Abstract:We address quantum spatial search on graphs and its implementation by continuous-time quantum walks in the presence of dynamical noise. In particular, we focus on search on the complete graph and on the star graph of order N, also proving that noiseless spatial search shows optimal quantum speedup in the latter, in the computational limit N 1. The noise is modeled by independent sources of random telegraph noise (RTN), dynamically perturbing the links of the graph. We observe two different behaviors depending … Show more
“…with (H s C N ) 0 = I, the probability of finding the target node is found to be p w (t) = | w|e −iHt |s | 2 = 1 N cos 2 t N . Recently, the same quadratic speedup has been proved also for the star graph [33], i.e. a graph where only a central node is connected to all the other (N − 1) nodes.…”
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confidence: 53%
“…By properly manipulating the expression of the Hamiltonian and after using perturbation theory [33], one obtains that the initial state |s evolves into the state |w + O(N −1/2 ) after a time t opt = T . This indicates that for very large values of N the algorithm is optimal even for external target nodes.…”
We address continuous-time quantum walks on graphs in the presence of time-and space-dependent noise. Noise is modeled as generalized dynamical percolation, i.e. classical timedependent fluctuations affecting the tunneling amplitudes of the walker. In order to illustrate the general features of the model, we review recent results on two paradigmatic examples: the dynamics of quantum walks on the line and the effects of noise on the performances of quantum spatial search on the complete and the star graph. We also discuss future perspectives, including extension to many-particle quantum walk, to noise model for on-site energies and to the analysis of different noise spectra. Finally, we address the use of quantum walks as a quantum probe to characterize defects and perturbations occurring in complex, classical and quantum, networks.
“…with (H s C N ) 0 = I, the probability of finding the target node is found to be p w (t) = | w|e −iHt |s | 2 = 1 N cos 2 t N . Recently, the same quadratic speedup has been proved also for the star graph [33], i.e. a graph where only a central node is connected to all the other (N − 1) nodes.…”
mentioning
confidence: 53%
“…By properly manipulating the expression of the Hamiltonian and after using perturbation theory [33], one obtains that the initial state |s evolves into the state |w + O(N −1/2 ) after a time t opt = T . This indicates that for very large values of N the algorithm is optimal even for external target nodes.…”
We address continuous-time quantum walks on graphs in the presence of time-and space-dependent noise. Noise is modeled as generalized dynamical percolation, i.e. classical timedependent fluctuations affecting the tunneling amplitudes of the walker. In order to illustrate the general features of the model, we review recent results on two paradigmatic examples: the dynamics of quantum walks on the line and the effects of noise on the performances of quantum spatial search on the complete and the star graph. We also discuss future perspectives, including extension to many-particle quantum walk, to noise model for on-site energies and to the analysis of different noise spectra. Finally, we address the use of quantum walks as a quantum probe to characterize defects and perturbations occurring in complex, classical and quantum, networks.
“…Grover's algorithm has proven to be equivalent to a continuous-time quantum walk on a complete network [26]. In addition, a speed-up by continuous-time quantum walks on a star network has also been found [27], and this has encouraged further study of continuous-time quantum walks on regular networks. Here, a network is said to be regular if it has a repeating pattern in its network topology.…”
Section: Introductionmentioning
confidence: 99%
“…Unlike a classical random walker, the propagation of the quantum walker is coherent, i.e., besides the randomness inherited from quantum-mechanical probability amplitudes the coherence between different sites also governs the system dynamics [21]. The study of continuoustime quantum walks is mathematically based on network theory [22][23][24] and is closely related to other fields in quantum information theory, e.g., universal quantum computation [25], quantum algorithms [26][27][28], and perfect state transfer [29]. A continuous-time quantum walk can be experimentally implemented, usually by such quantum optical systems as waveguides [30] or Rydberg atoms [31].…”
Non-Markovianity may significantly speed up quantum dynamics when the system interacts strongly with an infinite large reservoir, of which the coupling spectrum should be fine-tuned. The potential benefits are evident in many dynamics schemes, especially the continuous-time quantum walk. Difficulty exists, however, in producing closed-form solutions with controllable accuracy against the complexity of memory kernels. Here, we introduce a new multiple-scale perturbation method that works on integro-differential equations for general study of memory effects in dynamical systems. We propose an open-system model in which a continuous-time quantum walk is enclosed in a non-Markovian reservoir, that naturally corresponds to an error correction algorithm scheme. By applying the multiple-scale method we show how emergence of different timescales is related to transition of system dynamics into the non-Markovian regime. We find that up to two long-term modes and two short-term modes exist in regular networks, limited by their intrinsic symmetries. In addition to the effective approximation by our perturbation method on general forms of reservoirs, the speed-up of quantum walks assisted by non-Markovianity is also confirmed, revealing the advantage of reservoir engineering in designing time-sensitive quantum algorithms.
“…In these systems, the graph Laplacian L (also referred to as the Kirchhoff matrix of the graph) plays the role of the free Hamiltonian, i.e., it corresponds to the kinetic energy of the particle. Perturbations to ideal CTQWs have been investigated earlier [4][5][6][7][8][9][10][11][12], however with the main focus being on the decoherence effects of stochastic noise rather than the quantum effects induced by a perturbing Hamiltonian. A notable exception exists, though, given by the quantum spatial search, where the perturbation induced by the so-called oracle Hamiltonian has been largely investigated as a tool to induce localization on a desired site [13][14][15][16][17][18].…”
We address the properties of continuous-time quantum walks with Hamiltonians of the form H = L + λL 2 , with L the Laplacian matrix of the underlying graph and the perturbation λL 2 motivated by its potential use to introduce next-nearest-neighbor hopping. We consider cycle, complete, and star graphs as paradigmatic models with low and high connectivity and/or symmetry. First, we investigate the dynamics of an initially localized walker. Then we devote attention to estimating the perturbation parameter λ using only a snapshot of the walker dynamics. Our analysis shows that a walker on a cycle graph spreads ballistically independently of the perturbation, whereas on complete and star graphs one observes perturbation-dependent revivals and strong localization phenomena. Concerning the estimation of the perturbation, we determine the walker preparations and the simple graphs that maximize the quantum Fisher information. We also assess the performance of position measurement, which turns out to be optimal, or nearly optimal, in several situations of interest. Besides fundamental interest, our study may find applications in designing enhanced algorithms on graphs.
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