and a sequence h0,…,hT−1∈Kh_0,\ldots,h_{T-1}\in Kh0​,…,hT−1​∈K, put N=2qN=2^qN=2q, P=ϕaϕa∗P=\phi_a\phi_a^\astP=ϕa​ϕa∗​, and let CCC be the address shift with entries Crs=1{r=(s+1) mod N}C_{rs}=\mathbf1_{\{r=(s+1)\bmod N\}}Crs​=1{r=(s+1)modN}​. Set B=P⊗IN+(II−P)⊗CB=P\otimes I_N+(I_I-P)\otimes CB=P⊗IN​+(II​−P)⊗C, and let RjR_jRj​ be block diagonal in the address, with block II−2ϕhjϕhj∗I_I-2\phi_{h_j}\phi_{h_j}^\astII​−2ϕhj​​ϕhj​∗​ at address j+1j+1j+1 and identity blocks elsewhere. This defines (RT−1B)⋯(R0B)(R_{T-1}B)\cdots(R_0B)(RT−1​B)⋯(R0​B), with the empty product equal to the identity when T=0T=0T=0. No vectors are required to be normalized, and no relation between TTT and 2q2^q2q is imposed: when j+1≥2qj+1\ge2^qj+1≥2q, RjR_jRj​ is the identity while the factor BBB remains.

QAlgorithms.Papers.Independent.Intakethird100.P67.binaryMeasure

For an index type III with decidable equality, any vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, and any natural number qqq, put N=2qN=2^qN=2q and Pij=ϕiϕj‾P_{ij}=\phi_i\overline{\phi_j}Pij​=ϕi​ϕj​​. This defines the complex matrix on I×{0,…,N−1}I\times\{0,\ldots,N-1\}I×{0,…,N−1} with entry Pijδrs+(δij−Pij)1{r=(s+1) mod N}P_{ij}\delta_{rs}+(\delta_{ij}-P_{ij})\mathbf1_{\{r=(s+1)\bmod N\}}Pij​δrs​+(δij​−Pij​)1{r=(s+1)modN}​ at row (i,r)(i,r)(i,r) and column (j,s)(j,s)(j,s), where δ\deltaδ is the Kronecker delta. No normalization of ϕ\phiϕ is assumed. When q=0q=0q=0, this matrix is the identity.

QAlgorithms.Papers.Independent.Intakethird100.P67.bridgeSamples

For index types KKK and III, any family of complex matrices SkS_kSk​ indexed by I×II\times II×I, any vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, and any α,β∈C\alpha,\beta\in\mathbb Cα,β∈C, this defines a matrix-valued function on an optional pair consisting of a Boolean and an element of KKK. Put cfalse=αc_{\mathrm{false}}=\alphacfalse​=α and ctrue=βc_{\mathrm{true}}=\betactrue​=β. At the absent value, its entry from column (j,c)(j,c)(j,c) to row (i,b)(i,b)(i,b) is ϕicb ϕjcc‾\phi_i c_b\,\overline{\phi_j c_c}ϕi​cb​ϕj​cc​​. At a present value (b0,k)(b_0,k)(b0​,k), that entry is (Sk)ij(S_k)_{ij}(Sk​)ij​ if b=c=b0b=c=b_0b=c=b0​, and zero otherwise. No normalization of ϕ,α,β\phi,\alpha,\betaϕ,α,β, or positivity or trace condition on SkS_kSk​, is required.

QAlgorithms.Papers.Independent.Intakethird100.P67.coherentErasureChannel

For finite index types III and LLL, arbitrary real weights pℓp_\ellpℓ​, arbitrary complex matrices WℓW_\ellWℓ​ indexed by I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true}, and an arbitrary complex matrix ρ\rhoρ indexed by III, this defines

∑ℓ∈Lpℓ Tr⁡bit ⁣[Wℓ(ρ⊗mm†)Wℓ†],mfalse=12,mtrue=−12,\sum_{\ell\in L}p_\ell\, \operatorname{Tr}_{\mathrm{bit}}\!\left[ W_\ell\bigl(\rho\otimes mm^\dagger\bigr)W_\ell^\dagger \right], \qquad m_{\mathrm{false}}=\frac1{\sqrt2}, \quad m_{\mathrm{true}}=-\frac1{\sqrt2},ℓ∈L∑​pℓ​Trbit​[Wℓ​(ρ⊗mm†)Wℓ†​],mfalse​=2​1​,mtrue​=−2​1​,

where †\dagger† denotes conjugate transpose and the partial trace means (Tr⁡bitX)i,i′=∑bX(i,b),(i′,b)(\operatorname{Tr}_{\mathrm{bit}}X)_{i,i'}=\sum_bX_{(i,b),(i',b)}(Trbit​X)i,i′​=∑b​X(i,b),(i′,b)​. The real weights are regarded as complex scalars in this matrix sum. No normalization or positivity of ppp or ρ\rhoρ, and no unitarity of WℓW_\ellWℓ​, is required. If LLL is empty, the result is the zero matrix.

QAlgorithms.Papers.Independent.Intakethird100.P67.compressedReflection

For finite index types I,KI,KI,K, with decidable equality on III, an arbitrary family ϕk∈CI\phi_k\in\mathbb C^Iϕk​∈CI, and elements a,k∈Ka,k\in Ka,k∈K, this defines

Q(1−2ϕkϕk†)Q,Q=Π−ϕaϕa†,Π=f ⁣(∑r∈Kϕrϕr†),f(t)={0,t=0,1,t≠0.Q\bigl(\mathbf1-2\phi_k\phi_k^\dagger\bigr)Q, \qquad Q=\Pi-\phi_a\phi_a^\dagger, \qquad \Pi=f\!\left(\sum_{r\in K}\phi_r\phi_r^\dagger\right), \quad f(t)= \begin{cases} 0,&t=0,\\ 1,&t\ne0. \end{cases}Q(1−2ϕk​ϕk†​)Q,Q=Π−ϕa​ϕa†​,Π=f(r∈K∑​ϕr​ϕr†​),f(t)={0,1,​t=0,t=0.​

Here (vv†)i,i′=vivi′‾(vv^\dagger)_{i,i'}=v_i\overline{v_{i'}}(vv†)i,i′​=vi​vi′​​, and fff is applied to the matrix by the real continuous functional calculus, so Π\PiΠ is the spectral projection onto the nonzero eigenspaces of the positive semidefinite sum. The vectors need not be normalized or linearly independent, and aaa and kkk may coincide. If every ϕr\phi_rϕr​ is zero, the defined matrix is zero.

QAlgorithms.Papers.Independent.Intakethird100.P67.compressedReflectionChannel

For finite index types I,KI,KI,K with decidable equality, any family ϕ:K→CI\phi:K\to\mathbb C^Iϕ:K→CI, an anchor a∈Ka\in Ka∈K, and any complex matrix ρ\rhoρ indexed by III, define DkD_kDk​ by (Dk)ij=ϕk(i)ϕk(j)‾(D_k)_{ij}=\phi_k(i)\overline{\phi_k(j)}(Dk​)ij​=ϕk​(i)ϕk​(j)​, and let Π=f(∑k∈KDk)\Pi=f(\sum_{k\in K}D_k)Π=f(∑k∈K​Dk​), using matrix functional calculus with f(0)=0f(0)=0f(0)=0 and f(x)=1f(x)=1f(x)=1 for x≠0x\ne0x=0. Put Q=Π−DaQ=\Pi-D_aQ=Π−Da​, Ck=Q(Id−2Dk)QC_k=Q(\mathrm{Id}-2D_k)QCk​=Q(Id−2Dk​)Q, and pa(k)=0p_a(k)=0pa​(k)=0 when k=ak=ak=a, otherwise pa(k)=1/(∣K∣−1)p_a(k)=1/(|K|-1)pa​(k)=1/(∣K∣−1). The definition returns

∑k∈Kpa(k) CkρCk.\sum_{k\in K}p_a(k)\,C_k\rho C_k.k∈K∑​pa​(k)Ck​ρCk​.

The vectors need not be normalized, and ρ\rhoρ need not be a density matrix. The anchor makes KKK nonempty; if KKK has one element, the result is zero. The subtraction in ∣K∣−1|K|-1∣K∣−1 is natural-number subtraction, and division uses the convention 1/0=01/0=01/0=0.

QAlgorithms.Papers.Independent.Intakethird100.P67.conjugateBasis

For an index type III, a natural number ddd, any family θ0,…,θd−1∈CI\theta_0,\ldots,\theta_{d-1}\in\mathbb C^Iθ0​,…,θd−1​∈CI, and an index 0≤j<d0\le j<d0≤j<d, this defines the vector ∑k=0d−1(d)−1exp⁡(2πikj/d) θk\sum_{k=0}^{d-1}(\sqrt d)^{-1}\exp(2\pi\mathrm{i}kj/d)\,\theta_k∑k=0d−1​(d​)−1exp(2πikj/d)θk​. The vectors θk\theta_kθk​ are not required to be normalized, orthogonal, or a basis. The parameter d=0d=0d=0 is included, but then there is no index jjj at which to evaluate this definition.

QAlgorithms.Papers.Independent.Intakethird100.P67.coordinateExpansion

For a finite index type III with decidable equality, an index type KKK, any natural number TTT, family ϕ:K→CI\phi:K\to\mathbb C^Iϕ:K→CI, anchor a∈Ka\in Ka∈K, history h:{0,…,T−1}→Kh:\{0,\ldots,T-1\}\to Kh:{0,…,T−1}→K, and vector ψ∈CI\psi\in\mathbb C^Iψ∈CI, define (Dk)ij=ϕk(i)ϕk(j)‾(D_k)_{ij}=\phi_k(i)\overline{\phi_k(j)}(Dk​)ij​=ϕk​(i)ϕk​(j)​, r0=ψr_0=\psir0​=ψ, and rt+1=(Id−2Dh(t))(Id−Da)rtr_{t+1}=(\mathrm{Id}-2D_{h(t)})(\mathrm{Id}-D_a)r_trt+1​=(Id−2Dh(t)​)(Id−Da​)rt​. Let uT,tu_{T,t}uT,t​ be the length-TTT Boolean word whose bit jjj is true exactly when j<tj<tj<t. The definition returns the vector EEE indexed by pairs (i,z)(i,z)(i,z), with i∈Ii\in Ii∈I and zzz a length-TTT Boolean word, given by

E(i,z)=∑t=0T−1(∑j∈Iϕa(j)‾ rt(j))ϕa(i) 1{z=uT,t}+rT(i) 1{z=uT,T}.E(i,z)= \sum_{t=0}^{T-1} \left(\sum_{j\in I}\overline{\phi_a(j)}\,r_t(j)\right) \phi_a(i)\,\mathbf1_{\{z=u_{T,t}\}} +r_T(i)\,\mathbf1_{\{z=u_{T,T}\}}.E(i,z)=t=0∑T−1​​j∈I∑​ϕa​(j)​rt​(j)​ϕa​(i)1{z=uT,t​}​+rT​(i)1{z=uT,T​}​.

Here 1\mathbf11 is the indicated equality indicator. No vectors are required to be normalized. For T=0T=0T=0, the sum is empty and E(i,z)=ψ(i)E(i,z)=\psi(i)E(i,z)=ψ(i) for the unique empty word zzz.

QAlgorithms.Papers.Independent.Intakethird100.P67.densityConjugation

For a finite index type III and arbitrary complex matrices V,ρV,\rhoV,ρ indexed by I×II\times II×I, this defines their density conjugation to be VρV†V\rho V^\daggerVρV†, where V†V^\daggerV† is the conjugate transpose. Neither unitarity of VVV nor positivity or normalization of ρ\rhoρ is assumed; the definition also applies when III is empty.

QAlgorithms.Papers.Independent.Intakethird100.P67.doubleControlledSwap

For an index type III with decidable equality, this defines a complex matrix indexed by (I×I)×({false,true}×{false,true})(I\times I)\times(\{\mathrm{false},\mathrm{true}\}\times\{\mathrm{false},\mathrm{true}\})(I×I)×({false,true}×{false,true}). Its entry at row ((i,j),(b,c))((i,j),(b,c))((i,j),(b,c)) and column ((k,ℓ),(b′,c′))((k,\ell),(b',c'))((k,ℓ),(b′,c′)) is zero unless (b,c)=(b′,c′)(b,c)=(b',c')(b,c)=(b′,c′); when the Boolean pairs agree, the entry is 1{i=ℓ, j=k}\mathbf1_{\{i=\ell,\ j=k\}}1{i=ℓ, j=k}​ if both bbb and ccc are true, and 1{i=k, j=ℓ}\mathbf1_{\{i=k,\ j=\ell\}}1{i=k, j=ℓ}​ otherwise. Thus the two III-registers are swapped exactly in the block where both Boolean values are true. If III is empty, the matrix is empty.

QAlgorithms.Papers.Independent.Intakethird100.P67.effectiveHamiltonian

For a coordinate index type III, any vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, natural number nnn, and real coupling ccc, this defines the complex matrix

c(n+1)ϕϕ†,(c(n+1)ϕϕ†)ij=c(n+1)ϕiϕj‾.c(n+1)\phi\phi^\dagger, \qquad \bigl(c(n+1)\phi\phi^\dagger\bigr)_{ij} =c(n+1)\phi_i\overline{\phi_j}.c(n+1)ϕϕ†,(c(n+1)ϕϕ†)ij​=c(n+1)ϕi​ϕj​​.

No normalization of ϕ\phiϕ or sign restriction on ccc is imposed. In particular, n=0n=0n=0 gives cϕϕ†c\phi\phi^\daggercϕϕ†, and ϕ=0\phi=0ϕ=0 gives the zero matrix.

QAlgorithms.Papers.Independent.Intakethird100.P67.elementaryMatrix

For every natural number NNN, this definition assigns a complex matrix, with rows and columns indexed by Boolean strings x,y:{0,…,N−1}→{false,true}x,y:\{0,\ldots,N-1\}\to\{\mathrm{false},\mathrm{true}\}x,y:{0,…,N−1}→{false,true}, to each elementary gate on NNN wires. For a one-wire gate specified by qqq and a unitary 2×22\times22×2 matrix UUU, its entry is Uxq,yqU_{x_q,y_q}Uxq​,yq​​ if xℓ=yℓx_\ell=y_\ellxℓ​=yℓ​ for every ℓ≠q\ell\ne qℓ=q, and is zero otherwise. For a four-wire gate specified by an injection www, its entry is 111 precisely when xxx is obtained from yyy by swapping the values on wires w(2)w(2)w(2) and w(3)w(3)w(3) if both yw(0)y_{w(0)}yw(0)​ and yw(1)y_{w(1)}yw(1)​ are true, and by leaving yyy unchanged otherwise; every other entry is zero. In the swap case, the two replacement values are both taken from the original string yyy.

QAlgorithms.Papers.Independent.Intakethird100.P67.emulate

For finite index types I,KI,KI,K with decidable equality, an arbitrary vector family ϕk∈CI\phi_k\in\mathbb C^Iϕk​∈CI, an anchor a∈Ka\in Ka∈K, a complex matrix UUU on III, a natural number TTT, and a matrix ρ\rhoρ on III, this defines the matrix

Tr⁡anc∑b∈{false,true}∑h:{0,…,T−1}→K(∏j=0T−1ph(j))Hout(h)†[(Uϕa)(Uϕa)†⊗Tr⁡I ⁣((Pb⊗1)Hin(h)(ρ⊗mTmT†)Hin(h)†(Pb†⊗1))]Hout(h).\operatorname{Tr}_{\mathrm{anc}} \sum_{b\in\{\mathrm{false},\mathrm{true}\}} \sum_{h:\{0,\ldots,T-1\}\to K} \left(\prod_{j=0}^{T-1}p_{h(j)}\right) H_{\mathrm{out}}(h)^\dagger \left[ (U\phi_a)(U\phi_a)^\dagger\otimes \operatorname{Tr}_I\!\left( (P_b\otimes\mathbf1)H_{\mathrm{in}}(h) (\rho\otimes m_Tm_T^\dagger) H_{\mathrm{in}}(h)^\dagger(P_b^\dagger\otimes\mathbf1) \right) \right]H_{\mathrm{out}}(h).Tranc​b∈{false,true}∑​h:{0,…,T−1}→K∑​(j=0∏T−1​ph(j)​)Hout​(h)†[(Uϕa​)(Uϕa​)†⊗TrI​((Pb​⊗1)Hin​(h)(ρ⊗mT​mT†​)Hin​(h)†(Pb†​⊗1))]Hout​(h).

Here pa=0p_a=0pa​=0 and pk=1/(∣K∣−1)p_k=1/(|K|-1)pk​=1/(∣K∣−1) for k≠ak\ne ak=a, with natural-number subtraction and reciprocal zero equal to zero; Pfalse=ϕaϕa†P_{\mathrm{false}}=\phi_a\phi_a^\daggerPfalse​=ϕa​ϕa†​, Ptrue=1−ϕaϕa†P_{\mathrm{true}}=\mathbf1-\phi_a\phi_a^\daggerPtrue​=1−ϕa​ϕa†​, and mT(z)=2−T/2(−1)∣{j:zj=true}∣m_T(z)=2^{-T/2}(-1)^{|\{j:z_j=\mathrm{true}\}|}mT​(z)=2−T/2(−1)∣{j:zj​=true}∣. Outer products have entries vivi′‾v_i\overline{v_{i'}}vi​vi′​​. To specify the history matrices, put Rk=1−2ϕkϕk†R_k=\mathbf1-2\phi_k\phi_k^\daggerRk​=1−2ϕk​ϕk†​ and let C(R)C(R)C(R) have entry Ri,i′R_{i,i'}Ri,i′​ when both Boolean indices are true, δi,i′\delta_{i,i'}δi,i′​ when both are false, and zero when they differ; set

Ek=C(Rk)(1⊗H)C(Ra),Ek′=(U⊗12)Ek(U⊗12)†,H=12(111−1).E_k=C(R_k)(\mathbf1\otimes H)C(R_a), \qquad E'_k=(U\otimes\mathbf1_2)E_k(U\otimes\mathbf1_2)^\dagger, \qquad H=\frac1{\sqrt2}\begin{pmatrix}1&1\\1&-1\end{pmatrix}.Ek​=C(Rk​)(1⊗H)C(Ra​),Ek′​=(U⊗12​)Ek​(U⊗12​)†,H=2​1​(11​1−1​).

Then Hin(h)H_{\mathrm{in}}(h)Hin​(h) and Hout(h)H_{\mathrm{out}}(h)Hout​(h) are the reverse-order products of Eh(j)E_{h(j)}Eh(j)​ and Eh(j)′E'_{h(j)}Eh(j)′​, respectively, each embedded on the system and bit jjj by retaining its entries when all other bits agree and using zero otherwise. The inner partial trace sums equal III indices, and the outer partial trace sums equal length-TTT ancillary bitstrings. At T=0T=0T=0 the history products and weight are identities and 111, respectively. If KKK is a singleton and T>0T>0T>0, all history weights vanish. No normalization of ϕk\phi_kϕk​ or ρ\rhoρ, positivity of ρ\rhoρ, or unitarity of UUU is assumed.

QAlgorithms.Papers.Independent.Intakethird100.P67.encodeUnary

For an index type III, natural numbers q,Tq,Tq,T, and any vector vvv indexed by I×{false,true}TI\times\{\mathrm{false},\mathrm{true}\}^TI×{false,true}T, define utu_tut​ to be the length-TTT bit string whose coordinate jjj is true exactly when j<tj<tj<t. This defines a vector www indexed by I×{0,…,2q−1}I\times\{0,\ldots,2^q-1\}I×{0,…,2q−1} by w(i,r)=∑t=0T1{r=t}v(i,ut)w(i,r)=\sum_{t=0}^{T}\mathbf1_{\{r=t\}}v(i,u_t)w(i,r)=∑t=0T​1{r=t}​v(i,ut​); equivalently, w(i,r)=v(i,ur)w(i,r)=v(i,u_r)w(i,r)=v(i,ur​) if r≤Tr\le Tr≤T, and zero otherwise. No condition T<2qT<2^qT<2q is required: values associated with t≥2qt\ge2^qt≥2q have no output address, and values of vvv on bit strings other than the utu_tut​ are unused. When T=0T=0T=0, only address zero can have a nonzero coordinate.

QAlgorithms.Papers.Independent.Intakethird100.P67.eraseProbability

For finite index types I,LI,LI,L, arbitrary real weights pℓp_\ellpℓ​, complex matrices WℓW_\ellWℓ​ on I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true}, a vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, a natural number TTT, and a matrix ρ\rhoρ on III, this defines

Re⁡tr⁡ ⁣(ϕϕ† C T(ρ)),C(X)=∑ℓ∈Lpℓ Tr⁡bit ⁣[Wℓ(X⊗mm†)Wℓ†].\operatorname{Re}\operatorname{tr}\!\left(\phi\phi^\dagger\,\mathcal C^{\,T}(\rho)\right), \qquad \mathcal C(X)= \sum_{\ell\in L}p_\ell\, \operatorname{Tr}_{\mathrm{bit}}\!\left[ W_\ell(X\otimes mm^\dagger)W_\ell^\dagger \right].Retr(ϕϕ†CT(ρ)),C(X)=ℓ∈L∑​pℓ​Trbit​[Wℓ​(X⊗mm†)Wℓ†​].

Here (vv†)i,i′=vivi′‾(vv^\dagger)_{i,i'}=v_i\overline{v_{i'}}(vv†)i,i′​=vi​vi′​​, m=(1,−1)/2m=(1,-1)/\sqrt2m=(1,−1)/2​ in Boolean order (false,true)(\mathrm{false},\mathrm{true})(false,true), and the partial trace has entries ∑bY(i,b),(i′,b)\sum_bY_{(i,b),(i',b)}∑b​Y(i,b),(i′,b)​. The exponent on C\mathcal CC means TTT successive applications of this function, with C0\mathcal C^0C0 the identity function. Thus at T=0T=0T=0 the value is Re⁡tr⁡(ϕϕ†ρ)\operatorname{Re}\operatorname{tr}(\phi\phi^\dagger\rho)Retr(ϕϕ†ρ). No hypotheses ensure that this real number is a probability: the weights, vector, matrices, and input are unrestricted.

QAlgorithms.Papers.Independent.Intakethird100.P67.erasureGate

For a finite index type III with decidable equality, an arbitrary label type KKK, a family ϕk∈CI\phi_k\in\mathbb C^Iϕk​∈CI, and labels a,k∈Ka,k\in Ka,k∈K, this defines the matrix C(Rϕk)(II⊗H)C(Rϕa)C(R_{\phi_k})(I_I\otimes H)C(R_{\phi_a})C(Rϕk​​)(II​⊗H)C(Rϕa​​) on I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true}. Here Rϕ=II−2ϕϕ†R_\phi=I_I-2\phi\phi^\daggerRϕ​=II​−2ϕϕ†, with (ϕϕ†)ij=ϕ(i)ϕ(j)‾(\phi\phi^\dagger)_{ij}=\phi(i)\overline{\phi(j)}(ϕϕ†)ij​=ϕ(i)ϕ(j)​; C(V)C(V)C(V) preserves the Boolean coordinate and acts by VVV on its true block and by the identity on its false block; and, in Boolean order (false,true)(\mathrm{false},\mathrm{true})(false,true), H=12(111−1)H=\frac1{\sqrt2}\begin{pmatrix}1&1\\1&-1\end{pmatrix}H=2​1​(11​1−1​). The rightmost factor acts first. The labels may coincide, and no normalization of the vectors is assumed.

QAlgorithms.Papers.Independent.Intakethird100.P67.gentleChannel

For finite index types I,L,AI,L,AI,L,A, with decidable equality on III, any real-valued function p:L→Rp:L\to\mathbb Rp:L→R, complex matrix families V:L→CI×IV:L\to\mathbb C^{I\times I}V:L→CI×I and P:A→CI×IP:A\to\mathbb C^{I\times I}P:A→CI×I, and complex matrix ρ\rhoρ indexed by III, set Bℓ,a=Vℓ†PaVℓB_{\ell,a}=V_\ell^\dagger P_aV_\ellBℓ,a​=Vℓ†​Pa​Vℓ​. The definition returns

∑ℓ∈Lp(ℓ)∑a∈ABℓ,aρBℓ,a†.\sum_{\ell\in L}p(\ell)\sum_{a\in A} B_{\ell,a}\rho B_{\ell,a}^\dagger.ℓ∈L∑​p(ℓ)a∈A∑​Bℓ,a​ρBℓ,a†​.

Real weights are regarded as complex scalars. The definition imposes no positivity or normalization on ppp, no unitarity on VVV, no projector conditions on PPP, and no density-matrix conditions on ρ\rhoρ. If either summation index type is empty, the result is zero.

QAlgorithms.Papers.Independent.Intakethird100.P67.gentleProbability

For finite index types I,LI,LI,L, with decidable equality on III, an index type AAA, any function p:L→Rp:L\to\mathbb Rp:L→R, complex matrix families V:L→CI×IV:L\to\mathbb C^{I\times I}V:L→CI×I and P:A→CI×IP:A\to\mathbb C^{I\times I}P:A→CI×I, complex matrix ρ\rhoρ indexed by III, and selected label a∈Aa\in Aa∈A, the definition returns the real number

∑ℓ∈Lp(ℓ) Re⁡tr⁡(PaVℓρVℓ†).\sum_{\ell\in L}p(\ell)\, \operatorname{Re}\operatorname{tr} \left(P_aV_\ell\rho V_\ell^\dagger\right).ℓ∈L∑​p(ℓ)Retr(Pa​Vℓ​ρVℓ†​).

There are no distribution, unitarity, effect, projector, or density-matrix hypotheses on these arguments, so the definition itself does not require this number to lie in [0,1][0,1][0,1]. If LLL is empty, it is zero.

QAlgorithms.Papers.Independent.Intakethird100.P67.historyUnitary

For a finite system index type III with decidable equality, a label type LLL, a natural number TTT, a family of complex matrices WℓW_\ellWℓ​ indexed by I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true}, and a history h:{0,…,T−1}→Lh:\{0,\ldots,T-1\}\to Lh:{0,…,T−1}→L, this defines the matrix

ET−1⋯E1E0,(Ej)(i,z),(i′,z′)={(Wh(j))(i,zj),(i′,zj′),zℓ=zℓ′ for every ℓ≠j,0,otherwise,E_{T-1}\cdots E_1E_0, \qquad (E_j)_{(i,z),(i',z')}= \begin{cases} (W_{h(j)})_{(i,z_j),(i',z'_j)},&z_\ell=z'_\ell\text{ for every }\ell\ne j,\\ 0,&\text{otherwise}, \end{cases}ET−1​⋯E1​E0​,(Ej​)(i,z),(i′,z′)​={(Wh(j)​)(i,zj​),(i′,zj′​)​,0,​zℓ​=zℓ′​ for every ℓ=j,otherwise,​

where z,z′z,z'z,z′ are bitstrings of length TTT. Thus the factor with index 000 acts first under matrix multiplication on column vectors. For T=0T=0T=0, the result is the identity matrix. No unitarity assumption is imposed on the matrices WℓW_\ellWℓ​.

QAlgorithms.Papers.Independent.Intakethird100.P67.historyWeight

For a label type LLL, a natural number TTT, an arbitrary real-valued function p:L→Rp:L\to\mathbb Rp:L→R, and a history h:{0,…,T−1}→Lh:\{0,\ldots,T-1\}\to Lh:{0,…,T−1}→L, this defines the real number

∏j=0T−1p(h(j)).\prod_{j=0}^{T-1}p(h(j)).j=0∏T−1​p(h(j)).

The function ppp need not be nonnegative or sum to one. For T=0T=0T=0, the product is 111, including when LLL is empty.

QAlgorithms.Papers.Independent.Intakethird100.P67.increment

For every natural number qqq, put N=2qN=2^qN=2q. This defines the N×NN\times NN×N complex matrix whose entry at row xxx and column yyy is one if x=(y+1) mod Nx=(y+1)\bmod Nx=(y+1)modN, and zero otherwise, for 0≤x,y<N0\le x,y<N0≤x,y<N. Thus it shifts each coordinate basis vector forward by one modulo NNN. In particular, q=0q=0q=0 gives the 1×11\times11×1 identity matrix.

QAlgorithms.Papers.Independent.Intakethird100.P67.inputOutputRecords

For a label type KKK, a finite coordinate type III, any family of complex vectors ϕk∈CI\phi_k\in\mathbb C^Iϕk​∈CI, and any complex matrix UUU on III, this definition assigns to each Boolean-label pair (b,k)(b,k)(b,k) the matrix

Rb,k={U ∣ϕk⟩⟨ϕk∣ U†,b=true,∣ϕk⟩⟨ϕk∣,b=false,(∣ϕk⟩⟨ϕk∣)ij=ϕk(i)ϕk(j)‾.R_{b,k}= \begin{cases} U\,|\phi_k\rangle\langle\phi_k|\,U^\dagger,&b=\mathrm{true},\\ |\phi_k\rangle\langle\phi_k|,&b=\mathrm{false}, \end{cases} \qquad (|\phi_k\rangle\langle\phi_k|)_{ij} =\phi_k(i)\overline{\phi_k(j)}.Rb,k​={U∣ϕk​⟩⟨ϕk​∣U†,∣ϕk​⟩⟨ϕk​∣,​b=true,b=false,​(∣ϕk​⟩⟨ϕk​∣)ij​=ϕk​(i)ϕk​(j)​.

Neither normalization of the vectors nor unitarity of UUU is assumed; an empty label type or empty coordinate type is allowed.

QAlgorithms.Papers.Independent.Intakethird100.P67.jointBranch

For finite index types I,J,LI,J,LI,J,L, with decidable equality on the system indices, arbitrary weights p:L→Rp:L\to\mathbb Rp:L→R, matrix families WℓinW^{\mathrm{in}}_\ellWℓin​ on I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true} and WℓoutW^{\mathrm{out}}_\ellWℓout​ on J×{false,true}J\times\{\mathrm{false},\mathrm{true}\}J×{false,true}, vectors ϕ∈CI\phi\in\mathbb C^Iϕ∈CI and ϕout∈CJ\phi_{\mathrm{out}}\in\mathbb C^Jϕout​∈CJ, a natural number TTT, a Boolean bbb, and a matrix ρ\rhoρ on III, this defines

∑h:{0,…,T−1}→L(∏j=0T−1p(h(j)))Hout(h)†[ϕoutϕout†⊗Tr⁡I ⁣((Pb⊗1)Hin(h)(ρ⊗mTmT†)Hin(h)†(Pb†⊗1))]Hout(h).\sum_{h:\{0,\ldots,T-1\}\to L} \left(\prod_{j=0}^{T-1}p(h(j))\right) H_{\mathrm{out}}(h)^\dagger \left[ \phi_{\mathrm{out}}\phi_{\mathrm{out}}^\dagger\otimes \operatorname{Tr}_I\!\left( (P_b\otimes\mathbf1)H_{\mathrm{in}}(h) (\rho\otimes m_Tm_T^\dagger) H_{\mathrm{in}}(h)^\dagger(P_b^\dagger\otimes\mathbf1) \right) \right]H_{\mathrm{out}}(h).h:{0,…,T−1}→L∑​(j=0∏T−1​p(h(j)))Hout​(h)†[ϕout​ϕout†​⊗TrI​((Pb​⊗1)Hin​(h)(ρ⊗mT​mT†​)Hin​(h)†(Pb†​⊗1))]Hout​(h).

Here Pfalse=ϕϕ†P_{\mathrm{false}}=\phi\phi^\daggerPfalse​=ϕϕ†, Ptrue=1−ϕϕ†P_{\mathrm{true}}=\mathbf1-\phi\phi^\daggerPtrue​=1−ϕϕ†, outer products have entries vivi′‾v_i\overline{v_{i'}}vi​vi′​​, and mT(z)=2−T/2(−1)∣{j:zj=true}∣m_T(z)=2^{-T/2}(-1)^{|\{j:z_j=\mathrm{true}\}|}mT​(z)=2−T/2(−1)∣{j:zj​=true}∣. Each Hin/out(h)H_{\mathrm{in/out}}(h)Hin/out​(h) is ET−1⋯E0E_{T-1}\cdots E_0ET−1​⋯E0​, with (Ej)(i,z),(i′,z′)=(Wh(j)in/out)(i,zj),(i′,zj′)(E_j)_{(i,z),(i',z')}=(W^{\mathrm{in/out}}_{h(j)})_{(i,z_j),(i',z'_j)}(Ej​)(i,z),(i′,z′)​=(Wh(j)in/out​)(i,zj​),(i′,zj′​)​ if the bitstrings agree outside jjj, and zero otherwise; Tr⁡I\operatorname{Tr}_ITrI​ sums equal system indices. No positivity, normalization, or unitarity hypotheses are imposed. At T=0T=0T=0 there is one empty history of weight 111, even if LLL is empty, and both history products are identities; if LLL is empty and T>0T>0T>0, the sum is zero.

QAlgorithms.Papers.Independent.Intakethird100.P67.jointBranchHistory

For finite system index types I,JI,JI,J with decidable equality, a label type LLL, a natural number TTT, arbitrary matrix families WℓinW^{\mathrm{in}}_\ellWℓin​ on I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true} and WℓoutW^{\mathrm{out}}_\ellWℓout​ on J×{false,true}J\times\{\mathrm{false},\mathrm{true}\}J×{false,true}, vectors ϕ∈CI\phi\in\mathbb C^Iϕ∈CI and ϕout∈CJ\phi_{\mathrm{out}}\in\mathbb C^Jϕout​∈CJ, a history h:{0,…,T−1}→Lh:\{0,\ldots,T-1\}\to Lh:{0,…,T−1}→L, a Boolean bbb, and an arbitrary matrix ρ\rhoρ on III, this defines

Hout†[ϕoutϕout†⊗Tr⁡I ⁣((Pb⊗1)Hin(ρ⊗mTmT†)Hin†(Pb†⊗1))]Hout.H_{\mathrm{out}}^\dagger \left[ \phi_{\mathrm{out}}\phi_{\mathrm{out}}^\dagger\otimes \operatorname{Tr}_I\!\left( (P_b\otimes\mathbf1)H_{\mathrm{in}} (\rho\otimes m_Tm_T^\dagger) H_{\mathrm{in}}^\dagger(P_b^\dagger\otimes\mathbf1) \right) \right]H_{\mathrm{out}}.Hout†​[ϕout​ϕout†​⊗TrI​((Pb​⊗1)Hin​(ρ⊗mT​mT†​)Hin†​(Pb†​⊗1))]Hout​.

Here Pfalse=ϕϕ†P_{\mathrm{false}}=\phi\phi^\daggerPfalse​=ϕϕ†, Ptrue=1−ϕϕ†P_{\mathrm{true}}=\mathbf1-\phi\phi^\daggerPtrue​=1−ϕϕ†, (vv†)i,i′=vivi′‾(vv^\dagger)_{i,i'}=v_i\overline{v_{i'}}(vv†)i,i′​=vi​vi′​​, and mT(z)=2−T/2(−1)∣{j:zj=true}∣m_T(z)=2^{-T/2}(-1)^{|\{j:z_j=\mathrm{true}\}|}mT​(z)=2−T/2(−1)∣{j:zj​=true}∣ for each length-TTT bitstring zzz. Each Hin/outH_{\mathrm{in/out}}Hin/out​ is the product ET−1⋯E0E_{T-1}\cdots E_0ET−1​⋯E0​, where EjE_jEj​ has entry (Wh(j)in/out)(i,zj),(i′,zj′)(W^{\mathrm{in/out}}_{h(j)})_{(i,z_j),(i',z'_j)}(Wh(j)in/out​)(i,zj​),(i′,zj′​)​ when z,z′z,z'z,z′ agree outside jjj, and zero otherwise. The partial trace is (Tr⁡IX)z,z′=∑iX(i,z),(i,z′)(\operatorname{Tr}_IX)_{z,z'}=\sum_iX_{(i,z),(i,z')}(TrI​X)z,z′​=∑i​X(i,z),(i,z′)​. For T=0T=0T=0, both history products are identities and the ancillary space has one coordinate with m0=1m_0=1m0​=1. No vector normalization, matrix positivity, or unitarity is assumed.

QAlgorithms.Papers.Independent.Intakethird100.P67.jointEmulator

For finite index types I,J,LI,J,LI,J,L, with decidable equality on the system indices, arbitrary real weights pℓp_\ellpℓ​, matrix families WℓinW^{\mathrm{in}}_\ellWℓin​ on I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true} and WℓoutW^{\mathrm{out}}_\ellWℓout​ on J×{false,true}J\times\{\mathrm{false},\mathrm{true}\}J×{false,true}, vectors ϕ∈CI\phi\in\mathbb C^Iϕ∈CI and ϕout∈CJ\phi_{\mathrm{out}}\in\mathbb C^Jϕout​∈CJ, a natural number TTT, and a matrix ρ\rhoρ on III, this defines

∑b∈{false,true}∑h:{0,…,T−1}→L(∏j=0T−1p(h(j)))Hout(h)†[ϕoutϕout†⊗Tr⁡I ⁣((Pb⊗1)Hin(h)(ρ⊗mTmT†)Hin(h)†(Pb†⊗1))]Hout(h).\sum_{b\in\{\mathrm{false},\mathrm{true}\}} \sum_{h:\{0,\ldots,T-1\}\to L} \left(\prod_{j=0}^{T-1}p(h(j))\right) H_{\mathrm{out}}(h)^\dagger \left[ \phi_{\mathrm{out}}\phi_{\mathrm{out}}^\dagger\otimes \operatorname{Tr}_I\!\left( (P_b\otimes\mathbf1)H_{\mathrm{in}}(h) (\rho\otimes m_Tm_T^\dagger) H_{\mathrm{in}}(h)^\dagger(P_b^\dagger\otimes\mathbf1) \right) \right]H_{\mathrm{out}}(h).b∈{false,true}∑​h:{0,…,T−1}→L∑​(j=0∏T−1​p(h(j)))Hout​(h)†[ϕout​ϕout†​⊗TrI​((Pb​⊗1)Hin​(h)(ρ⊗mT​mT†​)Hin​(h)†(Pb†​⊗1))]Hout​(h).

Here Pfalse=ϕϕ†P_{\mathrm{false}}=\phi\phi^\daggerPfalse​=ϕϕ†, Ptrue=1−ϕϕ†P_{\mathrm{true}}=\mathbf1-\phi\phi^\daggerPtrue​=1−ϕϕ†, (vv†)i,i′=vivi′‾(vv^\dagger)_{i,i'}=v_i\overline{v_{i'}}(vv†)i,i′​=vi​vi′​​, and mT(z)=2−T/2(−1)∣{j:zj=true}∣m_T(z)=2^{-T/2}(-1)^{|\{j:z_j=\mathrm{true}\}|}mT​(z)=2−T/2(−1)∣{j:zj​=true}∣. Each Hin/out(h)=ET−1⋯E0H_{\mathrm{in/out}}(h)=E_{T-1}\cdots E_0Hin/out​(h)=ET−1​⋯E0​, where EjE_jEj​ acts through Wh(j)in/outW^{\mathrm{in/out}}_{h(j)}Wh(j)in/out​ on the system and bit jjj: its entry is (Wh(j)in/out)(i,zj),(i′,zj′)(W^{\mathrm{in/out}}_{h(j)})_{(i,z_j),(i',z'_j)}(Wh(j)in/out​)(i,zj​),(i′,zj′​)​ when all other bits agree, and zero otherwise. The partial trace sums equal system indices. No normalization, positivity, or unitarity is required. For T=0T=0T=0, the sole history has weight 111 and identity history matrices; for empty LLL and positive TTT, the result is zero.

QAlgorithms.Papers.Independent.Intakethird100.P67.lambdaPerp

For finite index types I,KI,KI,K with decidable equality, any family ϕ:K→CI\phi:K\to\mathbb C^Iϕ:K→CI, and an anchor a∈Ka\in Ka∈K, set (Dk)ij=ϕk(i)ϕk(j)‾(D_k)_{ij}=\phi_k(i)\overline{\phi_k(j)}(Dk​)ij​=ϕk​(i)ϕk​(j)​, Π=f(∑kDk)\Pi=f(\sum_kD_k)Π=f(∑k​Dk​) by matrix functional calculus with f(0)=0f(0)=0f(0)=0 and f(x)=1f(x)=1f(x)=1 for x≠0x\ne0x=0, and Ck=(Π−Da)(Id−2Dk)(Π−Da)C_k=(\Pi-D_a)(\mathrm{Id}-2D_k)(\Pi-D_a)Ck​=(Π−Da​)(Id−2Dk​)(Π−Da​). With pa(a)=0p_a(a)=0pa​(a)=0 and pa(k)=1/(∣K∣−1)p_a(k)=1/(|K|-1)pa​(k)=1/(∣K∣−1) for k≠ak\ne ak=a, the definition returns the Euclidean operator norm

∥∑k∈Kpa(k) Ck⊗Ck‾∥2→2,\left\|\sum_{k\in K}p_a(k)\,C_k\otimes\overline{C_k}\right\|_{2\to2},​k∈K∑​pa​(k)Ck​⊗Ck​​​2→2​,

where the bar means entrywise complex conjugation and ⊗\otimes⊗ is the Kronecker product. No normalization of the vectors is required. If KKK consists only of aaa, this value is zero; the reciprocal convention is 1/0=01/0=01/0=0.

QAlgorithms.Papers.Independent.Intakethird100.P67.meanSampleDensity

For any index type III, finite index type KKK, and family ϕ:K→CI\phi:K\to\mathbb C^Iϕ:K→CI, the definition returns the complex matrix

Mij=1∣K∣∑k∈Kϕk(i)ϕk(j)‾.M_{ij}=\frac1{|K|}\sum_{k\in K}\phi_k(i)\overline{\phi_k(j)}.Mij​=∣K∣1​k∈K∑​ϕk​(i)ϕk​(j)​.

The vectors are arbitrary and need not have norm one. If KKK is empty, the sum and the resulting matrix are zero, with the reciprocal of zero interpreted as zero.

QAlgorithms.Papers.Independent.Intakethird100.P67.minusRegister

For every natural number TTT, including T=0T=0T=0, this defines a complex vector indexed by Boolean strings z:{0,…,T−1}→{false,true}z:\{0,\ldots,T-1\}\to\{\mathrm{false},\mathrm{true}\}z:{0,…,T−1}→{false,true}, with coordinate ∏j=0T−1c(zj)\prod_{j=0}^{T-1}c(z_j)∏j=0T−1​c(zj​), where c(false)=1/2c(\mathrm{false})=1/\sqrt2c(false)=1/2​ and c(true)=−1/2c(\mathrm{true})=-1/\sqrt2c(true)=−1/2​. Equivalently, its coordinate is 2−T/2(−1)∣{j:zj=true}∣2^{-T/2}(-1)^{|\{j:z_j=\mathrm{true}\}|}2−T/2(−1)∣{j:zj​=true}∣. When T=0T=0T=0, there is one empty string and its coordinate is the empty product 111.

QAlgorithms.Papers.Independent.Intakethird100.P67.minusVector

This defines the complex vector indexed by the two Boolean values whose false coordinate is 1/21/\sqrt21/2​ and whose true coordinate is −1/2-1/\sqrt2−1/2​, namely (1/2,−1/2)(1/\sqrt2,-1/\sqrt2)(1/2​,−1/2​) in Boolean order (false,true)(\mathrm{false},\mathrm{true})(false,true).

QAlgorithms.Papers.Independent.Intakethird100.P67.mixedEmulate

For finite index types I,KI,KI,K, any family S:K→Mat⁡I(C)S:K\to\operatorname{Mat}_I(\mathbb C)S:K→MatI​(C), anchor a∈Ka\in Ka∈K, vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, arbitrary matrices U,ρ∈Mat⁡I(C)U,\rho\in\operatorname{Mat}_I(\mathbb C)U,ρ∈MatI​(C), and natural number TTT, this defines the matrix whose entries are

∣K∣−T∑h:{0,…,T−1}→K∫[0,1]T[Tr⁡anc(Vout†((Uϕ)(Uϕ)†⊗Tr⁡IX)Vout)]ij dt.|K|^{-T}\sum_{h:\{0,\ldots,T-1\}\to K} \int_{[0,1]^T} \left[ \operatorname{Tr}_{\mathrm{anc}} \left( V_{\mathrm{out}}^\dagger \left((U\phi)(U\phi)^\dagger\otimes\operatorname{Tr}_{I}X\right) V_{\mathrm{out}} \right) \right]_{ij}\,d\mathbf t.∣K∣−Th:{0,…,T−1}→K∑​∫[0,1]T​[Tranc​(Vout†​((Uϕ)(Uϕ)†⊗TrI​X)Vout​)]ij​dt.

For each history and parameter tuple, Vin=AT−1⋯A0V_{\mathrm{in}}=A_{T-1}\cdots A_0Vin​=AT−1​⋯A0​, where AjA_jAj​ acts on the system and Boolean register jjj by C(e−itjShj)(1⊗H)C(e−iπSa)C(e^{-it_jS_{h_j}})(1\otimes H)C(e^{-i\pi S_a})C(e−itj​Shj​​)(1⊗H)C(e−iπSa​) and preserves the other registers; C(M)C(M)C(M) applies 111 in the false sector and MMM in the true sector, and H=2−1/2(111−1)H=2^{-1/2}\begin{pmatrix}1&1\\1&-1\end{pmatrix}H=2−1/2(11​1−1​). Further,

mT(z)=∏j<T(−1)zj2,X=Vin(ρ⊗mTmT†)Vin†,Vout=(U⊗1)Vin(U†⊗1).m_T(z)=\prod_{j<T}\frac{(-1)^{z_j}}{\sqrt2},\qquad X=V_{\mathrm{in}}(\rho\otimes m_Tm_T^\dagger)V_{\mathrm{in}}^\dagger,\qquad V_{\mathrm{out}}=(U\otimes1)V_{\mathrm{in}}(U^\dagger\otimes1).mT​(z)=j<T∏​2​(−1)zj​​,X=Vin​(ρ⊗mT​mT†​)Vin†​,Vout​=(U⊗1)Vin​(U†⊗1).

The partial traces sum matching indices of the indicated register, and the integral is entrywise with respect to product Lebesgue measure. The histories include occurrences of the anchor. No normalization, positivity, Hermitian, or unitarity hypotheses are imposed. The anchor requires K≠∅K\ne\varnothingK=∅; T=0T=0T=0 is allowed, with one empty history, normalization factor 111, and integration over the singleton empty tuple.

QAlgorithms.Papers.Independent.Intakethird100.P67.mixedGate

For a finite coordinate index type III, any family S:K→Mat⁡I(C)S:K\to\operatorname{Mat}_I(\mathbb C)S:K→MatI​(C), indices a,k∈Ka,k\in Ka,k∈K, and real number ttt, this defines

C ⁣(e−itSk)(1⊗H)C ⁣(e−iπSa),H=12(111−1),C\!\left(e^{-itS_k}\right)(1\otimes H) C\!\left(e^{-i\pi S_a}\right), \qquad H=\frac1{\sqrt2}\begin{pmatrix}1&1\\1&-1\end{pmatrix},C(e−itSk​)(1⊗H)C(e−iπSa​),H=2​1​(11​1−1​),

on the system and a Boolean register ordered false, true. Here C(M)C(M)C(M) preserves the Boolean register, applies the identity to the system when that register is false, and applies MMM when it is true; the rightmost factor acts first. The matrices SkS_kSk​ need not be Hermitian, and ttt is unrestricted, so unitarity is not an input hypothesis.

QAlgorithms.Papers.Independent.Intakethird100.P67.mixedHistory

For a finite coordinate index type III, any index type KKK, family S:K→Mat⁡I(C)S:K\to\operatorname{Mat}_I(\mathbb C)S:K→MatI​(C), anchor a∈Ka\in Ka∈K, natural number TTT, history h:{0,…,T−1}→Kh:\{0,\ldots,T-1\}\to Kh:{0,…,T−1}→K, and real parameters (tj)j<T(t_j)_{j<T}(tj​)j<T​, this defines

AT−1⋯A1A0,A_{T-1}\cdots A_1A_0,AT−1​⋯A1​A0​,

where AjA_jAj​ acts on the system and Boolean register jjj by

Gj=C(e−itjShj)(1⊗H)C(e−iπSa),H=12(111−1),G_j=C(e^{-it_jS_{h_j}})(1\otimes H)C(e^{-i\pi S_a}), \qquad H=\frac1{\sqrt2}\begin{pmatrix}1&1\\1&-1\end{pmatrix},Gj​=C(e−itj​Shj​​)(1⊗H)C(e−iπSa​),H=2​1​(11​1−1​),

and preserves all other Boolean registers. Explicitly, (Aj)(i,z),(i′,z′)=(Gj)(i,zj),(i′,zj′)(A_j)_{(i,z),(i',z')}=(G_j)_{(i,z_j),(i',z'_j)}(Aj​)(i,z),(i′,z′)​=(Gj​)(i,zj​),(i′,zj′​)​ when zℓ=zℓ′z_\ell=z'_\ellzℓ​=zℓ′​ for every ℓ≠j\ell\ne jℓ=j, and is zero otherwise; C(M)C(M)C(M) applies 111 in the false sector and MMM in the true sector. No Hermitian assumptions or bounds on the real parameters are imposed. For T=0T=0T=0, the product is the identity.

QAlgorithms.Papers.Independent.Intakethird100.P67.mixedHistoryOutput

For a finite coordinate index type III, any index type KKK, family S:K→Mat⁡I(C)S:K\to\operatorname{Mat}_I(\mathbb C)S:K→MatI​(C), anchor a∈Ka\in Ka∈K, vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, arbitrary matrices U,ρ∈Mat⁡I(C)U,\rho\in\operatorname{Mat}_I(\mathbb C)U,ρ∈MatI​(C), natural number TTT, history h:{0,…,T−1}→Kh:\{0,\ldots,T-1\}\to Kh:{0,…,T−1}→K, and real parameters (tj)j<T(t_j)_{j<T}(tj​)j<T​, let Vin=AT−1⋯A0V_{\mathrm{in}}=A_{T-1}\cdots A_0Vin​=AT−1​⋯A0​, where AjA_jAj​ acts on the system and Boolean register jjj by C(e−itjShj)(1⊗H)C(e−iπSa)C(e^{-it_jS_{h_j}})(1\otimes H)C(e^{-i\pi S_a})C(e−itj​Shj​​)(1⊗H)C(e−iπSa​) and preserves the other registers; here C(M)C(M)C(M) applies 111 in the false sector and MMM in the true sector, and H=2−1/2(111−1)H=2^{-1/2}\begin{pmatrix}1&1\\1&-1\end{pmatrix}H=2−1/2(11​1−1​). With

mT(z)=∏j=0T−1(−1)zj2,X=Vin(ρ⊗mTmT†)Vin†,Vout=(U⊗1)Vin(U†⊗1),m_T(z)=\prod_{j=0}^{T-1}\frac{(-1)^{z_j}}{\sqrt2},\qquad X=V_{\mathrm{in}}(\rho\otimes m_Tm_T^\dagger)V_{\mathrm{in}}^\dagger,\qquad V_{\mathrm{out}}=(U\otimes1)V_{\mathrm{in}}(U^\dagger\otimes1),mT​(z)=j=0∏T−1​2​(−1)zj​​,X=Vin​(ρ⊗mT​mT†​)Vin†​,Vout​=(U⊗1)Vin​(U†⊗1),

the definition returns

Tr⁡anc[Vout†((Uϕ)(Uϕ)†⊗Tr⁡IX)Vout].\operatorname{Tr}_{\mathrm{anc}} \left[ V_{\mathrm{out}}^\dagger \left((U\phi)(U\phi)^\dagger\otimes\operatorname{Tr}_{I}X\right) V_{\mathrm{out}} \right].Tranc​[Vout†​((Uϕ)(Uϕ)†⊗TrI​X)Vout​].

The partial traces sum matching indices of the indicated register. No normalization, positivity, Hermitian, or unitarity hypotheses are imposed. The case T=0T=0T=0 is included: mT=1m_T=1mT​=1, Vin=1V_{\mathrm{in}}=1Vin​=1, and Vout=UU†V_{\mathrm{out}}=UU^\daggerVout​=UU† under the empty-register identification.

QAlgorithms.Papers.Independent.Intakethird100.P67.mixedSampleErasureChannel

For finite index types I,KI,KI,K, any family S:K→Mat⁡I(C)S:K\to\operatorname{Mat}_I(\mathbb C)S:K→MatI​(C), anchor a∈Ka\in Ka∈K, and arbitrary matrix ρ∈Mat⁡I(C)\rho\in\operatorname{Mat}_I(\mathbb C)ρ∈MatI​(C), this defines the matrix with entries

1∣K∣∑k∈K∫[0,1][Tr⁡Bool(Ga,k(t)(ρ⊗mm†)Ga,k(t)†)]ij dt,\frac1{|K|}\sum_{k\in K}\int_{[0,1]} \left[ \operatorname{Tr}_{\mathrm{Bool}} \left(G_{a,k}(t)(\rho\otimes mm^\dagger)G_{a,k}(t)^\dagger\right) \right]_{ij}\,dt,∣K∣1​k∈K∑​∫[0,1]​[TrBool​(Ga,k​(t)(ρ⊗mm†)Ga,k​(t)†)]ij​dt,

where mfalse=1/2m_{\mathrm{false}}=1/\sqrt2mfalse​=1/2​, mtrue=−1/2m_{\mathrm{true}}=-1/\sqrt2mtrue​=−1/2​, and

Ga,k(t)=C(e−itSk)(1⊗H)C(e−iπSa),H=12(111−1).G_{a,k}(t)=C(e^{-itS_k})(1\otimes H)C(e^{-i\pi S_a}), \qquad H=\frac1{\sqrt2}\begin{pmatrix}1&1\\1&-1\end{pmatrix}.Ga,k​(t)=C(e−itSk​)(1⊗H)C(e−iπSa​),H=2​1​(11​1−1​).

The controlled matrix C(M)C(M)C(M) applies 111 on the false Boolean sector and MMM on the true sector, and the partial trace sums the two matching Boolean indices. The integral is taken entry by entry with respect to Lebesgue measure. The sum includes k=ak=ak=a; the existence of aaa requires KKK to be nonempty. No Hermitian condition on SkS_kSk​ or density-matrix condition on ρ\rhoρ is imposed.

QAlgorithms.Papers.Independent.Intakethird100.P67.negativeFourier

For every natural number ddd, this defines the complex matrix with rows and columns indexed by 0,…,d−10,\ldots,d-10,…,d−1 and entries Fjk=(d)−1exp⁡(−2πijk/d)F_{jk}=(\sqrt d)^{-1}\exp(-2\pi\mathrm{i}jk/d)Fjk​=(d​)−1exp(−2πijk/d). For d=0d=0d=0, this is the empty matrix, so there are no entries at which the division by ddd is evaluated.

QAlgorithms.Papers.Independent.Intakethird100.P67.nonanchorProbability

For a finite type KKK with decidable equality and elements a,k∈Ka,k\in Ka,k∈K, this defines

{0,k=a,1max⁡(∣K∣−1,0),k≠a,\begin{cases} 0,&k=a,\\ \displaystyle\frac1{\max(|K|-1,0)},&k\ne a, \end{cases}⎩⎨⎧​0,max(∣K∣−1,0)1​,​k=a,k=a,​

where the subtraction is performed in the natural numbers before conversion to a real number, and the reciprocal of zero is defined to be zero. In particular, when ∣K∣=1|K|=1∣K∣=1, the function is identically zero. If KKK is empty, there are no elements a,ka,ka,k to which the definition can be applied.

QAlgorithms.Papers.Independent.Intakethird100.P67.onAncilla

For an index type III, a natural number TTT, a complex matrix VVV indexed by I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true}, and an index j∈{0,…,T−1}j\in\{0,\ldots,T-1\}j∈{0,…,T−1}, this defines a matrix indexed by I×{false,true}TI\times\{\mathrm{false},\mathrm{true}\}^TI×{false,true}T. For system indices i,i′∈Ii,i'\in Ii,i′∈I and bitstrings z,z′z,z'z,z′ of length TTT, its entry is

{V(i,zj),(i′,zj′),zℓ=zℓ′ for every ℓ≠j,0,otherwise.\begin{cases} V_{(i,z_j),(i',z'_j)},&z_\ell=z'_\ell\text{ for every }\ell\ne j,\\ 0,&\text{otherwise}. \end{cases}{V(i,zj​),(i′,zj′​)​,0,​zℓ​=zℓ′​ for every ℓ=j,otherwise.​

There is no assumption that VVV is unitary. When T=0T=0T=0, there is no admissible index jjj.

QAlgorithms.Papers.Independent.Intakethird100.P67.positivePhaseEvolution

For a finite index type III with decidable equality, any complex matrix HHH indexed by III, and any real number θ\thetaθ, the definition returns the matrix exponential

exp⁡(iθH)=∑m=0∞(iθH)mm!.\exp(i\theta H)=\sum_{m=0}^{\infty}\frac{(i\theta H)^m}{m!}.exp(iθH)=m=0∑∞​m!(iθH)m​.

There is no Hermitian hypothesis on HHH or restriction on θ\thetaθ; in particular, θ=0\theta=0θ=0 returns the identity matrix.

QAlgorithms.Papers.Independent.Intakethird100.P67.precisionRounds

For every natural number ddd, including 000, and arbitrary real numbers λ,ε\lambda,\varepsilonλ,ε, this defines the natural number

precisionRounds⁡(d,λ,ε)={0,d≤1,max⁡ ⁣{1, ⌈log⁡ ⁣(8(ε−1)2(d−1))1−λ⌉N},d>1.\operatorname{precisionRounds}(d,\lambda,\varepsilon)= \begin{cases} 0,&d\le1,\\[2mm] \displaystyle \max\!\left\{1,\ \left\lceil \frac{\log\!\left(8(\varepsilon^{-1})^2(d-1)\right)} {1-\lambda} \right\rceil_{\mathbb N}\right\},&d>1. \end{cases}precisionRounds(d,λ,ε)=⎩⎨⎧​0,max{1, ⌈1−λlog(8(ε−1)2(d−1))​⌉N​},​d≤1,d>1.​

Here d−1d-1d−1 inside the logarithm is real subtraction, and ⌈x⌉N\lceil x\rceil_{\mathbb N}⌈x⌉N​ is the least natural number at least xxx, giving 000 for x≤0x\le0x≤0. There are no restrictions on λ\lambdaλ or ε\varepsilonε: inverses and division are total, with 0−1=00^{-1}=00−1=0 and division by zero equal to zero, while the real logarithm has log⁡0=0\log0=0log0=0 and log⁡(−x)=log⁡x\log(-x)=\log xlog(−x)=logx. Consequently, for d>1d>1d>1, either ε=0\varepsilon=0ε=0 or λ=1\lambda=1λ=1 gives the value 111.

QAlgorithms.Papers.Independent.Intakethird100.P67.projectionBranch

For finite index types I,KI,KI,K with decidable equality, any family ϕ:K→CI\phi:K\to\mathbb C^Iϕ:K→CI, natural number TTT, Boolean bbb, and complex matrix ρ\rhoρ indexed by III, put (Dk)ij=ϕk(i)ϕk(j)‾(D_k)_{ij}=\phi_k(i)\overline{\phi_k(j)}(Dk​)ij​=ϕk​(i)ϕk​(j)​ and Rk=Id−2DkR_k=\mathrm{Id}-2D_kRk​=Id−2Dk​. Let mTm_TmT​ be the vector on length-TTT Boolean words with mT(z)=2−T/2(−1)∣{j:zj=true}∣m_T(z)=2^{-T/2}(-1)^{|\{j:z_j=\mathrm{true}\}|}mT​(z)=2−T/2(−1)∣{j:zj​=true}∣, and set P=Id⊗mTmT†P=\mathrm{Id}\otimes m_Tm_T^\daggerP=Id⊗mT​mT†​. For each history h:{0,…,T−1}→Kh:\{0,\ldots,T-1\}\to Kh:{0,…,T−1}→K, let Gh,jG_{h,j}Gh,j​ apply Rh(j)R_{h(j)}Rh(j)​ to the system when ancilla bit jjj is true and apply the identity when it is false, leaving every other ancilla bit unchanged, and set Vh=Gh,T−1⋯Gh,0V_h=G_{h,T-1}\cdots G_{h,0}Vh​=Gh,T−1​⋯Gh,0​, with the empty product equal to the identity. Taking Qb=PQ_b=PQb​=P if bbb is true and Qb=Id−PQ_b=\mathrm{Id}-PQb​=Id−P otherwise, the definition returns

(∣K∣T)−1∑hTr⁡anc[Vh†QbVh(ρ⊗mTmT†)Vh†Qb†Vh],(|K|^T)^{-1}\sum_h \operatorname{Tr}_{\mathrm{anc}} \left[ V_h^\dagger Q_bV_h (\rho\otimes m_Tm_T^\dagger) V_h^\dagger Q_b^\dagger V_h \right],(∣K∣T)−1h∑​Tranc​[Vh†​Qb​Vh​(ρ⊗mT​mT†​)Vh†​Qb†​Vh​],

where (Tr⁡ancX)ij=∑zX(i,z),(j,z)(\operatorname{Tr}_{\mathrm{anc}}X)_{ij}=\sum_zX_{(i,z),(j,z)}(Tranc​X)ij​=∑z​X(i,z),(j,z)​. No normalization, positivity, or unitarity hypotheses are imposed on ϕ,ρ\phi,\rhoϕ,ρ, or the resulting matrices VhV_hVh​. For T=0T=0T=0, the true branch returns ρ\rhoρ and the false branch returns zero; if KKK is empty and T>0T>0T>0, both return zero. Reciprocals use 0−1=00^{-1}=00−1=0, and 00=10^0=100=1.

QAlgorithms.Papers.Independent.Intakethird100.P67.projectionChannel

For finite index types I,KI,KI,K with decidable equality, any family ϕ:K→CI\phi:K\to\mathbb C^Iϕ:K→CI, natural number TTT, and complex matrix ρ\rhoρ indexed by III, define DkD_kDk​ by (Dk)ij=ϕk(i)ϕk(j)‾(D_k)_{ij}=\phi_k(i)\overline{\phi_k(j)}(Dk​)ij​=ϕk​(i)ϕk​(j)​, let mT(z)=2−T/2(−1)∣{j:zj=true}∣m_T(z)=2^{-T/2}(-1)^{|\{j:z_j=\mathrm{true}\}|}mT​(z)=2−T/2(−1)∣{j:zj​=true}∣ on length-TTT Boolean words, and put P=Id⊗mTmT†P=\mathrm{Id}\otimes m_Tm_T^\daggerP=Id⊗mT​mT†​. For each history h:{0,…,T−1}→Kh:\{0,\ldots,T-1\}\to Kh:{0,…,T−1}→K, form Vh=Gh,T−1⋯Gh,0V_h=G_{h,T-1}\cdots G_{h,0}Vh​=Gh,T−1​⋯Gh,0​, where Gh,jG_{h,j}Gh,j​ applies Id−2Dh(j)\mathrm{Id}-2D_{h(j)}Id−2Dh(j)​ to the system conditional on ancilla bit jjj being true and leaves the other ancillas unchanged. The definition returns

(∣K∣T)−1∑h∑Q∈{Id−P,P}Tr⁡anc[Vh†QVh(ρ⊗mTmT†)Vh†Q†Vh],(|K|^T)^{-1}\sum_h\sum_{Q\in\{\mathrm{Id}-P,P\}} \operatorname{Tr}_{\mathrm{anc}} \left[ V_h^\dagger QV_h(\rho\otimes m_Tm_T^\dagger) V_h^\dagger Q^\dagger V_h \right],(∣K∣T)−1h∑​Q∈{Id−P,P}∑​Tranc​[Vh†​QVh​(ρ⊗mT​mT†​)Vh†​Q†Vh​],

where the inner sum means the two displayed choices, and partial trace sums equal ancilla indices. There are no normalization or positivity assumptions on the inputs. For T=0T=0T=0 it returns ρ\rhoρ; for empty KKK and T>0T>0T>0 it returns zero, using 0−1=00^{-1}=00−1=0 and 00=10^0=100=1.

QAlgorithms.Papers.Independent.Intakethird100.P67.pureFisherInformation

For a coordinate index type III, a function v:R→CIv:\mathbb R\to\mathbb C^Iv:R→CI in complex Euclidean space, and any α∈R\alpha\in\mathbb Rα∈R, this defines the real number

4(∥v′(α)∥2−∣⟨v(α),v′(α)⟩C∣2).4\left(\|v'(\alpha)\|^2-\left|\langle v(\alpha),v'(\alpha)\rangle_{\mathbb C}\right|^2\right).4(∥v′(α)∥2−∣⟨v(α),v′(α)⟩C​∣2).

The complex inner product conjugates its first argument. No normalization or differentiability hypothesis is imposed on vvv; the derivative is the total derivative operation, which returns zero when vvv is not differentiable at α\alphaα.

QAlgorithms.Papers.Independent.Intakethird100.P67.pureSamples

For arbitrary index and label types I,KI,KI,K and a family of complex vectors ϕk∈CI\phi_k\in\mathbb C^Iϕk​∈CI, this defines the matrix family SkS_kSk​ by Sk(i,j)=ϕk(i)ϕk(j)‾S_k(i,j)=\phi_k(i)\overline{\phi_k(j)}Sk​(i,j)=ϕk​(i)ϕk​(j)​. No normalization or nonzero condition is imposed on the vectors; in particular, a zero vector gives the zero matrix.

QAlgorithms.Papers.Independent.Intakethird100.P67.referenceVector

For any coordinate index type III, vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, and natural number nnn, this defines a vector indexed by functions x:{0,…,n−1}→Ix:\{0,\ldots,n-1\}\to Ix:{0,…,n−1}→I, whose coordinate at xxx is

∏j=0n−1ϕ(xj).\prod_{j=0}^{n-1}\phi(x_j).j=0∏n−1​ϕ(xj​).

No normalization is required of ϕ\phiϕ. The case n=0n=0n=0 is included: there is one empty indexing function, and its coordinate is the empty product 111.

QAlgorithms.Papers.Independent.Intakethird100.P67.registerSwap

For an index type III with decidable equality, this defines the complex matrix on I×II\times II×I whose entry at row (i,j)(i,j)(i,j) and column (k,ℓ)(k,\ell)(k,ℓ) is one exactly when i=ℓi=\elli=ℓ and j=kj=kj=k, and zero otherwise. Thus it sends the coordinate basis vector indexed by (k,ℓ)(k,\ell)(k,ℓ) to that indexed by (ℓ,k)(\ell,k)(ℓ,k). The type III is not required to be nonempty; if it is empty, the matrix is empty.

QAlgorithms.Papers.Independent.Intakethird100.P67.residual

For a finite index type III with decidable equality, an index type KKK, any family ϕ:K→CI\phi:K\to\mathbb C^Iϕ:K→CI, anchor a∈Ka\in Ka∈K, vector ψ∈CI\psi\in\mathbb C^Iψ∈CI, and finite list h=[k0,…,km−1]h=[k_0,\ldots,k_{m-1}]h=[k0​,…,km−1​] of elements of KKK, let (Dk)ij=ϕk(i)ϕk(j)‾(D_k)_{ij}=\phi_k(i)\overline{\phi_k(j)}(Dk​)ij​=ϕk​(i)ϕk​(j)​. Starting with r0=ψr_0=\psir0​=ψ, successively form

rs+1=(Id−2Dks)(Id−Da)rs(0≤s<m).r_{s+1}=(\mathrm{Id}-2D_{k_s})(\mathrm{Id}-D_a)r_s \qquad(0\le s<m).rs+1​=(Id−2Dks​​)(Id−Da​)rs​(0≤s<m).

The definition returns rmr_mrm​, with matrix action given by ordinary matrix-vector multiplication. An empty list returns ψ\psiψ; repeated labels and unnormalized vectors are allowed.

QAlgorithms.Papers.Independent.Intakethird100.P67.sampleAlgebra

For a finite index type III with decidable equality, an arbitrary label type KKK, and a family S=(Sk)k∈KS=(S_k)_{k\in K}S=(Sk​)k∈K​ of complex I×II\times II×I matrices, this defines the complex linear subspace spanned by all products Sk1⋯SkrS_{k_1}\cdots S_{k_r}Sk1​​⋯Skr​​ with r≥1r\geq1r≥1. Labels may repeat, and the factors retain their listed order. Thus its elements are finite complex linear combinations of nonempty products; the empty product is excluded from the generating set. If KKK is empty, this subspace is {0}\{0\}{0}.

QAlgorithms.Papers.Independent.Intakethird100.P67.sampleDimension

For a finite index type III with decidable equality, a finite label type KKK, and arbitrary complex I×II\times II×I matrices SkS_kSk​, this defines the natural number dim⁡Crange⁡(ΠS)\dim_{\mathbb C}\operatorname{range}(\Pi_S)dimC​range(ΠS​), viewing ΠS\Pi_SΠS​ as a complex linear map on CI\mathbb C^ICI. Here ΠS=f(∑kSk)\Pi_S=f(\sum_kS_k)ΠS​=f(∑k​Sk​) is obtained by real continuous functional calculus with f(0)=0f(0)=0f(0)=0 and f(x)=1f(x)=1f(x)=1 for nonzero real xxx. For a Hermitian sum, this counts its nonzero eigenvalues with multiplicity; for a non-Hermitian sum, it is zero. It is also zero when KKK or III is empty.

QAlgorithms.Papers.Independent.Intakethird100.P67.samplePi

For a finite index type III with decidable equality, a finite label type KKK, and arbitrary complex I×II\times II×I matrices SkS_kSk​, put A=∑k∈KSkA=\sum_{k\in K}S_kA=∑k∈K​Sk​. This defines ΠS=f(A)\Pi_S=f(A)ΠS​=f(A) using real continuous functional calculus, where f(0)=0f(0)=0f(0)=0 and f(x)=1f(x)=1f(x)=1 for every nonzero real xxx. When AAA is Hermitian, ΠS\Pi_SΠS​ is the orthogonal projection onto the sum of its nonzero eigenspaces, including eigenspaces with negative eigenvalues. When AAA is not Hermitian, the totalized real functional calculus returns the zero matrix. No positivity assumption is imposed on the samples or their sum; an empty label type gives ΠS=0\Pi_S=0ΠS​=0.

QAlgorithms.Papers.Independent.Intakethird100.P67.sampleReflection

For an index type III with decidable equality and an arbitrary complex vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, this defines the matrix Rϕ=II−2ϕϕ†R_\phi=I_I-2\phi\phi^\daggerRϕ​=II​−2ϕϕ†, whose (i,j)(i,j)(i,j)-entry is δij−2ϕ(i)ϕ(j)‾\delta_{ij}-2\phi(i)\overline{\phi(j)}δij​−2ϕ(i)ϕ(j)​. No normalization is assumed. In particular, ϕ=0\phi=0ϕ=0 gives the identity matrix.

QAlgorithms.Papers.Independent.Intakethird100.P67.slowFactor

For every natural number ddd, every real ε\varepsilonε, and every natural number rrr, this defines

slowFactor⁡(d,ε,r)=(1+log⁡(d+1)+log⁡(1+ε−1))r,\operatorname{slowFactor}(d,\varepsilon,r) =\left(1+\log(d+1)+\log(1+\varepsilon^{-1})\right)^r,slowFactor(d,ε,r)=(1+log(d+1)+log(1+ε−1))r,

where the additions involving ddd are real arithmetic. No positivity or nonzero assumption is imposed on ε\varepsilonε; the inverse is total with 0−1=00^{-1}=00−1=0, and the real logarithm is total with log⁡0=0\log0=0log0=0 and log⁡(−x)=log⁡x\log(-x)=\log xlog(−x)=logx. In particular, ε=0\varepsilon=0ε=0 gives (1+log⁡(d+1))r(1+\log(d+1))^r(1+log(d+1))r, and r=0r=0r=0 gives 111, including when the base is zero.

QAlgorithms.Papers.Independent.Intakethird100.P67.swapHamiltonian

For a coordinate index type III, any natural number nnn, and any real coupling ccc, this defines the complex matrix

Hn,c=c∑j=0n−1SjH_{n,c}=c\sum_{j=0}^{n-1}S_jHn,c​=cj=0∑n−1​Sj​

on indices (i,r)∈I×I{0,…,n−1}(i,r)\in I\times I^{\{0,\ldots,n-1\}}(i,r)∈I×I{0,…,n−1}, where SjS_jSj​ has entry 111 from column (i′,r′)(i',r')(i′,r′) to row (i,r)(i,r)(i,r) exactly when i=rj′i=r'_ji=rj′​ and rrr equals r′r'r′ with coordinate jjj replaced by i′i'i′, and has entry 000 otherwise. The coupling may be negative or zero. For n=0n=0n=0, the sum is empty and H0,c=0H_{0,c}=0H0,c​=0.

QAlgorithms.Papers.Independent.Intakethird100.P67.swapJoint

For a finite coordinate index type III, any vector ϕ∈CI\phi\in\mathbb C^Iϕ∈CI, natural number nnn, real numbers c,tc,tc,t, and arbitrary complex matrix ρ\rhoρ indexed by III, this defines

V(ρ⊗rr†)V†,V=exp⁡(−itH),H=c∑j=0n−1Sj,r(x)=∏j=0n−1ϕ(xj),V\bigl(\rho\otimes rr^\dagger\bigr)V^\dagger, \qquad V=\exp(-itH),\qquad H=c\sum_{j=0}^{n-1}S_j,\qquad r(x)=\prod_{j=0}^{n-1}\phi(x_j),V(ρ⊗rr†)V†,V=exp(−itH),H=cj=0∑n−1​Sj​,r(x)=j=0∏n−1​ϕ(xj​),

where SjS_jSj​ exchanges the distinguished III-coordinate with reference coordinate jjj, and rr†rr^\daggerrr† has entries r(x)r(y)‾r(x)\overline{r(y)}r(x)r(y)​. No normalization of ϕ\phiϕ, positivity or trace condition on ρ\rhoρ, or sign restriction on c,tc,tc,t is imposed. The case n=0n=0n=0 uses the one-dimensional empty reference register, r=1r=1r=1, and H=0H=0H=0, so the resulting matrix has entries ρij\rho_{ij}ρij​ under the natural identification with the distinguished register.

QAlgorithms.Papers.Independent.Intakethird100.P67.swapReference

For a coordinate index type III, a natural number nnn, and an index j∈{0,…,n−1}j\in\{0,\ldots,n-1\}j∈{0,…,n−1}, this defines a complex matrix indexed by pairs (i,r)(i,r)(i,r), where i∈Ii\in Ii∈I and r:{0,…,n−1}→Ir:\{0,\ldots,n-1\}\to Ir:{0,…,n−1}→I. Its entry in row (i,r)(i,r)(i,r) and column (i′,r′)(i',r')(i′,r′) is 111 exactly when i=rj′i=r'_ji=rj′​ and rrr is obtained from r′r'r′ by replacing its jjj-th coordinate with i′i'i′; otherwise the entry is 000. Thus its action exchanges the distinguished coordinate with reference coordinate jjj. When n=0n=0n=0, there is no admissible choice of jjj.

QAlgorithms.Papers.Independent.Intakethird100.P67.systemControlled

For an index type III with decidable equality and an arbitrary complex I×II\times II×I matrix VVV, this defines a matrix C(V)C(V)C(V) indexed by I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true}. Its entry from (j,c)(j,c)(j,c) to (i,b)(i,b)(i,b) is zero when b≠cb\neq cb=c, is VijV_{ij}Vij​ when b=c=trueb=c=\mathrm{true}b=c=true, and is δij\delta_{ij}δij​ when b=c=falseb=c=\mathrm{false}b=c=false. Thus the Boolean coordinate controls whether VVV or the identity acts on the III-coordinate. No unitarity assumption is imposed on VVV.

QAlgorithms.Papers.Independent.Intakethird100.P67.transportedGate

For a finite system index type III, a label type LLL, an arbitrary complex matrix UUU on III, and an arbitrary family of complex matrices WℓW_\ellWℓ​ on I×{false,true}I\times\{\mathrm{false},\mathrm{true}\}I×{false,true}, this defines the family

ℓ⟼(U⊗12) Wℓ (U⊗12)†,\ell\longmapsto (U\otimes\mathbf1_2)\,W_\ell\,(U\otimes\mathbf1_2)^\dagger,ℓ⟼(U⊗12​)Wℓ​(U⊗12​)†,

where 12\mathbf1_212​ is the identity matrix on the Boolean index and †\dagger† denotes conjugate transpose. Neither UUU nor the matrices WℓW_\ellWℓ​ are assumed unitary.

QAlgorithms.Papers.Independent.Intakethird100.P67.unaryWord

For all natural numbers T,tT,tT,t, the definition returns the Boolean word uT,tu_{T,t}uT,t​ of length TTT whose bit at position j∈{0,…,T−1}j\in\{0,\ldots,T-1\}j∈{0,…,T−1} is true exactly when j<tj<tj<t. Thus its first min⁡(t,T)\min(t,T)min(t,T) bits are true and its remaining bits are false. In particular, t=0t=0t=0 gives the all-false word, t≥Tt\ge Tt≥T gives the all-true word, and T=0T=0T=0 gives the unique empty word.

QAlgorithms.Papers.Independent.Intakethird100.P67.uniformAddress

For every natural number ddd, this defines the vector in C{0,…,d−1}\mathbb C^{\{0,\ldots,d-1\}}C{0,…,d−1} whose every coordinate equals (d)−1(\sqrt d)^{-1}(d​)−1. When d=0d=0d=0, the coordinate set is empty and the result is the unique vector in the zero-dimensional space; the real inverse of zero is defined to be zero.

QAlgorithms.Papers.Independent.Intakethird100.P67.wireBranch

For finite index types I,KI,KI,K, any family (ϕk)k∈K(\phi_k)_{k\in K}(ϕk​)k∈K​ of vectors in CI\mathbb C^ICI, anchor a∈Ka\in Ka∈K, arbitrary complex matrices U,ρU,\rhoU,ρ indexed by III, natural number TTT, and Boolean bbb, this defines the following matrix. Write Pk=ϕkϕk†P_k=\phi_k\phi_k^\daggerPk​=ϕk​ϕk†​, Rk=1−2PkR_k=1-2P_kRk​=1−2Pk​, pa(k)=0p_a(k)=0pa​(k)=0 if k=ak=ak=a and pa(k)=(∣K∣−1)−1p_a(k)=(|K|-1)^{-1}pa​(k)=(∣K∣−1)−1 otherwise, where the subtraction is natural-number subtraction and the real inverse of zero is zero. For any system matrix MMM, let C(M)C(M)C(M) preserve a Boolean register and apply 111 when that register is false and MMM when it is true; let H=2−1/2(111−1)H=2^{-1/2}\begin{pmatrix}1&1\\1&-1\end{pmatrix}H=2−1/2(11​1−1​) in the order false, true, and put Ek=C(Rk)(1⊗H)C(Ra)E_k=C(R_k)(1\otimes H)C(R_a)Ek​=C(Rk​)(1⊗H)C(Ra​). For a history h:{0,…,T−1}→Kh:\{0,\ldots,T-1\}\to Kh:{0,…,T−1}→K, let VhV_hVh​ apply EhjE_{h_j}Ehj​​ to the system and Boolean register jjj, in increasing order of jjj, and let V~h\widetilde V_hVh​ be the corresponding product with each EkE_kEk​ replaced by (U⊗1)Ek(U†⊗1)(U\otimes1)E_k(U^\dagger\otimes1)(U⊗1)Ek​(U†⊗1). Set

wh=∏j=0T−1pa(hj),mT(z)=∏j=0T−1(−1)zj2,Xh=Vh(ρ⊗mTmT†)Vh†.w_h=\prod_{j=0}^{T-1}p_a(h_j),\qquad m_T(z)=\prod_{j=0}^{T-1}\frac{(-1)^{z_j}}{\sqrt2},\qquad X_h=V_h(\rho\otimes m_Tm_T^\dagger)V_h^\dagger.wh​=j=0∏T−1​pa​(hj​),mT​(z)=j=0∏T−1​2​(−1)zj​​,Xh​=Vh​(ρ⊗mT​mT†​)Vh†​.

If bbb is true, the result is

∑hwh Tr⁡anc ⁣[((1−Pa)⊗1)Xh((1−Pa)⊗1)†].\sum_h w_h\,\operatorname{Tr}_{\mathrm{anc}} \!\left[((1-P_a)\otimes1)X_h((1-P_a)\otimes1)^\dagger\right].h∑​wh​Tranc​[((1−Pa​)⊗1)Xh​((1−Pa​)⊗1)†].

If bbb is false, the result is

∑hwh Tr⁡anc ⁣[V~h†((Uϕa)(Uϕa)†⊗Tr⁡I ⁣[(Pa⊗1)Xh(Pa⊗1)†])V~h].\sum_h w_h\,\operatorname{Tr}_{\mathrm{anc}} \!\left[ \widetilde V_h^\dagger \left((U\phi_a)(U\phi_a)^\dagger\otimes \operatorname{Tr}_{I}\!\left[(P_a\otimes1)X_h(P_a\otimes1)^\dagger\right]\right) \widetilde V_h \right].h∑​wh​Tranc​[Vh†​((Uϕa​)(Uϕa​)†⊗TrI​[(Pa​⊗1)Xh​(Pa​⊗1)†])Vh​].

Here each partial trace sums matching row and column indices of the indicated register. No normalization, positivity, or unitarity hypotheses are imposed on the inputs. For T=0T=0T=0, there is one empty history, its weight is 111, and both history products are identities; if KKK is a singleton and T>0T>0T>0, all history weights are zero.

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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