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Quantum Singular-Value Transformation — Examples

1 · Prerequisites

2 · Summary

The rank-one example verifies the unitary dilation and degree-one QSVT block at every singular value σ∈[0,1], including both endpoints. The counterexample takes the zero map and shows that assigning nonzero values to zero-singular-vector pairs makes a cross-space rank-one sum depend on independent kernel-basis choices. The stated odd and even conventions remove that ambiguity.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

CounterexampleConstruction: Literature-sourcedVerification: AI-adaptedprecheck passjudge pass (gpt-6-luna)Open item page →

Parity violation makes singular-value action basis dependent

Statement

A false extension of the odd singular-value formula that assigns a nonzero coefficient to zero-singular-vector pairs depends on arbitrary basis choices. Take A=0:C→C and the scalar function f(x)=1. Pair the right zero vector v=1 with either left zero vector u=1 or u=−1. The resulting rank-one sums are respectively I and −I, despite the same zero map A.

Facts & Assumptions

Given: The zero linear map A:C→C, the scalar value f(0)=1, and the rank-one map convention of Dirac Notation Conversion.

[F1]

Odd and even singular-value transforms: an odd singular-value transform sums only over positive singular pairs, while an even right transform uses f(0) times the canonical projection onto ker⁡A.

[F2]

Dirac Notation Conversion: ∣u⟩⟨v∣ maps x to ⟨x,v⟩rootu.

Proof

1.1givenF2algebra

For A=0, the entire domain and codomain are zero-singular spaces; both u=1 and u=−1 are unit left-kernel vectors, and v=1 is a unit right-kernel vector. With the first pairing, ∣1⟩⟨1∣ sends x to x, so the false zero-pair sum with coefficient f(0)=1 is I.

2.1F1F2step 1.1algebra∎

With the second equally valid left singular basis, ∣−1⟩⟨1∣ sends x to −x, so the same false rule gives −I. Since I≠−I on C, this rule is not basis independent. The valid odd definition avoids the defect because odd polynomials have f(0)=0 and the sum contains only positive singular values; the valid even definition adds f(0)Πker⁡A=I, which is canonical and unchanged by the choice of kernel basis.

ExampleConstruction: Literature-sourcedVerification: AI-adaptedprecheck passjudge pass (gpt-6-luna)Open item page →

Rank-one PUE singular-plane calculation

Example

Let 0≤σ≤1, H=C2, Uσ=(σ1−σ21−σ2−σ), and ΠR=ΠL=∣0⟩⟨0∣. The PUE block is the scalar matrix A=[σ]. Use the degree-one phase list (0,0), whose scalar polynomial is P(x)=x.

Facts & Assumptions

Given: σ∈[0,1], the standard orthonormal basis ∣0⟩,∣1⟩ of C2, the PUE definition, and the ordered QSVT sequence.

[F1]

PUE singular-space invariant decomposition: for 0<σ<1, the matrix of the PUE unitary on its singular plane is WR(σ); at σ=0 the right kernel maps into the left projector complement, and at σ=1 the singular block is a line.

[F2]

QSVT action on singular subspaces: degree-one QSVT compresses to the odd singular-value transform with coefficient P(σ), including the zero-kernel case.

Proof

1.1givenF1algebra

Put s=1−σ2. Direct multiplication gives Uσ∗Uσ=Uσ2=(σ2+s2σs−σsσs−σss2+σ2)=I, so Uσ is unitary. The projection onto ∣0⟩ gives A∣0⟩=ΠLUσ∣0⟩=σ∣0⟩, hence the PUE block is [σ]. Its complementary matrix entry is s, so the ordered basis realizes WR(σ) on the full ambient space: for 0<σ<1 this is the singular plane, at σ=0 it is the zero-kernel/complement block, and at σ=1 it splits into the singular line C∣0⟩ and residual complement C∣1⟩.

2.1F1F2step 1.1algebra∎

The zero phases make both endpoint phase matrices the identity, so the degree-one sequence is Uσ itself. Its compressed block is ΠLUσΠR∣HR=[σ]. The scalar polynomial is the upper-left entry of WR(x), namely P(x)=x; therefore for σ>0 the odd transform is PoddSV(A)=[P(σ)]=[σ], and for σ=0 the positive singular sum is empty and both blocks are zero. The same formulas give [1] at σ=1.

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