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Walk detection correctness and cost
Statement
Let be a finite symmetric lazy transition matrix on a nonempty finite set , with uniform stationary law. Fix real promise parameters and . When , suppose ; the marked-set promise is or . The finite algorithm input includes certified dyadic brackets for with ; the containment is an input promise and every endpoint bit and comparison cost is charged separately. Such brackets exist for every allowed real parameter. For , the promise parameters are unused. Write , , and . Give the algorithm the stated uniform-state circuit, a row-preparation access model for the absorbing chain , its controlled and inverse calls needed for the one-reflection walk, the marked check, and all their separate costs. Put
where the least-integer formulas are exactly the finite comparisons used by the algorithm. Then Szegedy-walk marked-set detection has no false positive on an empty marked set and outputs NONEMPTY with probability at least on every promised nonempty instance. For , let , where the terms are the supplied uniform-state and one row-preparation costs, an upper bound for the initial marked/unmarked Lüders test and its marked-branch label readout and verification, the cost of one controlled one-reflection walk call, and the phase-register preparation and inverse-QFT gate cost. Its worst-case charged quantum cost is at most
when only one-step controlled-walk access is supplied. The factorwise implementation of charges one controlled row-preparation inverse, one controlled row preparation, the controlled clean-state reflection, and the controlled swap. With separately supplied controlled powers, replace by the sum of their declared costs. The bracket ratios imply and , so the approved all-real parameter scope retains the same asymptotic resource bound. This is a detection result; a NONEMPTY phase-test outcome does not supply a marked label. Synthesis, endpoint bits, exact algebraic/rational comparisons, description bits and precision remain separate coordinates.
Facts & Assumptions
Given: The symmetric lazy chain and promise, the absorbing-row access and marked predicate in Szegedy-walk marked-set detection, and the QPE cutoff and repetition parameters above.
Spectral bound for a symmetric lazy walk killed on a marked set: is positive semidefinite and when the uniform chain has second eigenvalue at most and . The actual gap satisfies ; on a promised nonempty instance .
Discriminant of the marked-state absorbing walk: is row-stochastic and its Szegedy discriminant is .
Szegedy spectral mapping for one and two reflections: for the one-reflection walk , a discriminant eigenvalue gives walk eigenvalues ; at the corresponding row-space line has eigenvalue .
Phase-estimation nearest-grid and tail bounds: for and , QPE has probability at most of circular phase-estimation error at least .
Phase estimation on a superposition of eigenspaces: QPE outcome probabilities on an orthogonal eigenspace superposition are the mixture of the eigenphase outcome laws with the squared eigenspace norms as weights.
Exact phase recovery on the QPE grid: a zero phase is returned as outcome with certainty.
Phase-estimation query and gate costs: an -bit QPE from one controlled-step oracle makes exactly controlled-step calls; phase-register gates are charged separately.
Exact row-preparation access count for one and two walk steps: the factorwise controlled implementation of one charges one controlled inverse row preparation, one controlled forward row preparation, one controlled clean-state reflection, and one controlled swap.
Dirac Notation Conversion: orthogonal computational-basis labels define the finite register measurement and its projected outcome branches.
The Szegedy discriminant is self-adjoint and contractive: the transition-state map is an isometry, so distinct basis row states are orthogonal and each has norm one.
Circular phase distance modulo one: for , distance to zero is , equivalently the distance from to its nearest integer.
Finite projective measurements and Projective measurement outcome weights are probabilities give the projectors and their outcome probabilities. The algorithm explicitly supplies the Lüders instrument for the binary marked/unmarked projectors; The square-root Lüders maps form an instrument validates its branch maps, and Conditional state for a projective measurement identifies each positive-probability conditional state as the normalized projected state.
Signs, monotonicity intervals, and ranges of sine and cosine: cosine is strictly decreasing on .
Sine and cosine are -Lipschitz on : for , .
Proof
If , the supplied predicate is evaluated on the sole label and the procedure returns the exact answer. Assume henceforth . In the empty case , , and the prepared row state is , where . Symmetry of gives , so [F3] places it on the eigenline and its phase is exactly zero. The first marked check cannot accept, and [F6] makes QPE output , for which the strict cutoff fails. Thus neither branch falsely accepts.
In a nonempty instance write . The first-register check measures a uniformly distributed label; if it is marked, the algorithm accepts immediately, including the endpoint . Otherwise is nonempty and the conditional row state is , with . By [F10], each first-register outcome has squared norm under , and [F12] projects onto the sum of exactly the unmarked row vectors and normalizes it.
On , [F1] and the promises give . Hence its eigenvalues are at most and their one-reflection phases have circular distance from zero at least . The state lies in and is orthogonal to every marked row vector , , because those vectors have a distinct first-register label; the orthogonality also follows from the isometry [F10]. It therefore has no marked component and no component in . The decomposition [F2] and spectral mapping [F3] show that all its spectral components are the nonzero-phase signal components just bounded.
The choice of gives . By [F13], , and [F14] with and therefore gives , or . Also , so by [F13] and [F17]; [F14] gives . Thus the branch comparison in algorithm step 5 is exact: implies , while for both angles lie in and strict decrease of cosine makes equivalent to ; equality takes the rejected branch. Set . Then , so [F4] bounds the probability of a circular QPE error at least by . To justify the needed distance comparison from the definition [F11], take and . Choose nearest integers to , respectively, so and . Since , its distance to the nearest integer is at most its distance to the particular integer ; hence Thus . On every outcome with estimation error , step 2.1 gives Thus the algorithm accepts on that outcome. By [F5] the same failure bound holds for the whole conditional state, so a phase-test run accepts with probability at least . Including the initial marked-label branch can only raise its success probability.
Each fresh run therefore misses a promised nonempty set with probability at most . Independent fresh preparations make the probability that all runs miss at most by the definition of and the certified bracket. The empty case remains exact by step 1.1. The output relation only asserts the decision bit, since the phase-test branch measured no marked label.
For , a run makes one supplied uniform-state preparation, one row preparation, one initial marked check, one -bit QPE, and then at most controlled calls by [F7]. If each controlled walk is expanded factorwise, [F8] supplies its four separately charged calls. Multiplying this worst-case per-run sum by proves the cost upper bound; early stopping only reduces it. For , the exact branch uses only the sole-label predicate check. The named gate, query, synthesis, precision and bit coordinates are not combined, by the stated input accounting. To relate the finite parameters to the real promises, put . Then by [F15]–[F16], so . The least-power-of-two choice gives ; since , . Also , so .
Depends on
- Szegedy-walk marked-set detection
- Szegedy spectral mapping for one and two reflections
- Spectral bound for a symmetric lazy walk killed on a marked set
- Discriminant of the marked-state absorbing walk
- Phase-estimation nearest-grid and tail bounds
- Phase estimation on a superposition of eigenspaces
- Exact phase recovery on the QPE grid
- Phase-estimation query and gate costs
- Exact row-preparation access count for one and two walk steps
- Dirac Notation Conversion
- Circular phase distance modulo one
- Principal inverse sine and inverse cosine
- Signs, monotonicity intervals, and ranges of sine and cosine
- Quarter-turn values and shifts by pi/2 and pi
- Double-angle and quadratic power-reduction identities
- Sine and cosine are $1$-Lipschitz on $\mathbb{R}$
- The Szegedy discriminant is self-adjoint and contractive
- Finite projective measurements
- Projective measurement outcome weights are probabilities
- Finite POVMs and their outcome law
- Finite instruments and conditional states
- Non-negative and positive operators
- A non-negative operator has a unique non-negative square root
- The square-root Lüders maps form an instrument
- Conditional state for a projective measurement
Used by
Nothing in the library uses this result yet.
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Sources
- Andrew M. Childs, Lecture Notes on Quantum Algorithms, Chapter 18, §18.4 (standard reference, not scraped)
- Ronald de Wolf, Quantum Computing: Lecture Notes, Chapter 8, §§8.1–8.2 (standard reference, not scraped)
- Frédéric Magniez, Ashwin Nayak, Jérémie Roland, and Miklos Santha, Search via Quantum Walk, §§2–3 (standard reference, not scraped)