QuantumComputinglib learn · inspect · formalize
Checked on this commit 4,524 public declarations commit 4e2c5b2c0be5 Build record

QuantumComputingBench · graph-grounded exercise book

Polynomial Signals

Follow the roles of input states, operator access, polynomial transformations and output interpretation. Source-only algorithm questions keep their assumptions and query/gate/readout boundaries explicit.

Back to Quantum Scientific Computing

test_public · proof

Exercise PLAN-502

Let A be a Hermitian n-qubit operator and let U be a unitary on one flag ancilla and the system whose exact clean block is A: J†UJ=A, where J maps v to |0>v. Do not assume U is Hermitian. Set P=JJ† and R=2P-I. For a unit…

primary source nl only

test_public · boundary

Exercise PLAN-503

On the invariant plane attached to a value t in the closed interval from minus one to one, the qubitization iterate acts as the plane rotation M = [[t, -sqrt(1-t^2)],[sqrt(1-t^2), t]]. Prove that the k-th power of M has …

primary source nl only

test_public · proof

Exercise PLAN-504

Let A be a general (not necessarily normal) n-qubit operator with singular value decomposition sending each right singular vector v_i to sigma_i times the left singular vector w_i. A block-encoding unitary U realizes A i…

primary source nl only

test_public · counterexample

Exercise PLAN-505

Consider the two-by-two operator A that sends the first basis vector to zero and the second basis vector to the first (the strictly upper-triangular nilpotent). A tempting inference says: since the only eigenvalue of A i…

primary source nl only

test_public · proof

Exercise PLAN-506

A unitary U is written in two-by-two block form with top-left block B occupying the first p coordinates (p at most q, total p+q). Prove that the singular values of the top-left block B all lie in the closed interval from…

primary source nl only

test_public · counterexample

Exercise PLAN-507

In the cosine-sine view of qubitization the flag reflection is built from the single-qubit operator Z acting on the ancilla flag, and the large outer unitaries that diagonalize the construction are block-diagonal with re…

primary source nl only

test_public · proof

Exercise PLAN-508

To build a block encoding of a linear combination of even Chebyshev transforms, sum over k from 0 to K-1 of coefficients times the degree-2k Chebyshev transform, one needs a select operation that, conditioned on an index…

primary source nl only

test_public · proof

Exercise PLAN-509

The pure qubitization-plus-linear-combination construction directly produces block encodings of polynomials of DEFINITE parity (all-even or all-odd Chebyshev content). Suppose instead you are given a general real polynom…

primary source nl only

test_public · concept

Exercise PLAN-510

A single-ancilla block encoding alone does not specify its factor or error: with J|psi>=|0>_s|psi>, an exact (kappa,1)-block encoding satisfies J†U J=A/kappa for known kappa>0, while an approximate one only satisfies ||A…

primary source nl only

test_public · proof

Exercise PLAN-511

Suppose an operator A maps an N-dimensional input space into an N'-dimensional output space and is accessed through a single unitary U on a larger space together with two projectors: an input projector of rank N and an o…

primary source nl only

test_public · proof

Exercise PLAN-512

Take the smallest nontrivial subspace-encoding example: a four-dimensional space, the identity as the accessing unitary, an input projector that keeps the first qubit in its zero state, and an output projector obtained b…

primary source nl only

test_public · proof

Exercise PLAN-513

Keep the original promise of exactly one marked basis state among N states, with no exclusion of the positive endpoint N=1. Put g=|marked>, psi=N^(-1/2) sum_x |x>, R_g=I-2|g><g| and R_psi=2|psi><psi|-I, with Grover itera…

primary source nl only

test_public · proof

Exercise PLAN-514

For the single-marked search with N basis states, after choosing the number of iterations to be the nearest integer at or below a quarter of pi over the half-angle minus one half, prove that the failure probability (the …

primary source nl only

test_public · proof

Exercise PLAN-515

Keep the original assumptions: M>=1 marked states among N basis states, M known in advance, so the allowed domain includes M=N. Let Π_mark project onto the marked basis states, psi be uniform, and G=(2|psi><psi|-I)(I-2Π_…

primary source nl only

test_public · proof

Exercise PLAN-516

View Grover's single-marked search through qubitization beyond the computational basis. Let the uniform state and the marked state define rank-one projectors, and let the reflection about the uniform state play the role …

primary source nl only

test_public · boundary

Exercise PLAN-517

Let k be a natural number, m=2k+1, and T_m the first-kind Chebyshev polynomial, with T_j(cos beta)=cos(j beta). Grover's normalized-overlap calculation uses T_(2k+1)(a)=(-1)^k sin((2k+1)arcsin(a)) for a in[0,1], where ar…

primary source nl only

test_public · proof

Exercise PLAN-518

Keep the original setting N=2^n, a unique marked input and classical worst-case query count, including the unbiased-algorithm assumption. Assess/refute the predecessor's claim that success greater than1/2 on every input …

primary source nl only

test_public · proof

Exercise PLAN-519

The marking information for search is first given as a bit oracle that adds the function value into an answer qubit modulo two. Prove that running this bit oracle with the answer qubit prepared in the minus state convert…

primary source nl only

test_public · proof

Exercise PLAN-520

Keep the original assumption of a small positive initial success probability p for a state psi=U|0> and an orthogonal good projector Π, and keep the original query-level cost convention. Assess/refute the predecessor's a…

primary source nl only