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Quantum Physics (quant-ph)

Fri, 02 Jun 2023

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1.Numerical aspects of Casimir energy computation in acoustic scattering

Authors:Xiaoshu Sun, Timo Betcke, Alexander Strohmaier

Abstract: Computing the Casimir force and energy between objects is a classical problem of quantum theory going back to the 1940s. Several different approaches have been developed in the literature often based on different physical principles. Most notably a representation of the Casimir energy in terms of determinants of boundary layer operators makes it accessible to a numerical approach. In this paper, we first give an overview of the various methods and discuss the connection to the Krein-spectral shift function and computational aspects. We propose variants of Krylov subspace methods for the computation of the Casimir energy for large-scale problems and demonstrate Casimir computations for several complex configurations. This allows for Casimir energy calculation for large-scale practical problems and significantly speeds up the computations in that case.

2.A low-crosstalk double-side addressing system using acousto-optic deflectors for atomic ion qubits

Authors:Rui-Rui Li, Yi-Long Chen, Ran He, Shu-Qian Chen, Wen-Hao Qi, Jin-Ming Cui, Yun-Feng Huang, Chuan-Feng Li, Guang-Can Guo

Abstract: The ability to individually and agilely manipulate qubits is crucial for the scalable trapped-ion quantum information processing. A plethora of challenging proposals have been demonstrated with the utilization of optical addressing systems, in which single ions is addressed exclusively by individual laser beam. However, crosstalk error in optical addressing systems limits the gate fidelity, becoming an obstacle to quantum computing, especially quantum error correction. In this work, we demonstrate a low-crosstalk double-side addressing system based on a pair of acousto-optic deflectors (AODs). The AODs addressing method can flexibly and parallelly address arbitrary ions between which the distance is variable in a chain. We employ two 0.4~NA objective lenses in both arms of the Raman laser and obtain a beam waist of 0.95~$\mu\mathrm{m}$, resulting in a Rabi rate crosstalk as low as $6.32\times10^{-4}$ when the neighboring ion separation is about 5.5~$\mu\mathrm{m}$. This agile and low-crosstalk double-side addressing system is promising for higher-fidelity gates and the practical application of the quantum error correction.

3.Revisiting weak values through non-normality

Authors:Lorena Ballesteros Ferraz, Riccardo Muolo, Yves Caudano, Timoteo Carletti

Abstract: Quantum measurement is one of the most fascinating and discussed phenomena in quantum physics, due to the impact on the system of the measurement action and the resulting interpretation issues. Scholars proposed weak measurements to amplify measured signals by exploiting a quantity called a weak value, but also to overcome philosophical difficulties related to the system perturbation induced by the measurement process. The method finds many applications and raises many philosophical questions as well, especially about the proper interpretation of the observations. In this paper, we show that any weak value can be expressed as the expectation value of a suitable non-normal operator. We propose a preliminary explanation of their anomalous and amplification behavior based on the theory of non-normal matrices and their link with non-normality: the weak value is different from an eigenvalue when the operator involved in the expectation value is non-normal. Our study paves the way for a deeper understanding of the measurement phenomenon, helps the design of experiments, and it is a call for collaboration to researchers in both fields to unravel new quantum phenomena induced by non-normality.

4.Entanglement and Teleportation in a 1-D Network with Repeaters

Authors:Ganesh Mylavarapu, Indranil Chakrabarty, Kaushiki Mukherjee, Minyi Huang, Junde Wu

Abstract: The most simplest form of quantum network is an one dimensional quantum network with a single player in each node. In remote entanglement distribution each of the players carry out measurement at the intermediate nodes to produce an entangled state between initial and final node which are remotely separated. It is imperative to say that the flow of information as well as the percolation of entanglement in a network between the source and target node is an important area of study. This will help us to understand the limits of the resource states as well as the measurements that are carried out in the process of remote entanglement distribution. In this article we investigate how the concurrence of the final entangled state obtained is connected with the concurrences of the initial entangled states present in a 1-D chain. We extend the works done for the pure entangled states for mixed entangled states like Werner states, Bell diagonal states and for general mixed states. We did not limit ourselves to a situation where the measurements are happening perfectly. We also investigate how these relations change when we consider imperfect swapping. We obtain the limits on the number of swappings as well as the success probability measurements to ensure the final state to be entangled state after swapping. In addition to these we also investigate on how much quantum information can be sent from the initial node to the final node (by computing the teleportation fidelity) when the measurement is perfect and imperfect with the same set of examples. Here also we obtain the limits on the number of swapping and the success probability of measurement to ensure that the final state obtained is capable of transferring the information . These results have tremendous future applications in sending quantum information between two quantum processors in remote entangled distribution.

5.Topological methods for studying contextuality: $N$-cycle scenarios and beyond

Authors:Aziz Kharoof, Selman Ipek, Cihan Okay

Abstract: Simplicial distributions are combinatorial models describing distributions on spaces of measurements and outcomes that generalize non-signaling distributions on contextuality scenarios. This paper studies simplicial distributions on $2$-dimensional measurement spaces by introducing new topological methods. Two key ingredients are a geometric interpretation of Fourier--Motzkin elimination and a technique based on collapsing of measurement spaces. Using the first one, we provide a new proof of Fine's theorem characterizing non-contextual distributions on $N$-cycle scenarios. Our approach goes beyond these scenarios and can describe non-contextual distributions on scenarios obtained by gluing cycle scenarios of various sizes. The second technique is used for detecting contextual vertices and deriving new Bell inequalities. Combined with these methods, we explore a monoid structure on simplicial distributions.

6.Interaction induced phase transition in quantum many-body detection probability

Authors:Archak Purkayastha, Alberto Imparato

Abstract: We introduce and explore the physics of quantum many-body detection probability (QMBDP). Imagine a quantum many-body system starting from a far-from-equilibrium initial state. Few detectors are put at some given positions of the system. The detectors make simultaneous stroboscopic projective measurements of some chosen local operators. A particular measurement outcome is taken as the `signal'. By QMBDP we refer to the probability that the signal is detected within a given time. We find that, due to repeated stroboscopic measurements, there can emerge a time-scale within which the signal is almost certainly detected. Depending on the spectral properties of the Hamiltonian, there can be a phase transition where this time-scale increases dramatically on tuning some Hamiltonian parameters across the transition point. Consequently, over a finite but large regime of time, depending on the initial state, tuning some Hamiltonian parameters can result in sharp transition from a phase where the signal is certainly detected (QMBDP $=1$) to a phase where the the signal may not be detected (QMBDP $<1$). As an example, we present a single-impurity non-integrable model where such a far-from-equilibrium transition is achieved by varying the many-body interaction strength.

7.Quantum spectral analysis by continuous measurement of Landau-Zener transitions

Authors:Christopher C. Bounds School of Physics and Astronomy, Monash University, Melbourne, Australia, Josh P. Duff School of Physics and Astronomy, Monash University, Melbourne, Australia, Alex Tritt School of Physics and Astronomy, Monash University, Melbourne, Australia, Hamish Taylor School of Physics and Astronomy, Monash University, Melbourne, Australia, George X. Coe School of Physics and Astronomy, Monash University, Melbourne, Australia, Sam J. White School of Physics and Astronomy, Monash University, Melbourne, Australia, Lincoln D. Turner School of Physics and Astronomy, Monash University, Melbourne, Australia

Abstract: We demonstrate the simultaneous estimation of signal frequency and amplitude by a single ensemble qubit sensor under irreducibly time-dependent control. Sweeping the qubit splitting linearly across a span induces a non-adiabatic Landau-Zener transition as the qubit crosses resonance. The signal frequency determines the time of the transition, and the amplitude its extent. Continuous weak measurement of this unitary evolution informs a parameter estimator retrieving precision measurements of frequency and amplitude. Implemented on radiofrequency-dressed ultracold atoms read out by a Faraday spin-light interface, we sense a magnetic signal with $\unit[20]{pT}$ precision in amplitude, and near-transform-limited precision in frequency, in a single $\unit[300]{ms}$ sweep from $\unit[7-13]{kHz}$. The protocol realises a swept-sine quantum spectrum analyzer, potentially sensing hundreds or thousands of channels with a single ensemble qubit.

8.Reduction of finite sampling noise in quantum neural networks

Authors:David Kreplin, Marco Roth

Abstract: Quantum neural networks (QNNs) use parameterized quantum circuits with data-dependent inputs and generate outputs through the evaluation of expectation values. Calculating these expectation values necessitates repeated circuit evaluations, thus introducing fundamental finite-sampling noise even on error-free quantum computers. We reduce this noise by introducing the variance regularization, a technique for reducing the variance of the expectation value during the quantum model training. This technique requires no additional circuit evaluations if the QNN is properly constructed. Our empirical findings demonstrate the reduced variance speeds up the training and lowers the output noise as well as decreases the number of measurements in the gradient circuit evaluation. This regularization method is benchmarked on the regression of multiple functions. We show that in our examples, it lowers the variance by an order of magnitude on average and leads to a significantly reduced noise level of the QNN. We finally demonstrate QNN training on a real quantum device and evaluate the impact of error mitigation. Here, the optimization is practical only due to the reduced number shots in the gradient evaluation resulting from the reduced variance.

9.Nonadiabatic nuclear-electron dynamics: a quantum computing approach

Authors:Arseny Kovyrshin, Mårten Skogh, Lars Tornberg, Anders Broo, Stefano Mensa, Emre Sahin, Benjamin C. B. Symons, Jason Crain, Ivano Tavernelli

Abstract: The combined quantum electron-nuclear dynamics is often associated with the Born-Huang expansion of the molecular wave function and the appearance of nonadiabatic effects as a perturbation. On the other hand, native multicomponent representations of electrons and nuclei also exist, which do not rely on any a priori approximation. However, their implementation is hampered by prohibitive scaling costs and therefore quantum computers offer a unique opportunity for extending their use to larger systems. Here, we propose a quantum algorithm for the simulation of the time-evolution of molecular systems in the second quantization framework, which is applied to the simulation of the proton transfer dynamics in malonaldehyde. After partitioning the dynamics into slow and fast components, we show how the entanglement between the electronic and nuclear degrees of freedom can persist over long times if electrons are not adiabatically following the nuclear displacement. The proposed quantum algorithm may become a valid candidate for the study of electron-nuclear quantum phenomena when sufficiently powerful quantum computers become available.

10.Multichromatic Floquet engineering of quantum dissipation

Authors:François Impens, David Guéry-Odelin

Abstract: The monochromatic driving of a quantum system is a successful technique in quantum simulations, well captured by an effective Hamiltonian approach, and with applications in artificial gauge fields and topological engineering. In this letter, we investigate the modeling of multichromatic Floquet driving for the slow degrees of freedom. Within a well-defined range of parameters, we show that the time coarse-grained dynamics of such a driven closed quantum system is encapsulated in an effective Master equation for the time-averaged density matrix, that evolves under the action of an effective Hamiltonian and tunable Lindblad-type dissipation/quantum gain terms. As an application, we emulate the dissipation induced by phase noise and incoherent emission/absorption processes in the bichromatic driving of a two-level system.

11.Efficient Quantum State Synthesis with One Query

Authors:Gregory Rosenthal

Abstract: We present a polynomial-time quantum algorithm making a single query (in superposition) to a classical oracle, such that for every state $|\psi\rangle$ there exists a choice of oracle that makes the algorithm construct an exponentially close approximation of $|\psi\rangle$. Previous algorithms for this problem either used a linear number of queries and polynomial time [arXiv:1607.05256], or a constant number of queries and polynomially many ancillae but no nontrivial bound on the runtime [arXiv:2111.02999]. As corollaries we do the following: - We simplify the proof that statePSPACE $\subseteq$ stateQIP [arXiv:2108.07192] (a quantum state analogue of PSPACE $\subseteq$ IP) and show that a constant number of rounds of interaction suffices. - We show that QAC$\mathsf{_f^0}$ lower bounds for constructing explicit states would imply breakthrough circuit lower bounds for computing explicit boolean functions. - We prove that every $n$-qubit state can be constructed to within 0.01 error by an $O(2^n/n)$-size circuit over an appropriate finite gate set. More generally we give a size-error tradeoff which, by a counting argument, is optimal for any finite gate set.

12.Fast quantum state preparation and bath dynamics using non-Gaussian variational ansatz and quantum optimal control

Authors:Liam J. Bond, Arghavan Safavi-Naini, Jiří Minář

Abstract: We combine quantum optimal control with a variational ansatz based on non-Gaussian states for fast, non-adiabatic preparation of quantum many-body states. We demonstrate this on the example of the spin-boson model, and use a multi-polaron ansatz to prepare near-critical ground states. For one mode, we achieve a reduction in infidelity of up to $\approx 60$ ($\approx 20$) times compared to linear (optimised local adiabatic) ramps respectively; for many modes we achieve a reduction in infidelity of up to $\approx 5$ times compared to non-adiabatic linear ramps. Further, we show that the typical control quantity, the leakage from the variational manifold, provides only a loose bound on the state's fidelity. Instead, in analogy to the bond dimension of matrix product states, we suggest a controlled convergence criterion based on the number of polarons. Finally, motivated by the possibility of realizations in trapped ions, we study the dynamics of a system with bath properties going beyond the paradigm of (sub/super) Ohmic couplings. We apply the ansatz to the study of the out-of-time-order-correlator (OTOC) of the bath modes in a non-perturbative regime. The scrambling time is found to be a robust feature only weakly dependent on the details of the coupling between the bath and the spin.