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Definitions for Classical Shadows for Quantum Process Tomography on Near-term Quantum Computers

Definition
QAlgorithms_Papers_Independent_Intakethird100_P66

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

prove2quantum

The objects the formalized statements of Classical Shadows for Quantum Process Tomography on Near-term Quantum Computers (arXiv:2110.02965) are stated in. Each was checked against the paper by a blind read-back and a moderator.

  • appendMatrixTensor: Reference-first tensor product on the frozen bit-string register; p.2 Eq.(1).
  • processChoi: Unnormalized Choi matrix, p.2 Eq.(1), constructed by matrix units.
  • processChoiState: Trace-one Choi matrix rho_Lambda=Lambda/2^n, p.2; append-register adapter.
  • processMarginal: Retain both copies of the same physical subsystem, pp.2,14. Summation strings are zero on retained coordinates, counting each outside configuration once. The induced environment is maximally mixed.
  • embedProcessObservable: Extend a subsystem observable by identity on both complements, p.14 A7,A9.
  • BasisChoiceFrame: Finite basis-choice frame, pp.2,4,15. Only PaperFrame constructors supply frames in the named-ensemble claims; arbitrary projectors are not allowed.
  • pauliFrame: Pauli-6, p.2, with redundant outcome relabeling bits for preparation. Averaging gives exactly (1/3)|v><v| on each wire. Fixed outcome zero then prepares all six eigenstates as in the two-sided circuit, p.4.
  • globalFrame: Uniform global Clifford basis on all measured wires, pp.2,4. Finiteness enumerates the entire phase quotient, never a design subset.
  • tensorFrame: Independent fixed blocks, pp.4,15; no gate crosses the block boundary.
  • singleCliffordFrame: Product one-qubit Clifford measurement on m wires, pp.2,13.
  • CliffordBlocks: Fixed partitions into Clifford blocks, pp.4,15. No Pauli/Clifford hybrid ensemble is introduced. The empty frame is the zero-block product.
  • PaperFrame: Exactly Pauli-6 or a fixed Clifford-block partition, Appendix B. Reference and output use independent choices from the same named frame.
  • basisBornWeight: One shot: uniform basis choice followed by its Born outcome, pp.2,4.
  • recordProbability: N independent actual shots, without renormalizing arbitrary weights. For named frames on density matrices these are Born probabilities.
  • basisMeasurementChannel: Constructed complex-linear measurement channel, pp.4,15: the finite coefficient version of the accepted measurement channel.
  • frameInverse: Actual linear inverse, pp.4,15. Zero only totalizes incomplete frames; named PaperFrames are informationally complete. The inverse is linear (d+1)X-Tr(X)I, not the affine formula restricted to rank-one projectors.
  • frameSnapshot: Normalized single-shot reconstruction, pp.4,15.
  • choiSnapshot: Eq.(7): external scale is 2^n for n physical channel qubits.
  • meanChoiSnapshot: Expectation of Eq.(7), permitting indefinite reconstructed matrices.
  • ancillaReconstruction: Appendix B1 expectation, reference first; independent basis choices.
  • twoSidedReconstruction: Appendix B2 expectation: prepare Ui†|0><0|Ui and transpose its reconstructed input factor. Every choice is followed by a fresh channel use.
  • ErrorNorm: Source norms, pp.2,14; trace norm has no factor 1/2.
  • matrixError: The two ordinary matrix norms in II.1/A.3.
  • ReducedRecovers: Uniform recovery of every k-subsystem in one simultaneous event. The estimator precedes the unknown CPTP map and sees exactly N shots.
  • sampleCount: Exact k=0 scalar uses no samples; other real sufficient counts are rounded upward.
  • reducedLog: Common Frobenius logarithm, pp.2,14.
  • traceSampleLog: Trace-norm logarithm: the exponent is 2k, pp.2,14.
  • finiteMax: Finite real maximum, zero only for an empty index type. The theorem families are nonempty (M>0 or k<=n), with nonnegative entries.
  • centeredVariance: Accepted centered shadow variance, extended to raw matrices without a proof binder. The non-Hermitian fallback is never used by a theorem observable. Centering divides by the full measured dimension, not by two.
  • primitiveShotLaw: Frozen oneShotLaw without its unused density-proof parameter: this avoids assuming Choi normalization as a new theorem hypothesis. For CPTP E it is exactly the accepted law on processChoiState E, pp.2,13.
  • primitiveRecordLaw: Independent fresh preparations, counted by actual record length N.
  • PrimitiveReducedRecovers: Generic-primitive simultaneous reduced-process recovery, p.14. The estimator is measurable, as required for the statistical success event.
  • reducedVariance: Full family of ambient embedded 2k-wire Paulis, p.14 A5,A7-A9. Identity coefficients are known exactly.
  • pauliNormEnvelope: Retain the printed Pauli spectral-norm factor, p.14.
  • overlapObservable: Proof-defined observable with transposed input, p.13 A4, fixing the p.2 shorthand.
  • OverlapsRecover: One simultaneous event for all normalized overlaps, II.2. The physical process overlap is 2^n times this target.
  • PrimitiveOverlapsRecover: Same simultaneous task for an arbitrary informationally complete fixed primitive. Measurability rules out interpreting nonmeasurable success sets by outer measure.
Definition code
import Definitions.Def_QAlgorithms_Defs_ClassicalShadowPrediction
import Definitions.Def_QAlgorithms_Defs_LocalPauliShadows
import Definitions.Def_QAlgorithms_Defs_ProjectiveCliffords
import Definitions.Def_QAlgorithms_Defs_MatrixDistances
import Definitions.Def_QAlgorithms_Defs_QECC

/-!
Statements from Levy, Luo and Clark, arXiv:2110.02965v3.
Only the five nodes marked `state` have theorem declarations. Six deferred nodes
are inventoried in HARD.md. All new definitions are paper-local. Each sample
uses a fresh normalized Choi preparation. Compilation is pending batch handoff.
-/

noncomputable section

open MeasureTheory QAlgorithms ClassicalShadows
open scoped Matrix ComplexConjugate ENNReal

namespace QAlgorithms.Papers.Independent.Intakethird100.P66

attribute [local instance] Classical.propDecidable Classical.typeDecidableEq

/-- Reference-first tensor product on the frozen bit-string register; p.2 Eq.(1). -/
def appendMatrixTensor {a b : ℕ} (A : Space a) (B : Space b) : Space (a + b) :=
  (Matrix.kronecker A B).submatrix (qubitsAppendEquiv a b) (qubitsAppendEquiv a b)

/-- Unnormalized Choi matrix, p.2 Eq.(1), constructed by matrix units. -/
def processChoi {n : ℕ} (E : Superop (Qubits n) (Qubits n)) : Space (n + n) :=
  Matrix.of fun x y =>
    E (Matrix.single (qubitsAppendEquiv n n x).1
      (qubitsAppendEquiv n n y).1 1)
      (qubitsAppendEquiv n n x).2 (qubitsAppendEquiv n n y).2

/-- Trace-one Choi matrix rho_Lambda=Lambda/2^n, p.2; append-register adapter. -/
def processChoiState {n : ℕ} (E : Superop (Qubits n) (Qubits n)) : Space (n + n) :=
  ((2 : ℂ) ^ n)⁻¹ • processChoi E

/-- Retain both copies of the same physical subsystem, pp.2,14.
Summation strings are zero on retained coordinates, counting each outside
configuration once. The induced environment is maximally mixed. -/
def processMarginal {n k : ℕ} (rho : Space (n + n)) (w : Fin k ↪ Fin n) : Space (k + k) :=
  Matrix.of fun x y => ∑ a : Qubits n, ∑ b : Qubits n,
    if (∀ i, a (w i) = false) ∧ (∀ i, b (w i) = false) then
      rho (Fin.append (overwrite w a (qubitsAppendEquiv k k x).1)
        (overwrite w b (qubitsAppendEquiv k k x).2))
        (Fin.append (overwrite w a (qubitsAppendEquiv k k y).1)
        (overwrite w b (qubitsAppendEquiv k k y).2))
    else 0

/-- Extend a subsystem observable by identity on both complements, p.14 A7,A9. -/
def embedProcessObservable {n k : ℕ} (w : Fin k ↪ Fin n) (O : Space (k + k)) : Space (n + n) :=
  Matrix.of fun x y =>
    let a := qubitsAppendEquiv n n x
    let b := qubitsAppendEquiv n n y
    if ∀ j, (¬ ∃ i, w i = j) → a.1 j = b.1 j ∧ a.2 j = b.2 j then
      O (Fin.append (a.1 ∘ w) (a.2 ∘ w)) (Fin.append (b.1 ∘ w) (b.2 ∘ w))
    else 0

/-- Finite basis-choice frame, pp.2,4,15. Only `PaperFrame` constructors
supply frames in the named-ensemble claims; arbitrary projectors are not allowed. -/
structure BasisChoiceFrame (n : ℕ) where
  Basis : Type
  finite : Fintype Basis
  inhabited : Nonempty Basis
  projector : Basis → Qubits n → Space n

attribute [instance] BasisChoiceFrame.finite BasisChoiceFrame.inhabited

/-- Pauli-6, p.2, with redundant outcome relabeling bits for preparation.
Averaging gives exactly (1/3)|v><v| on each wire. Fixed outcome zero then
prepares all six eigenstates as in the two-sided circuit, p.4. -/
def pauliFrame (m : ℕ) : BasisChoiceFrame m where
  Basis := GroundStateLearning.ShadowLabel m
  finite := inferInstance
  inhabited := ⟨fun _ => (.Z, true)⟩
  projector a b := ((3 : ℂ) ^ m) • GroundStateLearning.pauliPOVM
    (fun j => ((a j).1, if b j then !(a j).2 else (a j).2))

/-- Uniform global Clifford basis on all measured wires, pp.2,4.
Finiteness enumerates the entire phase quotient, never a design subset. -/
def globalFrame (m : ℕ) [Fintype (Clifford.ProjectiveGroup m)] : BasisChoiceFrame m where
  Basis := Clifford.ProjectiveGroup m
  finite := inferInstance
  inhabited := inferInstance
  projector a b :=
    let U : Space m := (Clifford.representative a).val
    Matrix.of fun x y => conj (U b x) * U b y

/-- Independent fixed blocks, pp.4,15; no gate crosses the block boundary. -/
def tensorFrame {a b : ℕ} (F : BasisChoiceFrame a) (G : BasisChoiceFrame b) : BasisChoiceFrame (a + b) where
  Basis := F.Basis × G.Basis
  finite := inferInstance
  inhabited := inferInstance
  projector u x := appendMatrixTensor (F.projector u.1 (qubitsAppendEquiv a b x).1)
    (G.projector u.2 (qubitsAppendEquiv a b x).2)

/-- Product one-qubit Clifford measurement on m wires, pp.2,13. -/
def singleCliffordFrame [Fintype (Clifford.ProjectiveGroup 1)] : (m : ℕ) → BasisChoiceFrame m
  | 0 => pauliFrame 0
  | m + 1 => tensorFrame (singleCliffordFrame m) (globalFrame 1)

/-- Fixed partitions into Clifford blocks, pp.4,15. No Pauli/Clifford
hybrid ensemble is introduced. The empty frame is the zero-block product. -/
inductive CliffordBlocks : {m : ℕ} → BasisChoiceFrame m → Prop
  | empty : CliffordBlocks (pauliFrame 0)
  | global (m : ℕ) [Fintype (Clifford.ProjectiveGroup m)] :
      CliffordBlocks (globalFrame m)
  | blocks {a b : ℕ} {F : BasisChoiceFrame a} {G : BasisChoiceFrame b} :
      CliffordBlocks F → CliffordBlocks G → CliffordBlocks (tensorFrame F G)

/-- Exactly Pauli-6 or a fixed Clifford-block partition, Appendix B.
Reference and output use independent choices from the same named frame. -/
inductive PaperFrame : {m : ℕ} → BasisChoiceFrame m → Prop
  | pauli (m : ℕ) : PaperFrame (pauliFrame m)
  | clifford {m : ℕ} {F : BasisChoiceFrame m} : CliffordBlocks F → PaperFrame F

/-- One shot: uniform basis choice followed by its Born outcome, pp.2,4. -/
def basisBornWeight {m : ℕ} (F : BasisChoiceFrame m) (rho : Space m) (s : F.Basis × Qubits m) : ℝ :=
  (Fintype.card F.Basis : ℝ)⁻¹ * effectProb (F.projector s.1 s.2) rho

/-- N independent actual shots, without renormalizing arbitrary weights.
For named frames on density matrices these are Born probabilities. -/
def recordProbability {m N : ℕ} (F : BasisChoiceFrame m) (rho : Space m)
    (event : (Fin N → F.Basis × Qubits m) → Prop) : ℝ :=
  ∑ r : Fin N → F.Basis × Qubits m,
    if event r then ∏ j, basisBornWeight F rho (r j) else 0

/-- Constructed complex-linear measurement channel, pp.4,15:
the finite coefficient version of the accepted measurement channel. -/
def basisMeasurementChannel {m : ℕ} (F : BasisChoiceFrame m) : Space m →ₗ[ℂ] Space m where
  toFun X := Matrix.of fun i j => ∑ k, ∑ l,
    ((Fintype.card F.Basis : ℂ)⁻¹ *
      ∑ a : F.Basis, ∑ b : Qubits m,
        F.projector a b l k * F.projector a b i j) * X k l
  map_add' X Y := by ext i j; simp [mul_add, Finset.sum_add_distrib]
  map_smul' c X := by ext i j; simp [Finset.mul_sum, mul_left_comm]

/-- Actual linear inverse, pp.4,15. Zero only totalizes incomplete frames;
named PaperFrames are informationally complete. The inverse is linear
(d+1)X-Tr(X)I, not the affine formula restricted to rank-one projectors. -/
def frameInverse {m : ℕ} (F : BasisChoiceFrame m) : Space m →ₗ[ℂ] Space m :=
  if h : Function.Injective (basisMeasurementChannel F) then
    (LinearEquiv.ofBijective (basisMeasurementChannel F)
      ⟨h, LinearMap.injective_iff_surjective.mp h⟩).symm.toLinearMap
  else 0

/-- Normalized single-shot reconstruction, pp.4,15. -/
def frameSnapshot {m : ℕ} (F : BasisChoiceFrame m) (s : F.Basis × Qubits m) : Space m :=
  frameInverse F (F.projector s.1 s.2)

/-- Eq.(7): external scale is 2^n for n physical channel qubits. -/
def choiSnapshot {n : ℕ} (F : BasisChoiceFrame (n + n))
    (s : F.Basis × Qubits (n + n)) : Space (n + n) :=
  ((2 : ℂ) ^ n) • frameSnapshot F s

/-- Expectation of Eq.(7), permitting indefinite reconstructed matrices. -/
def meanChoiSnapshot {n : ℕ} (F : BasisChoiceFrame (n + n))
    (E : Superop (Qubits n) (Qubits n)) : Space (n + n) :=
  ∑ s : F.Basis × Qubits (n + n),
    (basisBornWeight F (processChoiState E) s : ℂ) • choiSnapshot F s

/-- Appendix B1 expectation, reference first; independent basis choices. -/
def ancillaReconstruction {n : ℕ} (F : BasisChoiceFrame n)
    (E : Superop (Qubits n) (Qubits n)) : Space (n + n) :=
  ((Fintype.card F.Basis : ℂ) ^ 2)⁻¹ •
    ∑ a : F.Basis, ∑ c : F.Basis, ∑ b : Qubits n, ∑ d : Qubits n,
      (effectProb (appendMatrixTensor (F.projector a b) (F.projector c d))
        (processChoiState E) : ℂ) •
        appendMatrixTensor (frameInverse F (F.projector a b)) (frameInverse F (F.projector c d))

/-- Appendix B2 expectation: prepare Ui†|0><0|Ui and transpose its
reconstructed input factor. Every choice is followed by a fresh channel use. -/
def twoSidedReconstruction {n : ℕ} (F : BasisChoiceFrame n)
    (E : Superop (Qubits n) (Qubits n)) : Space (n + n) :=
  ((Fintype.card F.Basis : ℂ) ^ 2)⁻¹ •
    ∑ a : F.Basis, ∑ c : F.Basis, ∑ d : Qubits n,
      (effectProb (F.projector c d) (E (F.projector a (fun _ => false))) : ℂ) •
        appendMatrixTensor (frameInverse F ((F.projector a (fun _ => false)).transpose))
          (frameInverse F (F.projector c d))

/-- Source norms, pp.2,14; trace norm has no factor 1/2. -/
inductive ErrorNorm where
  | frobenius | trace

/-- The two ordinary matrix norms in II.1/A.3. -/
def matrixError {m : ℕ} : ErrorNorm → Space m → ℝ
  | .frobenius, X => frobNorm X
  | .trace, X => traceNorm X

/-- Uniform recovery of every k-subsystem in one simultaneous event.
The estimator precedes the unknown CPTP map and sees exactly N shots. -/
def ReducedRecovers {n : ℕ} (F : BasisChoiceFrame (n + n)) (k N : ℕ)
    (norm : ErrorNorm) (eps delta : ℝ) : Prop :=
  ∃ estimate : (Fin N → F.Basis × Qubits (n + n)) → (Fin k ↪ Fin n) → Space (k + k),
    ∀ E : Superop (Qubits n) (Qubits n), IsChannel E →
      1 - delta ≤ recordProbability F (processChoiState E)
        (fun r => ∀ w, matrixError norm (estimate r w - processMarginal (processChoiState E) w) ≤ eps)

/-- Exact k=0 scalar uses no samples; other real sufficient counts are rounded upward. -/
def sampleCount (k : ℕ) (B : ℝ) : ℕ := if k = 0 then 0 else ⌈B⌉₊

/-- Common Frobenius logarithm, pp.2,14. -/
def reducedLog (n k : ℕ) (delta : ℝ) : ℝ :=
  Real.log (2 * (8 * (n : ℝ)) ^ (2 * k) / delta)

/-- Trace-norm logarithm: the exponent is 2k, pp.2,14. -/
def traceSampleLog (n k : ℕ) (delta : ℝ) : ℝ :=
  Real.log ((24 * (n : ℝ)) ^ (2 * k) / delta)

/-- Finite real maximum, zero only for an empty index type.
The theorem families are nonempty (M>0 or k<=n), with nonnegative entries. -/
def finiteMax {A : Type*} [Fintype A] (f : A → ℝ) : ℝ :=
  if h : (Finset.univ : Finset A).Nonempty then Finset.univ.sup' h f else 0

/-- Accepted centered shadow variance, extended to raw matrices without a
proof binder. The non-Hermitian fallback is never used by a theorem observable.
Centering divides by the full measured dimension, not by two. -/
def centeredVariance {m : ℕ} (P : MeasurementPrimitive m) (O : Space m) : ℝ :=
  if h : O.IsHermitian then
    shadowNorm P (tracelessPart O) (tracelessPart_hermitian O h) ^ 2
  else 0

/-- Frozen oneShotLaw without its unused density-proof parameter: this avoids
assuming Choi normalization as a new theorem hypothesis. For CPTP E it is
exactly the accepted law on processChoiState E, pp.2,13. -/
def primitiveShotLaw {m : ℕ} (P : MeasurementPrimitive m) (rho : Space m) :
    Measure (Matrix.unitaryGroup (Qubits m) ℂ × Qubits m) :=
  ∑ b : Qubits m,
    (P.ensemble.withDensity (fun U => ENNReal.ofReal
      (((U : Space m) * rho * star (U : Space m)) b b).re)).map (fun U => (U, b))

/-- Independent fresh preparations, counted by actual record length N. -/
def primitiveRecordLaw {m : ℕ} (P : MeasurementPrimitive m) (rho : Space m) (N : ℕ) :=
  Measure.pi fun _ : Fin N => primitiveShotLaw P rho

/-- Generic-primitive simultaneous reduced-process recovery, p.14.
The estimator is measurable, as required for the statistical success event. -/
def PrimitiveReducedRecovers {n : ℕ} (P : MeasurementPrimitive (n + n))
    (k N : ℕ) (eps delta : ℝ) : Prop :=
  ∃ estimate : (Fin N → Matrix.unitaryGroup (Qubits (n + n)) ℂ × Qubits (n + n)) →
      (Fin k ↪ Fin n) → Space (k + k),
    Measurable estimate ∧
    ∀ E : Superop (Qubits n) (Qubits n), IsChannel E →
      ENNReal.ofReal (1 - delta) ≤ primitiveRecordLaw P (processChoiState E) N
        {r | ∀ w, frobNorm (estimate r w - processMarginal (processChoiState E) w) ≤ eps}

/-- Full family of ambient embedded 2k-wire Paulis, p.14 A5,A7-A9.
Identity coefficients are known exactly. -/
def reducedVariance {n : ℕ} (P : MeasurementPrimitive (n + n)) (k : ℕ) : ℝ :=
  finiteMax fun p : (Fin k ↪ Fin n) × (Fin (k + k) → Stabilizer.Pauli) =>
    centeredVariance P (embedProcessObservable p.1 (pauliOps p.2))

/-- Retain the printed Pauli spectral-norm factor, p.14. -/
def pauliNormEnvelope (k : ℕ) : ℝ :=
  finiteMax fun p : Fin (k + k) → Stabilizer.Pauli => specNorm (pauliOps p) ^ 2

/-- Proof-defined observable with transposed input, p.13 A4, fixing the p.2 shorthand. -/
def overlapObservable {n : ℕ} (rho sigma : Space n) : Space (n + n) :=
  appendMatrixTensor rho.transpose sigma

/-- One simultaneous event for all normalized overlaps, II.2.
The physical process overlap is 2^n times this target. -/
def OverlapsRecover {n M : ℕ} (F : BasisChoiceFrame (n + n)) (O : Fin M → Space (n + n))
    (N : ℕ) (eps delta : ℝ) : Prop :=
  ∃ estimate : (Fin N → F.Basis × Qubits (n + n)) → Fin M → ℝ,
    ∀ E : Superop (Qubits n) (Qubits n), IsChannel E →
      1 - delta ≤ recordProbability F (processChoiState E)
        (fun r => ∀ i, |estimate r i - (O i * processChoiState E).trace.re| ≤ eps)

/-- Same simultaneous task for an arbitrary informationally complete fixed primitive.
Measurability rules out interpreting nonmeasurable success sets by outer measure. -/
def PrimitiveOverlapsRecover {n M : ℕ} (P : MeasurementPrimitive (n + n))
    (O : Fin M → Space (n + n)) (N : ℕ) (eps delta : ℝ) : Prop :=
  ∃ estimate : (Fin N → Matrix.unitaryGroup (Qubits (n + n)) ℂ × Qubits (n + n)) →
      Fin M → ℝ,
    Measurable estimate ∧
    ∀ E : Superop (Qubits n) (Qubits n), IsChannel E →
      ENNReal.ofReal (1 - delta) ≤ primitiveRecordLaw P (processChoiState E) N
        {r | ∀ i, |estimate r i - (O i * processChoiState E).trace.re| ≤ eps}

/-! Small boundary/structural sanity checks, not proofs of paper results. -/

example (B : ℝ) : sampleCount 0 B = 0 := by simp [sampleCount]

example (m : ℕ) (F : BasisChoiceFrame m) : frameInverse F 0 = 0 := map_zero _

example {m : ℕ} (P : MeasurementPrimitive m) (rho : Space m) (h : IsDensityMatrix rho) :
    primitiveShotLaw P rho = oneShotLaw P rho h := rfl

example {a b : ℕ} (A : Space a) (B : Space b) (x y : Qubits (a + b)) :
    appendMatrixTensor A B x y = A (qubitsAppendEquiv a b x).1 (qubitsAppendEquiv a b y).1 *
      B (qubitsAppendEquiv a b x).2 (qubitsAppendEquiv a b y).2 := rfl

example (a : GroundStateLearning.ShadowLabel 0) (b : Qubits 0) :
    (pauliFrame 0).projector a b = 1 := by
  ext x y
  simp [pauliFrame, GroundStateLearning.pauliPOVM, kronAll,
    Matrix.one_apply, Subsingleton.elim x y]

example : finiteMax (fun _ : Fin 0 => (7 : ℝ)) = 0 := by simp [finiteMax]

example {n : ℕ} (F : BasisChoiceFrame (n + n)) (s : F.Basis × Qubits (n + n)) :
    choiSnapshot F s = ((2 : ℂ) ^ n) • frameSnapshot F s := rfl

example {n : ℕ} (rho sigma : Space n) :
    overlapObservable rho sigma = appendMatrixTensor rho.transpose sigma := rfl

/-- Identity-channel normalization sanity check, p.2 Eq.(1). -/
example (n : ℕ) (a b : Qubits n) :
    processChoiState (fun X : Space n => X) (Fin.append a a) (Fin.append b b) =
      ((2 : ℂ) ^ n)⁻¹ := by
  have ha : qubitsAppendEquiv n n (Fin.append a a) = (a, a) :=
    (qubitsAppendEquiv n n).apply_symm_apply (a, a)
  have hb : qubitsAppendEquiv n n (Fin.append b b) = (b, b) :=
    (qubitsAppendEquiv n n).apply_symm_apply (b, b)
  simp [processChoiState, processChoi, ha, hb, Matrix.single_apply]

/-- The zero-shot event is deterministic even when the matrix argument is not a state. -/
example {m : ℕ} (F : BasisChoiceFrame m) (rho : Space m) :
    recordProbability (N := 0) F rho (fun _ => True) = 1 := by
  simp [recordProbability]

/-- Invertibility is constructed, not replaced by an unrelated reconstruction map. -/
example {m : ℕ} (F : BasisChoiceFrame m) (h : Function.Injective (basisMeasurementChannel F)) (X : Space m) :
    frameInverse F (basisMeasurementChannel F X) = X := by
  unfold frameInverse
  rw [dif_pos h]
  exact (LinearEquiv.ofBijective (basisMeasurementChannel F)
    ⟨h, LinearMap.injective_iff_surjective.mp h⟩).symm_apply_apply X

/-- Empty tensor product is a legitimate zero-block Clifford frame. -/
example [Fintype (Clifford.ProjectiveGroup 1)] : PaperFrame (singleCliffordFrame 0) :=
  PaperFrame.clifford CliffordBlocks.empty

end QAlgorithms.Papers.Independent.Intakethird100.P66
Source
Classical Shadows for Quantum Process Tomography on Near-term Quantum Computers, arXiv:2110.02965v3, https://arxiv.org/abs/2110.02965v3
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What the Lean code literally says, in plain math · gpt-6.1-sol

QAlgorithms.Papers.Independent.Intakethird100.P66.BasisChoiceFrame

For each natural number nnn, including zero, this defines a structure consisting of a type BBB, a specified finite enumeration of BBB, evidence that BBB is nonempty, and a function assigning to every a∈Ba\in Ba∈B and every nnn-bit string bbb an arbitrary complex matrix Pa,bP_{a,b}Pa,b​ indexed by nnn-bit strings. No equations or positivity, Hermiticity, idempotence, orthogonality, or normalization conditions are required of these matrices. For n=0n=0n=0, there is one bit string and each assigned matrix has one entry.

QAlgorithms.Papers.Independent.Intakethird100.P66.CliffordBlocks

This defines a proposition about frames on any natural number of bits, where a frame consists of a finite, nonempty choice set and assigned complex matrices for every choice and outcome string. It is generated by exactly three rules: the zero-bit frame with singleton choice set and matrix [1][1][1] satisfies the proposition; for every natural number mmm and specified finite enumeration of its projective group, the global frame satisfies it; and for all natural numbers a,ba,ba,b and frames F,GF,GF,G satisfying it on those respective lengths, their tensor frame satisfies it on a+ba+ba+b bits. In the global rule, the projective group is the normalizer of the unitary subgroup generated by ic⨂jPji^c\bigotimes_jP_jic⨂j​Pj​, with c∈{0,1,2,3}c\in\{0,1,2,3\}c∈{0,1,2,3} and Pj∈{I,X,Y,Z}P_j\in\{I,X,Y,Z\}Pj​∈{I,X,Y,Z}, quotiented by equality of conjugation on every complex matrix; its assigned matrices have entries (Ua)b,x‾(Ua)b,y\overline{(U_a)_{b,x}}(U_a)_{b,y}(Ua​)b,x​​(Ua​)b,y​ for the designated representative UaU_aUa​. In the tensor rule, choices are paired, outcomes and indices are split into consecutive blocks, and corresponding matrix entries are multiplied. Only frames obtainable by finitely many applications of these rules satisfy the proposition; zero-length global and tensor blocks are included.

QAlgorithms.Papers.Independent.Intakethird100.P66.ErrorNorm

This declaration defines a type with exactly two distinct values, named frobenius and trace, and no additional data attached to either value.

QAlgorithms.Papers.Independent.Intakethird100.P66.OverlapsRecover

For natural numbers n,Mn,Mn,M, let Bj={0,1}j\mathcal B_j=\{0,1\}^jBj​={0,1}j, and let FFF consist of a finite nonempty type AAA and arbitrary complex matrices Fa,bF_{a,b}Fa,b​ indexed by B2n\mathcal B_{2n}B2n​ for a∈Aa\in Aa∈A and b∈B2nb\in\mathcal B_{2n}b∈B2n​; no projector, positivity, or normalization conditions are imposed on these matrices. Given matrices O0,…,OM−1O_0,\ldots,O_{M-1}O0​,…,OM−1​ indexed by B2n\mathcal B_{2n}B2n​, a natural number NNN, and real numbers ε,δ\varepsilon,\deltaε,δ, this predicate says that there exists a function o^:(A×B2n)N→RM\widehat o:(A\times\mathcal B_{2n})^N\to\mathbb R^Mo:(A×B2n​)N→RM such that, for every map EEE on matrices indexed by Bn\mathcal B_nBn​ having a finite representation E(X)=∑a=0s−1KaXKa†E(X)=\sum_{a=0}^{s-1}K_aXK_a^\daggerE(X)=∑a=0s−1​Ka​XKa†​ with ∑a=0s−1Ka†Ka=I\sum_{a=0}^{s-1}K_a^\dagger K_a=I∑a=0s−1​Ka†​Ka​=I, the matrix

(CE)(u,v),(u′,v′)=2−nE(∣u⟩⟨u′∣)v,v′(C_E)_{(u,v),(u',v')}=2^{-n}E(|u\rangle\langle u'|)_{v,v'}(CE​)(u,v),(u′,v′)​=2−nE(∣u⟩⟨u′∣)v,v′​

satisfies

1−δ≤∑r∈(A×B2n)N1{∀i<M, ∣o^(r)i−Re⁡Tr⁡(OiCE)∣≤ε}∏j=0N−1(1∣A∣Re⁡Tr⁡(FrjCE)),1-\delta\le \sum_{r\in(A\times\mathcal B_{2n})^N} \mathbf1_{\{\forall i<M,\ |\widehat o(r)_i-\operatorname{Re}\operatorname{Tr}(O_iC_E)|\le\varepsilon\}} \prod_{j=0}^{N-1} \left(\frac{1}{|A|}\operatorname{Re}\operatorname{Tr}(F_{r_j}C_E)\right),1−δ≤r∈(A×B2n​)N∑​1{∀i<M, ∣o(r)i​−ReTr(Oi​CE​)∣≤ε}​j=0∏N−1​(∣A∣1​ReTr(Frj​​CE​)),

where pairs of nnn-bit strings index CEC_ECE​ by concatenation, Frj=Fa,bF_{r_j}=F_{a,b}Frj​​=Fa,b​ when rj=(a,b)r_j=(a,b)rj​=(a,b), and the indicator equals one precisely when its condition holds. The same estimate must work for every such EEE; neither the OiO_iOi​ nor the estimate has additional constraints. The displayed record weights are the specified real expressions and are not assumed nonnegative or normalized. Zero values of n,M,Nn,M,Nn,M,N are included: M=0M=0M=0 makes the accuracy condition vacuous, and N=0N=0N=0 leaves one empty record with product weight one. There are no range assumptions on ε\varepsilonε or δ\deltaδ.

QAlgorithms.Papers.Independent.Intakethird100.P66.PaperFrame

This defines a proposition about frames on any natural number mmm of bits, generated by two rules. First, for every mmm, it holds for the frame whose choices are functions aj=(Aj,tj)∈{X,Y,Z}×{false,true}a_j=(A_j,t_j)\in\{X,Y,Z\}\times\{\mathrm{false},\mathrm{true}\}aj​=(Aj​,tj​)∈{X,Y,Z}×{false,true} and whose matrix for outcome bbb has entries ∏j[(I+sjσAj)/2]xj,yj\prod_j[(I+s_j\sigma_{A_j})/2]_{x_j,y_j}∏j​[(I+sj​σAj​​)/2]xj​,yj​​, with sj=1s_j=1sj​=1 when tj≠bjt_j\ne b_jtj​=bj​ and sj=−1s_j=-1sj​=−1 otherwise, using the usual Pauli matrices. Second, it holds for any frame obtained by finitely combining the singleton zero-bit frame with matrix [1][1][1] and global frames by appended tensor products. Each global block of length rrr requires a specified finite enumeration of the quotient of the normalizer of the unitary subgroup generated by ic⨂jPji^c\bigotimes_jP_jic⨂j​Pj​, for c∈{0,1,2,3}c\in\{0,1,2,3\}c∈{0,1,2,3} and Pj∈{I,X,Y,Z}P_j\in\{I,X,Y,Z\}Pj​∈{I,X,Y,Z}, where two normalizer elements are identified when their conjugation functions agree on every complex matrix; its matrices have entries (Ua)b,x‾(Ua)b,y\overline{(U_a)_{b,x}}(U_a)_{b,y}(Ua​)b,x​​(Ua​)b,y​ for designated representatives. Tensor products pair choice sets and multiply matrix entries after splitting outcomes and indices into consecutive blocks. These are the only generating rules, and they include m=0m=0m=0.

QAlgorithms.Papers.Independent.Intakethird100.P66.PrimitiveOverlapsRecover

For any natural numbers n,M,Nn,M,Nn,M,N, real numbers ε,δ\varepsilon,\deltaε,δ, measurement primitive PPP on 2n2n2n qubits, and family O0,…,OM−1O_0,\ldots,O_{M-1}O0​,…,OM−1​ of arbitrary complex matrices indexed by Q2n={0,1}2nQ_{2n}=\{0,1\}^{2n}Q2n​={0,1}2n, this proposition asserts the existence of a measurable estimator, independent of the channel, that returns MMM real numbers from NNN recorded pairs of a unitary matrix and a bit string. Here Qj={0,1}jQ_j=\{0,1\}^jQj​={0,1}j, including the singleton Q0Q_0Q0​, and PPP consists of a Borel probability measure μ\muμ on unitary matrices indexed by Q2nQ_{2n}Q2n​, together with injectivity of the complex linear map

Mμ(X)ij=∑a,b∈Q2n(∫∑t∈Q2nUti‾UtjUtaUtb‾ dμ(U))Xab.\mathcal M_\mu(X)_{ij} =\sum_{a,b\in Q_{2n}} \left(\int \sum_{t\in Q_{2n}} \overline{U_{ti}}U_{tj}U_{ta}\overline{U_{tb}}\,d\mu(U)\right)X_{ab}.Mμ​(X)ij​=a,b∈Q2n​∑​​∫t∈Q2n​∑​Uti​​Utj​Uta​Utb​​dμ(U)​Xab​.

Specifically, there must exist a measurable function o^\widehat oo assigning a real number o^(r,i)\widehat o(r,i)o(r,i) to every record r=((Uj,bj))j=0N−1r=((U_j,b_j))_{j=0}^{N-1}r=((Uj​,bj​))j=0N−1​ and every i∈{0,…,M−1}i\in\{0,\ldots,M-1\}i∈{0,…,M−1}, such that the following holds for every channel EEE. A channel here means a function on complex matrices indexed by QnQ_nQn​ for which there exist a natural number sss and matrices K0,…,Ks−1K_0,\ldots,K_{s-1}K0​,…,Ks−1​ satisfying ∑hKh†Kh=I\sum_hK_h^\dagger K_h=I∑h​Kh†​Kh​=I and E(X)=∑hKhXKh†E(X)=\sum_hK_hXK_h^\daggerE(X)=∑h​Kh​XKh†​ for every XXX. Identify concatenated nnn-bit strings with pairs and define

(ρE)(a,b),(a′,b′)=2−n(E(∣a⟩⟨a′∣))b,b′,a,b,a′,b′∈Qn,(\rho_E)_{(a,b),(a',b')} =2^{-n}\bigl(E(|a\rangle\langle a'|)\bigr)_{b,b'}, \qquad a,b,a',b'\in Q_n,(ρE​)(a,b),(a′,b′)​=2−n(E(∣a⟩⟨a′∣))b,b′​,a,b,a′,b′∈Qn​,

where ∣a⟩⟨a′∣|a\rangle\langle a'|∣a⟩⟨a′∣ is the matrix with its sole nonzero entry, equal to 111, at (a,a′)(a,a')(a,a′). Define the one-shot measure on pairs (U,b)(U,b)(U,b) by

νE(A)=∑b∈Q2n∫1A(U,b) max⁡ ⁣{Re⁡(UρEU†)bb,0} dμ(U),\nu_E(A)= \sum_{b\in Q_{2n}}\int \mathbf 1_A(U,b)\, \max\!\left\{\operatorname{Re}(U\rho_EU^\dagger)_{bb},0\right\}\,d\mu(U),νE​(A)=b∈Q2n​∑​∫1A​(U,b)max{Re(UρE​U†)bb​,0}dμ(U),

and use its NNN-fold product as the record measure. Then

max⁡{1−δ,0}≤νE⊗N{r: for every 0≤i<M, ∣o^(r,i)−Re⁡tr⁡(OiρE)∣≤ε},\max\{1-\delta,0\} \le \nu_E^{\otimes N} \left\{r:\ \text{for every }0\le i<M,\ \left|\widehat o(r,i)-\operatorname{Re}\operatorname{tr}(O_i\rho_E)\right| \le\varepsilon\right\},max{1−δ,0}≤νE⊗N​{r: for every 0≤i<M, ∣o(r,i)−Retr(Oi​ρE​)∣≤ε},

with the left side viewed as an extended nonnegative real number. The matrices OiO_iOi​ need not be Hermitian, positive, or norm bounded; only the real parts of the displayed traces are estimated. All natural-number values, including n=0n=0n=0, M=0M=0M=0, and N=0N=0N=0, and all real values of ε,δ\varepsilon,\deltaε,δ, are included. When M=0M=0M=0, the simultaneous accuracy condition is vacuous. When N=0N=0N=0, there is a unique empty record with product-measure mass 111, so the estimator has no recorded observations on which to depend.

QAlgorithms.Papers.Independent.Intakethird100.P66.PrimitiveReducedRecovers

For any natural numbers n,k,Nn,k,Nn,k,N, real numbers ε,δ\varepsilon,\deltaε,δ, and measurement primitive PPP on 2n2n2n qubits, this proposition asserts the existence of a measurable estimator, independent of the channel, with the following property. Write Qj={0,1}jQ_j=\{0,1\}^jQj​={0,1}j, including the singleton Q0Q_0Q0​. The primitive PPP consists of a Borel probability measure μ\muμ on the unitary matrices indexed by Q2nQ_{2n}Q2n​, together with injectivity of the complex linear map

Mμ(X)ij=∑a,b∈Q2n(∫∑t∈Q2nUti‾UtjUtaUtb‾ dμ(U))Xab.\mathcal M_\mu(X)_{ij} =\sum_{a,b\in Q_{2n}} \left(\int \sum_{t\in Q_{2n}} \overline{U_{ti}}U_{tj}U_{ta}\overline{U_{tb}}\,d\mu(U)\right)X_{ab}.Mμ​(X)ij​=a,b∈Q2n​∑​​∫t∈Q2n​∑​Uti​​Utj​Uta​Utb​​dμ(U)​Xab​.

The estimator takes a record r=((Uj,bj))j=0N−1r=((U_j,b_j))_{j=0}^{N-1}r=((Uj​,bj​))j=0N−1​ and any injection w:{0,…,k−1}↪{0,…,n−1}w:\{0,\ldots,k-1\}\hookrightarrow\{0,\ldots,n-1\}w:{0,…,k−1}↪{0,…,n−1}, and returns a complex matrix ρ^(r,w)\widehat\rho(r,w)ρ​(r,w) indexed by Q2kQ_{2k}Q2k​. For every function EEE from complex matrices indexed by QnQ_nQn​ to such matrices that is a channel—meaning that there exist a natural number sss and matrices K0,…,Ks−1K_0,\ldots,K_{s-1}K0​,…,Ks−1​ satisfying ∑hKh†Kh=I\sum_h K_h^\dagger K_h=I∑h​Kh†​Kh​=I and E(X)=∑hKhXKh†E(X)=\sum_h K_hXK_h^\daggerE(X)=∑h​Kh​XKh†​ for every XXX—define the matrix ρE\rho_EρE​, using concatenated bit strings as pairs, by

(ρE)(a,b),(a′,b′)=2−n(E(∣a⟩⟨a′∣))b,b′,a,b,a′,b′∈Qn,(\rho_E)_{(a,b),(a',b')} =2^{-n}\bigl(E(|a\rangle\langle a'|)\bigr)_{b,b'}, \qquad a,b,a',b'\in Q_n,(ρE​)(a,b),(a′,b′)​=2−n(E(∣a⟩⟨a′∣))b,b′​,a,b,a′,b′∈Qn​,

where ∣a⟩⟨a′∣|a\rangle\langle a'|∣a⟩⟨a′∣ has entry 111 at (a,a′)(a,a')(a,a′) and 000 elsewhere. Define a one-shot measure νE\nu_EνE​ on pairs (U,b)(U,b)(U,b) by

νE(A)=∑b∈Q2n∫1A(U,b) max⁡ ⁣{Re⁡(UρEU†)bb,0} dμ(U),\nu_E(A)= \sum_{b\in Q_{2n}}\int \mathbf 1_A(U,b)\, \max\!\left\{\operatorname{Re}(U\rho_EU^\dagger)_{bb},0\right\}\,d\mu(U),νE​(A)=b∈Q2n​∑​∫1A​(U,b)max{Re(UρE​U†)bb​,0}dμ(U),

and let the record measure be the NNN-fold product νE⊗N\nu_E^{\otimes N}νE⊗N​. For each injection www, define ρE,w\rho_{E,w}ρE,w​ by the following entries: for a,b,a′,b′∈Qka,b,a',b'\in Q_ka,b,a′,b′∈Qk​,

(ρE,w)(a,b),(a′,b′)=∑u,v∈Qnu(w(i))=v(w(i))=0 for every i(ρE)(u[w←a], v[w←b]),(u[w←a′], v[w←b′]),(\rho_{E,w})_{(a,b),(a',b')} = \sum_{\substack{u,v\in Q_n\\ u(w(i))=v(w(i))=0\ \text{for every }i}} (\rho_E)_{(u[w\leftarrow a],\,v[w\leftarrow b]), (u[w\leftarrow a'],\,v[w\leftarrow b'])},(ρE,w​)(a,b),(a′,b′)​=u,v∈Qn​u(w(i))=v(w(i))=0 for every i​∑​(ρE​)(u[w←a],v[w←b]),(u[w←a′],v[w←b′])​,

where u[w←a]u[w\leftarrow a]u[w←a] replaces u(w(i))u(w(i))u(w(i)) by a(i)a(i)a(i) and leaves all other coordinates unchanged. The required bound is

max⁡{1−δ,0}≤νE⊗N{r: for every injection w, (∑x,y∈Q2k∣(ρ^(r,w)−ρE,w)xy∣2)1/2≤ε}.\max\{1-\delta,0\} \le \nu_E^{\otimes N} \left\{r:\ \text{for every injection }w,\ \left(\sum_{x,y\in Q_{2k}} \left|\bigl(\widehat\rho(r,w)-\rho_{E,w}\bigr)_{xy}\right|^2\right)^{1/2} \le\varepsilon\right\}.max{1−δ,0}≤νE⊗N​⎩⎨⎧​r: for every injection w, ​x,y∈Q2k​∑​​(ρ​(r,w)−ρE,w​)xy​​2​1/2≤ε⎭⎬⎫​.

The left side is regarded as an extended nonnegative real number. No sign or range restrictions on ε,δ\varepsilon,\deltaε,δ, or positivity restrictions on n,k,Nn,k,Nn,k,N, are imposed. If k>nk>nk>n, there are no such injections and the condition inside the event is vacuous; if k=0k=0k=0, the unique empty injection is still included. If N=0N=0N=0, the record is the unique empty record and its product measure has mass 111.

QAlgorithms.Papers.Independent.Intakethird100.P66.ReducedRecovers

For every natural number nnn, let Qn={0,1}nQ_n=\{0,1\}^nQn​={0,1}n and let FFF supply a finite nonempty type B\mathcal BB and arbitrary complex matrices Pa,bP_{a,b}Pa,b​ on Q2nQ_{2n}Q2n​. For every pair of natural numbers k,Nk,Nk,N, either choice ν\nuν of Frobenius or trace norm, and arbitrary real numbers ε,δ\varepsilon,\deltaε,δ, this predicate asserts that there exists one estimator J^\widehat JJ assigning a complex matrix on Q2kQ_{2k}Q2k​ to each record r:{0,…,N−1}→B×Q2nr:\{0,\ldots,N-1\}\to\mathcal B\times Q_{2n}r:{0,…,N−1}→B×Q2n​ and each injection w:{0,…,k−1}↪{0,…,n−1}w:\{0,\ldots,k-1\}\hookrightarrow\{0,\ldots,n-1\}w:{0,…,k−1}↪{0,…,n−1}, such that the following inequality holds for every function EEE on complex matrices on QnQ_nQn​ admitting a finite Kraus representation E(X)=∑h=0q−1KhXKh†E(X)=\sum_{h=0}^{q-1}K_hXK_h^\daggerE(X)=∑h=0q−1​Kh​XKh†​ with q∈Nq\in\mathbb Nq∈N and ∑hKh†Kh=I\sum_hK_h^\dagger K_h=I∑h​Kh†​Kh​=I:

1−δ ≤ ∑r:{0,…,N−1}→B×Q2n∀w, ∥J^(r,w)−Rw(JE)∥ν≤ε ∏j=0N−1Re⁡tr⁡(Paj,bjJE)∣B∣,r(j)=(aj,bj).1-\delta\ \le\ \sum_{\substack{r:\{0,\ldots,N-1\}\to\mathcal B\times Q_{2n}\\ \forall w,\ \|\widehat J(r,w)-R_w(J_E)\|_\nu\le\varepsilon}} \ \prod_{j=0}^{N-1} \frac{\operatorname{Re}\operatorname{tr}(P_{a_j,b_j}J_E)}{|\mathcal B|}, \qquad r(j)=(a_j,b_j).1−δ ≤ r:{0,…,N−1}→B×Q2n​∀w, ∥J(r,w)−Rw​(JE​)∥ν​≤ε​∑​ j=0∏N−1​∣B∣Retr(Paj​,bj​​JE​)​,r(j)=(aj​,bj​).

Here, under the identification of a concatenated bit string with its two halves, (JE)(u,v),(u′,v′)=2−n(E(eu,u′))v,v′(J_E)_{(u,v),(u',v')}=2^{-n}(E(e_{u,u'}))_{v,v'}(JE​)(u,v),(u′,v′)​=2−n(E(eu,u′​))v,v′​, with eu,u′e_{u,u'}eu,u′​ the matrix unit, and

(Rw(J))(u,v),(u′,v′)=∑a,b∈Qna∘w=0, b∘w=0J(a[w←u], b[w←v]), (a[w←u′], b[w←v′]),\bigl(R_w(J)\bigr)_{(u,v),(u',v')} = \sum_{\substack{a,b\in Q_n\\a\circ w=0,\ b\circ w=0}} J_{(a[w\leftarrow u],\,b[w\leftarrow v]),\, (a[w\leftarrow u'],\,b[w\leftarrow v'])},(Rw​(J))(u,v),(u′,v′)​=a,b∈Qn​a∘w=0, b∘w=0​∑​J(a[w←u],b[w←v]),(a[w←u′],b[w←v′])​,

where a[w←u]a[w\leftarrow u]a[w←u] replaces the bits of aaa at positions w(i)w(i)w(i) by u(i)u(i)u(i) and leaves all other bits unchanged. The chosen error is ∥X∥F=(∑i,j∣Xi,j∣2)1/2\|X\|_{\mathrm F}=(\sum_{i,j}|X_{i,j}|^2)^{1/2}∥X∥F​=(∑i,j​∣Xi,j​∣2)1/2 or ∥X∥tr=Re⁡tr⁡X†X\|X\|_{\mathrm{tr}}=\operatorname{Re}\operatorname{tr}\sqrt{X^\dagger X}∥X∥tr​=RetrX†X​. The estimator is chosen before EEE, and the error requirement is simultaneous over all injections www. No conditions on the frame matrices ensure that the displayed record weights are probabilities, and no sign or range restrictions are imposed on ε,δ\varepsilon,\deltaε,δ. All of n,k,Nn,k,Nn,k,N may be zero; for N=0N=0N=0 the unique empty record has weight 111, and for k>nk>nk>n there are no injections www, so the record condition is vacuous.

QAlgorithms.Papers.Independent.Intakethird100.P66.ancillaReconstruction

For every natural number nnn, including 000, let Qn={0,1}nQ_n=\{0,1\}^nQn​={0,1}n, let FFF supply a finite nonempty type B\mathcal BB and arbitrary matrices Pa,bP_{a,b}Pa,b​ on QnQ_nQn​, and let EEE be any function from complex matrices on QnQ_nQn​ to themselves. Identify Q2nQ_{2n}Q2n​ with Qn×QnQ_n\times Q_nQn​×Qn​, define (JE)(u,v),(u′,v′)=2−n(E(eu,u′))v,v′(J_E)_{(u,v),(u',v')}=2^{-n}(E(e_{u,u'}))_{v,v'}(JE​)(u,v),(u′,v′)​=2−n(E(eu,u′​))v,v′​, where eu,u′e_{u,u'}eu,u′​ is the corresponding matrix unit, and write A⊗BA\otimes BA⊗B for the matrix whose entry at ((u,v),(u′,v′))((u,v),(u',v'))((u,v),(u′,v′)) is Au,u′Bv,v′A_{u,u'}B_{v,v'}Au,u′​Bv,v′​. Set CF(X)=∣B∣−1∑a,btr⁡(Pa,bX)Pa,b\mathcal C_F(X)=|\mathcal B|^{-1}\sum_{a,b}\operatorname{tr}(P_{a,b}X)P_{a,b}CF​(X)=∣B∣−1∑a,b​tr(Pa,b​X)Pa,b​ and let IF=CF−1\mathcal I_F=\mathcal C_F^{-1}IF​=CF−1​ when this map is injective, or the zero map otherwise. The defined reconstruction is

1∣B∣2∑a,c∈B∑b,d∈QnRe⁡tr⁡ ⁣((Pa,b⊗Pc,d)JE)(IF(Pa,b)⊗IF(Pc,d)),\frac1{|\mathcal B|^2} \sum_{a,c\in\mathcal B}\sum_{b,d\in Q_n} \operatorname{Re}\operatorname{tr}\!\bigl((P_{a,b}\otimes P_{c,d})J_E\bigr) \bigl(\mathcal I_F(P_{a,b})\otimes\mathcal I_F(P_{c,d})\bigr),∣B∣21​a,c∈B∑​b,d∈Qn​∑​Retr((Pa,b​⊗Pc,d​)JE​)(IF​(Pa,b​)⊗IF​(Pc,d​)),

where real coefficients act as complex scalars. No channel assumption on EEE or projector conditions on the frame matrices are imposed, and the result is zero if CF\mathcal C_FCF​ is not injective.

QAlgorithms.Papers.Independent.Intakethird100.P66.appendMatrixTensor

For all natural numbers a,ba,ba,b, including zero, and arbitrary complex matrices AAA and BBB indexed respectively by aaa-bit and bbb-bit strings, this defines a complex matrix on (a+b)(a+b)(a+b)-bit strings. Writing x=u∥vx=u\mathbin{\|}vx=u∥v and y=u′∥v′y=u'\mathbin{\|}v'y=u′∥v′ for concatenations with first blocks of length aaa and second blocks of length bbb, its entries are

(A⊗appendB)x,y=Au,u′Bv,v′.(A\otimes_{\mathrm{append}}B)_{x,y}=A_{u,u'}B_{v,v'}.(A⊗append​B)x,y​=Au,u′​Bv,v′​.

No conditions on AAA or BBB are required. A zero-length block has exactly one bit string, so its matrix is a scalar factor.

QAlgorithms.Papers.Independent.Intakethird100.P66.basisBornWeight

For every natural number mmm, including 000, let Qm={0,1}mQ_m=\{0,1\}^mQm​={0,1}m, and let FFF consist of a finite nonempty type B\mathcal BB and matrices Pa,b∈CQm×QmP_{a,b}\in\mathbb C^{Q_m\times Q_m}Pa,b​∈CQm​×Qm​ for every a∈Ba\in\mathcal Ba∈B and b∈Qmb\in Q_mb∈Qm​. For every matrix ρ∈CQm×Qm\rho\in\mathbb C^{Q_m\times Q_m}ρ∈CQm​×Qm​ and pair s=(a,b)∈B×Qms=(a,b)\in\mathcal B\times Q_ms=(a,b)∈B×Qm​, this definition assigns the real number

wF(ρ;(a,b))=Re⁡tr⁡(Pa,bρ)∣B∣.w_F(\rho;(a,b))=\frac{\operatorname{Re}\operatorname{tr}(P_{a,b}\rho)}{|\mathcal B|}.wF​(ρ;(a,b))=∣B∣Retr(Pa,b​ρ)​.

The data defining FFF impose no projector, positivity, or completeness conditions on the matrices Pa,bP_{a,b}Pa,b​, and ρ\rhoρ is arbitrary, so these numbers need not be nonnegative or sum to 111. When m=0m=0m=0, QmQ_mQm​ contains the single empty bit string.

QAlgorithms.Papers.Independent.Intakethird100.P66.basisMeasurementChannel

For every natural number mmm, including 000, let Qm={0,1}mQ_m=\{0,1\}^mQm​={0,1}m and let FFF consist of a finite nonempty type B\mathcal BB and arbitrary matrices Pa,b∈CQm×QmP_{a,b}\in\mathbb C^{Q_m\times Q_m}Pa,b​∈CQm​×Qm​. This definition constructs the complex-linear map CF:CQm×Qm→CQm×Qm\mathcal C_F:\mathbb C^{Q_m\times Q_m}\to\mathbb C^{Q_m\times Q_m}CF​:CQm​×Qm​→CQm​×Qm​ given, for every matrix XXX and every i,j∈Qmi,j\in Q_mi,j∈Qm​, by

(CF(X))i,j=∑k,l∈Qm(1∣B∣∑a∈B∑b∈Qm(Pa,b)l,k(Pa,b)i,j)Xk,l=1∣B∣∑a,btr⁡(Pa,bX) (Pa,b)i,j.\bigl(\mathcal C_F(X)\bigr)_{i,j} =\sum_{k,l\in Q_m} \left(\frac1{|\mathcal B|} \sum_{a\in\mathcal B}\sum_{b\in Q_m} (P_{a,b})_{l,k}(P_{a,b})_{i,j}\right)X_{k,l} =\frac1{|\mathcal B|}\sum_{a,b}\operatorname{tr}(P_{a,b}X)\,(P_{a,b})_{i,j}.(CF​(X))i,j​=k,l∈Qm​∑​​∣B∣1​a∈B∑​b∈Qm​∑​(Pa,b​)l,k​(Pa,b​)i,j​​Xk,l​=∣B∣1​a,b∑​tr(Pa,b​X)(Pa,b​)i,j​.

The displayed products contain no complex conjugation. The frame data impose no further conditions ensuring positivity, trace preservation, or injectivity of this map.

QAlgorithms.Papers.Independent.Intakethird100.P66.centeredVariance

For every natural number mmm, write Bm={0,1}m\mathcal B_m=\{0,1\}^mBm​={0,1}m, and let PPP consist of a probability measure μ\muμ on unitary matrices indexed by Bm\mathcal B_mBm​, with the requirement that the linear map

Cμ(X)=∫∑b∈Bm(UXU†)bb U†∣b⟩⟨b∣U dμ(U)\mathcal C_\mu(X)=\int\sum_{b\in\mathcal B_m}(UXU^\dagger)_{bb}\, U^\dagger|b\rangle\langle b|U\,d\mu(U)Cμ​(X)=∫b∈Bm​∑​(UXU†)bb​U†∣b⟩⟨b∣Udμ(U)

is injective; its inverse is therefore defined on all matrices of this size. For every complex matrix OOO indexed by Bm\mathcal B_mBm​, this defines centeredVariance⁡(P,O)=0\operatorname{centeredVariance}(P,O)=0centeredVariance(P,O)=0 if OOO is not Hermitian. If OOO is Hermitian, put O0=O−Tr⁡(O)I/2mO_0=O-\operatorname{Tr}(O)I/2^mO0​=O−Tr(O)I/2m; the value is

(sup⁡σ⪰0Tr⁡σ=1∫∑b∈BmRe⁡(UσU†)bb [Re⁡ ⁣(UCμ−1(O0)U†)bb]2 dμ(U))2.\left( \sqrt{\sup_{\substack{\sigma\succeq0\\\operatorname{Tr}\sigma=1}} \int\sum_{b\in\mathcal B_m} \operatorname{Re}(U\sigma U^\dagger)_{bb}\, \left[\operatorname{Re}\!\left(U\mathcal C_\mu^{-1}(O_0)U^\dagger\right)_{bb}\right]^2 \,d\mu(U)} \right)^2.​σ⪰0Trσ=1​sup​∫b∈Bm​∑​Re(UσU†)bb​[Re(UCμ−1​(O0​)U†)bb​]2dμ(U)​​2.

The supremum and square root are the total real operations used in the definition. The case m=0m=0m=0 is included, with B0\mathcal B_0B0​ consisting of the unique empty bit string.

QAlgorithms.Papers.Independent.Intakethird100.P66.choiSnapshot

For every natural number nnn, including 000, let Q2n={0,1}2nQ_{2n}=\{0,1\}^{2n}Q2n​={0,1}2n, and let FFF supply a finite nonempty type B\mathcal BB and arbitrary matrices Pa,b∈CQ2n×Q2nP_{a,b}\in\mathbb C^{Q_{2n}\times Q_{2n}}Pa,b​∈CQ2n​×Q2n​. Define

CF(X)=1∣B∣∑a∈B∑b∈Q2ntr⁡(Pa,bX) Pa,b.\mathcal C_F(X)=\frac1{|\mathcal B|}\sum_{a\in\mathcal B}\sum_{b\in Q_{2n}} \operatorname{tr}(P_{a,b}X)\,P_{a,b}.CF​(X)=∣B∣1​a∈B∑​b∈Q2n​∑​tr(Pa,b​X)Pa,b​.

For every s=(a,b)∈B×Q2ns=(a,b)\in\mathcal B\times Q_{2n}s=(a,b)∈B×Q2n​, this definition assigns the matrix 2nCF−1(Pa,b)2^n\mathcal C_F^{-1}(P_{a,b})2nCF−1​(Pa,b​) if CF\mathcal C_FCF​ is injective, and the zero matrix otherwise. The inverse is the inverse complex-linear endomorphism, and 2n2^n2n is regarded as a complex scalar. At n=0n=0n=0, the scaling factor is 111 and the matrices have one row and one column.

QAlgorithms.Papers.Independent.Intakethird100.P66.embedProcessObservable

For all natural numbers n,kn,kn,k, an injection w:{0,…,k−1}↪{0,…,n−1}w:\{0,\ldots,k-1\}\hookrightarrow\{0,\ldots,n-1\}w:{0,…,k−1}↪{0,…,n−1}, and an arbitrary complex matrix OOO on 2k2k2k-bit strings, this defines a matrix O~\widetilde OO on 2n2n2n-bit strings. For nnn-bit strings u,v,u′,v′u,v,u',v'u,v,u′,v′, its entries are

O~u∥v,  u′∥v′={O(u∘w)∥(v∘w),  (u′∘w)∥(v′∘w),if uj=uj′ and vj=vj′ for every j∉im⁡w,0,otherwise.\widetilde O_{u\mathbin{\|}v,\;u'\mathbin{\|}v'} = \begin{cases} O_{(u\circ w)\mathbin{\|}(v\circ w),\; (u'\circ w)\mathbin{\|}(v'\circ w)}, &\text{if }u_j=u'_j\text{ and }v_j=v'_j \text{ for every }j\notin\operatorname{im}w,\\ 0,&\text{otherwise}. \end{cases}Ou∥v,u′∥v′​={O(u∘w)∥(v∘w),(u′∘w)∥(v′∘w)​,0,​if uj​=uj′​ and vj​=vj′​ for every j∈/imw,otherwise.​

Here concatenation joins the indicated bit strings, and the injection entails k≤nk\le nk≤n. There is no Hermiticity assumption on OOO. If k=0k=0k=0, the result is the sole entry of OOO times the identity; if www covers every position, the condition outside its image is vacuous.

QAlgorithms.Papers.Independent.Intakethird100.P66.finiteMax

For every type AAA equipped with a finite enumeration and every function f:A→Rf:A\to\mathbb Rf:A→R, this defines finiteMax⁡(f)\operatorname{finiteMax}(f)finiteMax(f) to be max⁡a∈Af(a)\max_{a\in A}f(a)maxa∈A​f(a) when AAA is nonempty, and zero when AAA is empty. In the nonempty case the maximum may be negative; zero is only the specified value for the empty case.

QAlgorithms.Papers.Independent.Intakethird100.P66.frameInverse

For every natural number mmm, including 000, let Qm={0,1}mQ_m=\{0,1\}^mQm​={0,1}m, and let FFF supply a finite nonempty type B\mathcal BB and arbitrary complex matrices Pa,bP_{a,b}Pa,b​ indexed by a∈Ba\in\mathcal Ba∈B and b∈Qmb\in Q_mb∈Qm​. Define the complex-linear map

CF(X)=1∣B∣∑a∈B∑b∈Qmtr⁡(Pa,bX) Pa,b.\mathcal C_F(X)=\frac1{|\mathcal B|}\sum_{a\in\mathcal B}\sum_{b\in Q_m} \operatorname{tr}(P_{a,b}X)\,P_{a,b}.CF​(X)=∣B∣1​a∈B∑​b∈Qm​∑​tr(Pa,b​X)Pa,b​.

This definition assigns a complex-linear map IF\mathcal I_FIF​ on the same matrix space: if CF\mathcal C_FCF​ is injective, then IF=CF−1\mathcal I_F=\mathcal C_F^{-1}IF​=CF−1​, using the fact that an injective linear endomorphism of this finite-dimensional space is bijective; otherwise IF\mathcal I_FIF​ is the zero map. Injectivity is tested in the definition and is not assumed of FFF.

QAlgorithms.Papers.Independent.Intakethird100.P66.frameSnapshot

For every natural number mmm, including 000, let Qm={0,1}mQ_m=\{0,1\}^mQm​={0,1}m, and let FFF supply a finite nonempty type B\mathcal BB and arbitrary matrices Pa,b∈CQm×QmP_{a,b}\in\mathbb C^{Q_m\times Q_m}Pa,b​∈CQm​×Qm​. Form the complex-linear map

CF(X)=1∣B∣∑a∈B∑b∈Qmtr⁡(Pa,bX) Pa,b.\mathcal C_F(X)=\frac1{|\mathcal B|}\sum_{a\in\mathcal B}\sum_{b\in Q_m} \operatorname{tr}(P_{a,b}X)\,P_{a,b}.CF​(X)=∣B∣1​a∈B∑​b∈Qm​∑​tr(Pa,b​X)Pa,b​.

For every pair s=(a,b)∈B×Qms=(a,b)\in\mathcal B\times Q_ms=(a,b)∈B×Qm​, the defined snapshot is CF−1(Pa,b)\mathcal C_F^{-1}(P_{a,b})CF−1​(Pa,b​) if CF\mathcal C_FCF​ is injective, and is the zero matrix otherwise; the inverse exists in the injective case because the domain and codomain are the same finite-dimensional complex vector space. No projector or normalization conditions on Pa,bP_{a,b}Pa,b​ are assumed.

QAlgorithms.Papers.Independent.Intakethird100.P66.globalFrame

For every natural number mmm, assuming a specified finite enumeration of the projective group described below, this defines a frame with that group as its basis-choice set. Start with the subgroup of unitary matrices on mmm-bit strings generated by all matrices ic⨂jPji^c\bigotimes_j P_jic⨂j​Pj​, where c∈{0,1,2,3}c\in\{0,1,2,3\}c∈{0,1,2,3} and each PjP_jPj​ is one of the usual matrices I,X,Y,ZI,X,Y,ZI,X,Y,Z; take its normalizer in the full unitary group, and identify two normalizer elements U,VU,VU,V exactly when UXU†=VXV†UXU^\dagger=VXV^\daggerUXU†=VXV† for every complex matrix XXX. The resulting quotient is the basis-choice set, which is nonempty because it contains the identity class. For a class aaa, choose its designated quotient representative UaU_aUa​; for every outcome mmm-bit string bbb, the assigned matrix is

Pa,b(x,y)=(Ua)b,x‾ (Ua)b,y.P_{a,b}(x,y)=\overline{(U_a)_{b,x}}\,(U_a)_{b,y}.Pa,b​(x,y)=(Ua​)b,x​​(Ua​)b,y​.

The definition includes m=0m=0m=0, where the outcome and matrix index sets each contain one empty bit string.

QAlgorithms.Papers.Independent.Intakethird100.P66.matrixError

For every natural number mmm, including 000, every complex matrix XXX indexed by the bit strings Qm={0,1}mQ_m=\{0,1\}^mQm​={0,1}m, and either choice frobenius or trace, this definition returns respectively

(∑u,v∈Qm∣Xu,v∣2)1/2orRe⁡tr⁡X†X,\left(\sum_{u,v\in Q_m}|X_{u,v}|^2\right)^{1/2} \quad\text{or}\quad \operatorname{Re}\operatorname{tr}\sqrt{X^\dagger X},​u,v∈Qm​∑​∣Xu,v​∣2​1/2orRetrX†X​,

where X†X^\daggerX† is the conjugate transpose and the square root is the positive semidefinite square root supplied by continuous functional calculus. No Hermitian or positivity assumption on XXX is required. When m=0m=0m=0, XXX is a one-by-one matrix.

QAlgorithms.Papers.Independent.Intakethird100.P66.meanChoiSnapshot

For every natural number nnn, including 000, write Qn={0,1}nQ_n=\{0,1\}^nQn​={0,1}n and identify a 2n2n2n-bit string with its ordered pair of nnn-bit halves. Let FFF supply a finite nonempty type B\mathcal BB and arbitrary matrices Pa,bP_{a,b}Pa,b​ on Q2nQ_{2n}Q2n​, and let EEE be any function from complex matrices on QnQ_nQn​ to complex matrices on QnQ_nQn​, without a linearity or channel assumption. Define the matrix JEJ_EJE​ by

(JE)(u,v),(u′,v′)=2−n(E(eu,u′))v,v′,(J_E)_{(u,v),(u',v')}=2^{-n}\bigl(E(e_{u,u'})\bigr)_{v,v'},(JE​)(u,v),(u′,v′)​=2−n(E(eu,u′​))v,v′​,

where eu,u′e_{u,u'}eu,u′​ has entry 111 at (u,u′)(u,u')(u,u′) and 000 elsewhere. Also set CF(X)=∣B∣−1∑a,btr⁡(Pa,bX)Pa,b\mathcal C_F(X)=|\mathcal B|^{-1}\sum_{a,b}\operatorname{tr}(P_{a,b}X)P_{a,b}CF​(X)=∣B∣−1∑a,b​tr(Pa,b​X)Pa,b​, and let IF=CF−1\mathcal I_F=\mathcal C_F^{-1}IF​=CF−1​ if CF\mathcal C_FCF​ is injective and IF=0\mathcal I_F=0IF​=0 otherwise. This definition assigns

2n∣B∣∑a∈B∑b∈Q2nRe⁡tr⁡(Pa,bJE) IF(Pa,b),\frac{2^n}{|\mathcal B|} \sum_{a\in\mathcal B}\sum_{b\in Q_{2n}} \operatorname{Re}\operatorname{tr}(P_{a,b}J_E)\,\mathcal I_F(P_{a,b}),∣B∣2n​a∈B∑​b∈Q2n​∑​Retr(Pa,b​JE​)IF​(Pa,b​),

with the real coefficients regarded as complex scalars. The expression is zero when CF\mathcal C_FCF​ is not injective; its coefficients are not assumed to form a probability distribution.

QAlgorithms.Papers.Independent.Intakethird100.P66.overlapObservable

For every natural number nnn and arbitrary complex matrices ρ,σ\rho,\sigmaρ,σ indexed by {0,1}n\{0,1\}^n{0,1}n, this defines a complex matrix indexed by 2n2n2n-bit strings through

overlapObservable⁡(ρ,σ)a ∥ b,  a′ ∥ b′=ρa′,a σb,b′,\operatorname{overlapObservable}(\rho,\sigma)_{a\,\Vert\,b,\;a'\,\Vert\,b'} =\rho_{a',a}\,\sigma_{b,b'},overlapObservable(ρ,σ)a∥b,a′∥b′​=ρa′,a​σb,b′​,

where a,a′,b,b′∈{0,1}na,a',b,b'\in\{0,1\}^na,a′,b,b′∈{0,1}n and ∥\Vert∥ denotes concatenation. Equivalently, it is ρT⊗σ\rho^{\mathsf T}\otimes\sigmaρT⊗σ expressed in concatenated-bit coordinates; the transpose does not conjugate entries. Neither input is required to be a density matrix or Hermitian, and n=0n=0n=0 is allowed.

QAlgorithms.Papers.Independent.Intakethird100.P66.pauliFrame

For every natural number mmm, this defines a frame whose finite, nonempty basis-choice set consists of all functions a:{0,…,m−1}→{X,Y,Z}×{false,true}a:\{0,\ldots,m-1\}\to\{X,Y,Z\}\times\{\mathrm{false},\mathrm{true}\}a:{0,…,m−1}→{X,Y,Z}×{false,true}, with the constant choice (Z,true)(Z,\mathrm{true})(Z,true) witnessing nonemptiness. For an outcome bit string bbb, write aj=(Aj,tj)a_j=(A_j,t_j)aj​=(Aj​,tj​) and let sj=1s_j=1sj​=1 if tj≠bjt_j\ne b_jtj​=bj​, and sj=−1s_j=-1sj​=−1 otherwise. The assigned matrix is

Pa,b(y,z)=∏j=0m−1[I+sjσAj2]yj,zj,σX=(0110),σY=(0−ii0),σZ=(100−1),P_{a,b}(y,z)= \prod_{j=0}^{m-1} \left[\frac{I+s_j\sigma_{A_j}}2\right]_{y_j,z_j}, \qquad \sigma_X=\begin{pmatrix}0&1\\1&0\end{pmatrix},\quad \sigma_Y=\begin{pmatrix}0&-i\\i&0\end{pmatrix},\quad \sigma_Z=\begin{pmatrix}1&0\\0&-1\end{pmatrix},Pa,b​(y,z)=j=0∏m−1​[2I+sj​σAj​​​]yj​,zj​​,σX​=(01​10​),σY​=(0i​−i0​),σZ​=(10​0−1​),

with rows and columns ordered as false, true. This expands the factor 3m3^m3m multiplying the defined Pauli measurement matrix, whose factor is 3−m3^{-m}3−m. When m=0m=0m=0, both the choice set and the outcome set are singletons, and the empty product gives the one-entry matrix [1][1][1].

QAlgorithms.Papers.Independent.Intakethird100.P66.pauliNormEnvelope

For every natural number kkk, this defines

pauliNormEnvelope⁡(k)=max⁡p∈{I,X,Y,Z}2k∥Qp∥op2,(Qp)y,z=∏j=02k−1(pj)yj,zj,y,z∈{0,1}2k,\operatorname{pauliNormEnvelope}(k)= \max_{p\in\{I,X,Y,Z\}^{2k}}\|Q_p\|_{\mathrm{op}}^2, \qquad (Q_p)_{y,z}=\prod_{j=0}^{2k-1}(p_j)_{y_j,z_j}, \quad y,z\in\{0,1\}^{2k},pauliNormEnvelope(k)=p∈{I,X,Y,Z}2kmax​∥Qp​∥op2​,(Qp​)y,z​=j=0∏2k−1​(pj​)yj​,zj​​,y,z∈{0,1}2k,

where ∥⋅∥op\|\cdot\|_{\mathrm{op}}∥⋅∥op​ is the operator norm for Euclidean norms, and the four matrices, in bit order 0,10,10,1, are

I=(1001),X=(0110),Y=(0−ii0),Z=(100−1).I=\begin{pmatrix}1&0\\0&1\end{pmatrix},\quad X=\begin{pmatrix}0&1\\1&0\end{pmatrix},\quad Y=\begin{pmatrix}0&-i\\i&0\end{pmatrix},\quad Z=\begin{pmatrix}1&0\\0&-1\end{pmatrix}.I=(10​01​),X=(01​10​),Y=(0i​−i0​),Z=(10​0−1​).

The maximum uses zero as its default for an empty indexing type, although this particular indexing type is always nonempty. When k=0k=0k=0, it contains the unique empty assignment, and its empty product is the 1×11\times11×1 identity matrix.

QAlgorithms.Papers.Independent.Intakethird100.P66.primitiveRecordLaw

For every natural number mmm, write Bm={0,1}m\mathcal B_m=\{0,1\}^mBm​={0,1}m, and let PPP specify a probability measure μ\muμ on unitary matrices indexed by Bm\mathcal B_mBm​ for which the map X↦∫∑b(UXU†)bbU†∣b⟩⟨b∣U dμ(U)X\mapsto\int\sum_b(UXU^\dagger)_{bb}U^\dagger|b\rangle\langle b|U\,d\mu(U)X↦∫∑b​(UXU†)bb​U†∣b⟩⟨b∣Udμ(U) is injective. For every complex matrix ρ\rhoρ indexed by Bm\mathcal B_mBm​ and every natural number NNN, this defines the product measure νP,ρ⊗N\nu_{P,\rho}^{\otimes N}νP,ρ⊗N​ on records (Uj,bj)j=0N−1(U_j,b_j)_{j=0}^{N-1}(Uj​,bj​)j=0N−1​, where

νP,ρ=∑b∈Bm(U↦(U,b))∗(max⁡{Re⁡(UρU†)bb,0} μ(dU)).\nu_{P,\rho} =\sum_{b\in\mathcal B_m}(U\mapsto(U,b))_* \left(\max\{\operatorname{Re}(U\rho U^\dagger)_{bb},0\}\,\mu(dU)\right).νP,ρ​=b∈Bm​∑​(U↦(U,b))∗​(max{Re(UρU†)bb​,0}μ(dU)).

There are no density-matrix assumptions on ρ\rhoρ. When N=0N=0N=0, the record space consists of the unique empty record and the product measure assigns it mass one.

QAlgorithms.Papers.Independent.Intakethird100.P66.primitiveShotLaw

For every natural number mmm, let Bm={0,1}m\mathcal B_m=\{0,1\}^mBm​={0,1}m, and let PPP specify a probability measure μ\muμ on unitary matrices indexed by Bm\mathcal B_mBm​ such that

X⟼∫∑b∈Bm(UXU†)bb U†∣b⟩⟨b∣U dμ(U)X\longmapsto\int\sum_{b\in\mathcal B_m}(UXU^\dagger)_{bb}\, U^\dagger|b\rangle\langle b|U\,d\mu(U)X⟼∫b∈Bm​∑​(UXU†)bb​U†∣b⟩⟨b∣Udμ(U)

is injective. For any complex matrix ρ\rhoρ indexed by Bm\mathcal B_mBm​, this defines a measure on pairs (U,b)(U,b)(U,b) by

νP,ρ=∑b∈Bm(U↦(U,b))∗(max⁡{Re⁡(UρU†)bb,0} μ(dU)).\nu_{P,\rho} =\sum_{b\in\mathcal B_m} (U\mapsto(U,b))_* \left(\max\{\operatorname{Re}(U\rho U^\dagger)_{bb},0\}\,\mu(dU)\right).νP,ρ​=b∈Bm​∑​(U↦(U,b))∗​(max{Re(UρU†)bb​,0}μ(dU)).

Thus each summand weights μ\muμ by the nonnegative part of the indicated real diagonal entry and then attaches the fixed outcome bbb. No assumption says that ρ\rhoρ is Hermitian, positive semidefinite, or trace one, so the definition does not require this measure to be a probability measure. The case m=0m=0m=0 is included.

QAlgorithms.Papers.Independent.Intakethird100.P66.processChoi

For every natural number nnn, including zero, and every function EEE from complex matrices on nnn-bit strings to complex matrices on nnn-bit strings, this defines a matrix JEJ_EJE​ on 2n2n2n-bit strings by

(JE)u∥v,  u′∥v′=(E(eu,u′))v,v′,(J_E)_{u\mathbin{\|}v,\;u'\mathbin{\|}v'}=\bigl(E(e_{u,u'})\bigr)_{v,v'},(JE​)u∥v,u′∥v′​=(E(eu,u′​))v,v′​,

where u,u′,v,v′u,u',v,v'u,u′,v,v′ are nnn-bit strings and eu,u′e_{u,u'}eu,u′​ is the matrix whose only nonzero entry is 111 at row uuu, column u′u'u′. There is no assumption that EEE is linear or is a channel. When n=0n=0n=0, the sole entry is the sole entry of E([1])E([1])E([1]).

QAlgorithms.Papers.Independent.Intakethird100.P66.processChoiState

For every natural number nnn, including zero, and arbitrary function EEE from complex matrices on nnn-bit strings to themselves, this defines the matrix with entries

(JEscaled)u∥v,  u′∥v′=2−n(E(eu,u′))v,v′,(J_E^{\mathrm{scaled}})_{u\mathbin{\|}v,\;u'\mathbin{\|}v'}=2^{-n}\bigl(E(e_{u,u'})\bigr)_{v,v'},(JEscaled​)u∥v,u′∥v′​=2−n(E(eu,u′​))v,v′​,

where concatenation places the first nnn-bit string before the second, and eu,u′e_{u,u'}eu,u′​ has entry 111 at (u,u′)(u,u')(u,u′) and zero elsewhere. No linearity, positivity, or trace condition is imposed on EEE or the resulting matrix. For n=0n=0n=0, the scaling factor is 111.

QAlgorithms.Papers.Independent.Intakethird100.P66.processMarginal

For all natural numbers n,kn,kn,k, an arbitrary complex matrix ρ\rhoρ on 2n2n2n-bit strings, and an injection w:{0,…,k−1}↪{0,…,n−1}w:\{0,\ldots,k-1\}\hookrightarrow\{0,\ldots,n-1\}w:{0,…,k−1}↪{0,…,n−1}, this defines a matrix on 2k2k2k-bit strings as follows. For an nnn-bit string aaa and a kkk-bit string uuu, let a[w←u]a[w\leftarrow u]a[w←u] have value uiu_iui​ at position w(i)w(i)w(i) and value aja_jaj​ at every position outside the image of www. Then

ρu∥v,  u′∥v′ w=∑a,b∈{0,1}naw(i)=bw(i)=0 for every iρ a[w←u]∥b[w←v],  a[w←u′]∥b[w←v′].\rho^{\,w}_{u\mathbin{\|}v,\;u'\mathbin{\|}v'} = \sum_{\substack{a,b\in\{0,1\}^n\\ a_{w(i)}=b_{w(i)}=0\ \text{for every }i}} \rho_{\,a[w\leftarrow u]\mathbin{\|}b[w\leftarrow v],\; a[w\leftarrow u']\mathbin{\|}b[w\leftarrow v']}.ρu∥v,u′∥v′w​=a,b∈{0,1}naw(i)​=bw(i)​=0 for every i​∑​ρa[w←u]∥b[w←v],a[w←u′]∥b[w←v′]​.

The injection entails k≤nk\le nk≤n. No density-matrix assumption is imposed on ρ\rhoρ. For k=0k=0k=0, this is the one-entry matrix containing tr⁡ρ\operatorname{tr}\rhotrρ; when www covers all positions, only the all-zero choices of a,ba,ba,b contribute.

QAlgorithms.Papers.Independent.Intakethird100.P66.recordProbability

For every pair of natural numbers m,Nm,Nm,N, let Qm={0,1}mQ_m=\{0,1\}^mQm​={0,1}m, let FFF consist of a finite nonempty type B\mathcal BB and arbitrary complex matrices Pa,bP_{a,b}Pa,b​ indexed by a∈Ba\in\mathcal Ba∈B and b∈Qmb\in Q_mb∈Qm​, and let ρ\rhoρ be any complex matrix indexed by QmQ_mQm​. For every predicate E\mathcal EE on records r:{0,…,N−1}→B×Qmr:\{0,\ldots,N-1\}\to\mathcal B\times Q_mr:{0,…,N−1}→B×Qm​, this definition assigns

∑r:{0,…,N−1}→B×QmE(r) ∏j=0N−1Re⁡tr⁡(Paj,bjρ)∣B∣,r(j)=(aj,bj).\sum_{\substack{r:\{0,\ldots,N-1\}\to\mathcal B\times Q_m\\ \mathcal E(r)}} \ \prod_{j=0}^{N-1} \frac{\operatorname{Re}\operatorname{tr}(P_{a_j,b_j}\rho)}{|\mathcal B|}, \qquad r(j)=(a_j,b_j).r:{0,…,N−1}→B×Qm​E(r)​∑​ j=0∏N−1​∣B∣Retr(Paj​,bj​​ρ)​,r(j)=(aj​,bj​).

No assumptions ensure that this expression is a probability. For N=0N=0N=0, there is one empty record and its product is 111, so the result is 111 if that record satisfies E\mathcal EE and 000 otherwise; m=0m=0m=0 is also allowed.

QAlgorithms.Papers.Independent.Intakethird100.P66.reducedLog

For all natural numbers n,kn,kn,k and every real number δ\deltaδ, this defines

reducedLog⁡(n,k,δ)=log⁡ ⁣(2(8n)2kδ).\operatorname{reducedLog}(n,k,\delta) =\log\!\left(\frac{2(8n)^{2k}}{\delta}\right).reducedLog(n,k,δ)=log(δ2(8n)2k​).

Here the real logarithm is total: log⁡0=0\log0=0log0=0, and for a negative argument it equals the logarithm of its absolute value; division by zero gives zero. Consequently δ=0\delta=0δ=0 gives zero. The exponent is zero when k=0k=0k=0, including when n=0n=0n=0, so that case gives log⁡(2/δ)\log(2/\delta)log(2/δ); when n=0n=0n=0 and k>0k>0k>0, the result is zero. There are no positivity assumptions on n,k,δn,k,\deltan,k,δ.

QAlgorithms.Papers.Independent.Intakethird100.P66.reducedVariance

For every natural number nnn, let Bj={0,1}j\mathcal B_j=\{0,1\}^jBj​={0,1}j, and let PPP specify a probability measure μ\muμ on unitary matrices indexed by B2n\mathcal B_{2n}B2n​ with injective linear map

Cμ(X)=∫∑b∈B2n(UXU†)bbU†∣b⟩⟨b∣U dμ(U).\mathcal C_\mu(X)=\int\sum_{b\in\mathcal B_{2n}} (UXU^\dagger)_{bb}U^\dagger|b\rangle\langle b|U\,d\mu(U).Cμ​(X)=∫b∈B2n​∑​(UXU†)bb​U†∣b⟩⟨b∣Udμ(U).

For each natural number kkk, this defines the maximum of the following quantity over all injections w:{0,…,k−1}↪{0,…,n−1}w:\{0,\ldots,k-1\}\hookrightarrow\{0,\ldots,n-1\}w:{0,…,k−1}↪{0,…,n−1} and all choices p0,…,p2k−1∈{I,X,Y,Z}p_0,\ldots,p_{2k-1}\in\{I,X,Y,Z\}p0​,…,p2k−1​∈{I,X,Y,Z}. Here

I=(1001),X=(0110),Y=(0−ii0),Z=(100−1),I=\begin{pmatrix}1&0\\0&1\end{pmatrix},\quad X=\begin{pmatrix}0&1\\1&0\end{pmatrix},\quad Y=\begin{pmatrix}0&-i\\i&0\end{pmatrix},\quad Z=\begin{pmatrix}1&0\\0&-1\end{pmatrix},I=(10​01​),X=(01​10​),Y=(0i​−i0​),Z=(10​0−1​),

and QpQ_pQp​ is the matrix with entries (Qp)s,t=∏j=02k−1(pj)sj,tj(Q_p)_{s,t}=\prod_{j=0}^{2k-1}(p_j)_{s_j,t_j}(Qp​)s,t​=∏j=02k−1​(pj​)sj​,tj​​. Define Ow,pO_{w,p}Ow,p​, indexed by pairs of nnn-bit strings, by

(Ow,p)(a,b),(a′,b′)={(Qp)(a∘w,b∘w),(a′∘w,b′∘w),aj=aj′ and bj=bj′ for every j∉range⁡(w),0,otherwise.(O_{w,p})_{(a,b),(a',b')}= \begin{cases} (Q_p)_{(a\circ w,b\circ w),(a'\circ w,b'\circ w)}, & a_j=a'_j\ \text{and }b_j=b'_j\text{ for every }j\notin\operatorname{range}(w),\\ 0,&\text{otherwise}. \end{cases}(Ow,p​)(a,b),(a′,b′)​={(Qp​)(a∘w,b∘w),(a′∘w,b′∘w)​,0,​aj​=aj′​ and bj​=bj′​ for every j∈/range(w),otherwise.​

For any matrix OOO, the quantity being maximized is zero if OOO is not Hermitian; otherwise, with O0=O−Tr⁡(O)I/22nO_0=O-\operatorname{Tr}(O)I/2^{2n}O0​=O−Tr(O)I/22n, it is

(sup⁡σ⪰0Tr⁡σ=1∫∑b∈B2nRe⁡(UσU†)bb[Re⁡ ⁣(UCμ−1(O0)U†)bb]2 dμ(U))2,\left( \sqrt{\sup_{\substack{\sigma\succeq0\\\operatorname{Tr}\sigma=1}} \int\sum_{b\in\mathcal B_{2n}} \operatorname{Re}(U\sigma U^\dagger)_{bb} \left[\operatorname{Re}\!\left(U\mathcal C_\mu^{-1}(O_0)U^\dagger\right)_{bb}\right]^2 \,d\mu(U)} \right)^2,​σ⪰0Trσ=1​sup​∫b∈B2n​∑​Re(UσU†)bb​[Re(UCμ−1​(O0​)U†)bb​]2dμ(U)​​2,

evaluated at O=Ow,pO=O_{w,p}O=Ow,p​. If the indexing set is empty, the value is defined to be zero; in particular this happens when k>nk>nk>n. The case k=0k=0k=0 includes the unique empty injection and empty Pauli assignment, whose matrix product is the scalar identity.

QAlgorithms.Papers.Independent.Intakethird100.P66.sampleCount

For every natural number kkk and real number BBB, this defines the natural number

sampleCount⁡(k,B)={0,k=0,max⁡{0,⌈B⌉},k≠0.\operatorname{sampleCount}(k,B)= \begin{cases} 0,&k=0,\\ \max\{0,\lceil B\rceil\},&k\ne0. \end{cases}sampleCount(k,B)={0,max{0,⌈B⌉},​k=0,k=0.​

Thus k=0k=0k=0 gives zero regardless of BBB, and B≤0B\le0B≤0 gives zero for every kkk.

QAlgorithms.Papers.Independent.Intakethird100.P66.singleCliffordFrame

Assuming a specified finite enumeration of the one-qubit projective group, this recursively defines a frame for every natural number mmm. This projective group is obtained by taking the normalizer, within the one-qubit unitary group, of the subgroup generated by icPi^cPicP for c∈{0,1,2,3}c\in\{0,1,2,3\}c∈{0,1,2,3} and P∈{I,X,Y,Z}P\in\{I,X,Y,Z\}P∈{I,X,Y,Z}, and identifying U,VU,VU,V when UXU†=VXV†UXU^\dagger=VXV^\daggerUXU†=VXV† for every complex 2×22\times22×2 matrix XXX. The zero-bit frame has a singleton choice set and assigned matrix [1][1][1]. At each successor, its choice set is the previous choice set times this projective group, and its matrices are the appended tensor products of the previous matrices with ((Ua)b,x‾(Ua)b,y)x,y\bigl(\overline{(U_a)_{b,x}}(U_a)_{b,y}\bigr)_{x,y}((Ua​)b,x​​(Ua​)b,y​)x,y​, where UaU_aUa​ is the designated representative of the new class and bbb is the new outcome bit. Thus, identifying choices with mmm successive classes a0,…,am−1a_0,\ldots,a_{m-1}a0​,…,am−1​, the assigned matrix for outcome bbb has entries

Pa,b(x,y)=∏j=0m−1(Uaj)bj,xj‾ (Uaj)bj,yj.P_{a,b}(x,y)=\prod_{j=0}^{m-1} \overline{(U_{a_j})_{b_j,x_j}}\,(U_{a_j})_{b_j,y_j}.Pa,b​(x,y)=j=0∏m−1​(Uaj​​)bj​,xj​​​(Uaj​​)bj​,yj​​.

At m=0m=0m=0, the product is empty and equals 111.

QAlgorithms.Papers.Independent.Intakethird100.P66.tensorFrame

For all natural numbers a,ba,ba,b and arbitrary frames FFF and GGG on respectively aaa and bbb bits, this defines a frame on a+ba+ba+b bits. A frame here supplies a finite, nonempty choice set and an arbitrary complex matrix for each choice and outcome bit string. The new choice set is the Cartesian product of the two supplied choice sets, with its induced finite enumeration and nonemptiness. For choices f,gf,gf,g, outcome x=u∥vx=u\mathbin{\|}vx=u∥v, and matrix indices y=r∥sy=r\mathbin{\|}sy=r∥s and z=r′∥s′z=r'\mathbin{\|}s'z=r′∥s′, the assigned matrix has entry

P(f,g), u∥v(y,z)=(Ff,u)r,r′(Gg,v)s,s′.P_{(f,g),\,u\mathbin{\|}v}(y,z) =(F_{f,u})_{r,r'}(G_{g,v})_{s,s'}.P(f,g),u∥v​(y,z)=(Ff,u​)r,r′​(Gg,v​)s,s′​.

No additional matrix conditions are assumed. Either block length may be zero, in which case that block contributes its one-entry matrix as a scalar factor.

QAlgorithms.Papers.Independent.Intakethird100.P66.traceSampleLog

For all natural numbers n,kn,kn,k and every real number δ\deltaδ, this defines

traceSampleLog⁡(n,k,δ)=log⁡ ⁣((24n)2kδ).\operatorname{traceSampleLog}(n,k,\delta) =\log\!\left(\frac{(24n)^{2k}}{\delta}\right).traceSampleLog(n,k,δ)=log(δ(24n)2k​).

The real logarithm is total, with log⁡0=0\log0=0log0=0 and log⁡x=log⁡∣x∣\log x=\log|x|logx=log∣x∣ for x≠0x\ne0x=0, and division by zero gives zero. Thus δ=0\delta=0δ=0 gives zero; k=0k=0k=0, including n=k=0n=k=0n=k=0, gives log⁡(1/δ)\log(1/\delta)log(1/δ); and n=0n=0n=0 with k>0k>0k>0 gives zero. No positivity assumptions are imposed.

QAlgorithms.Papers.Independent.Intakethird100.P66.twoSidedReconstruction

For every natural number nnn, including 000, let Qn={0,1}nQ_n=\{0,1\}^nQn​={0,1}n, let 0n0_n0n​ be its all-false string, let FFF supply a finite nonempty type B\mathcal BB and arbitrary complex matrices Pa,bP_{a,b}Pa,b​ on QnQ_nQn​, and let EEE be any function from complex matrices on QnQ_nQn​ to themselves. Define CF(X)=∣B∣−1∑a,btr⁡(Pa,bX)Pa,b\mathcal C_F(X)=|\mathcal B|^{-1}\sum_{a,b}\operatorname{tr}(P_{a,b}X)P_{a,b}CF​(X)=∣B∣−1∑a,b​tr(Pa,b​X)Pa,b​ and let IF\mathcal I_FIF​ be its inverse complex-linear map if it is injective, or the zero map otherwise. With A⊗BA\otimes BA⊗B represented on concatenated bit strings by (A⊗B)(u,v),(u′,v′)=Au,u′Bv,v′(A\otimes B)_{(u,v),(u',v')}=A_{u,u'}B_{v,v'}(A⊗B)(u,v),(u′,v′)​=Au,u′​Bv,v′​, this definition assigns

1∣B∣2∑a,c∈B∑d∈QnRe⁡tr⁡ ⁣(Pc,d E(Pa,0n))(IF(Pa,0nT)⊗IF(Pc,d)).\frac1{|\mathcal B|^2} \sum_{a,c\in\mathcal B}\sum_{d\in Q_n} \operatorname{Re}\operatorname{tr}\!\bigl(P_{c,d}\,E(P_{a,0_n})\bigr) \left(\mathcal I_F(P_{a,0_n}^{\mathsf T})\otimes \mathcal I_F(P_{c,d})\right).∣B∣21​a,c∈B∑​d∈Qn​∑​Retr(Pc,d​E(Pa,0n​​))(IF​(Pa,0n​T​)⊗IF​(Pc,d​)).

Here T{}^{\mathsf T}T denotes ordinary transpose without conjugation, and the real coefficients act as complex scalars. Only the outcome 0n0_n0n​ is used for the first frame matrix. No channel assumption on EEE or projector conditions on the frame are imposed; if CF\mathcal C_FCF​ is not injective, the result is 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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