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Stimulated Raman adiabatic passage in a three-level superconducting circuit  [PDF]
K. S. Kumar,A. Vepsalainen,S. Danilin,G. S. Paraoanu
Physics , 2015,
Abstract: The adiabatic manipulation of quantum states is a powerful technique that has opened up new directions in quantum engineering, enabling tests of fundamental concepts such as the Berry phase and its nonabelian generalization, the observation of topological transitions, and holds the promise of alternative models of quantum computation. Here we benchmark the stimulated Raman adiabatic passage process for circuit quantum electrodynamics, by using the first three levels of a transmon qubit. We demonstrate a population transfer efficiency above 80% between the ground state and the second excited state using two adiabatic Gaussian-shaped control microwave pulses coupled to the first and second transition. The advantage of this techniques is robustness against errors in the timing of the control pulses. By doing quantum tomography at successive moments during the Raman pulses, we investigate the transfer of the population in time-domain. We also show that this protocol can be reversed by applying a third adiabatic pulse on the first transition. Furthermore, we demonstrate a hybrid adiabatic-nonadiabatic gate using a fast pulse followed by the adiabatic Raman sequence, and we study experimentally the case of a quasi-degenerate intermediate level.
Shortcut to adiabatic passage in two and three level atoms  [PDF]
Xi Chen,I. Lizuain,A. Ruschhaupt,D. Guery-Odelin,J. G. Muga
Physics , 2010, DOI: 10.1103/PhysRevLett.105.123003
Abstract: We propose a method to transfer the population and control the state of two-level and three-level atoms speeding-up Adiabatic Passage techniques while keeping their robustness versus parameter variations. The method is based on supplementing the standard laser beam setup of Adiabatic Passage methods with auxiliary steering laser pulses of orthogonal polarization. This provides a shortcut to adiabaticity driving the system along the adiabatic path defined by the standard setup.
Chaos assisted adiabatic passage  [PDF]
Kyungsun Na,L. E. Reichl
Physics , 2004, DOI: 10.1103/PhysRevA.70.063405
Abstract: We study the exact dynamics underlying stimulated Raman adiabatic passage (STIRAP) for a particle in a multi-level anharmonic system (the infinite square-well) driven by two sequential laser pulses, each with constant carrier frequency. In phase space regions where the laser pulses create chaos, the particle can be transferred coherently into energy states different from those predicted by traditional STIRAP. It appears that a transition to chaos can provide a new tool to control the outcome of STIRAP.
Adiabatic passage in the presence of noise  [PDF]
T. Noel,M. R. Dietrich,N. Kurz,G. Shu,J. Wright,B. B. Blinov
Physics , 2011, DOI: 10.1103/PhysRevA.85.023401
Abstract: We report on an experimental investigation of rapid adiabatic passage (RAP) in a trapped barium ion system. RAP is implemented on the transition from the $6S_{1/2}$ ground state to the metastable $5D_{5/2}$ level by applying a laser at 1.76 $\mu$m. We focus on the interplay of laser frequency noise and laser power in shaping the effectiveness of RAP, which is commonly assumed to be a robust tool for high efficiency population transfer. However, we note that reaching high state transfer fidelity requires a combination of small laser linewidth and large Rabi frequency.
Shortcut to Adiabatic Passage in a Waveguide Coupler with Allen-Eberly scheme  [PDF]
Koushik Paul,Amarendra K. Sarma
Physics , 2015, DOI: 10.1103/PhysRevA.91.053406
Abstract: We propose a directional coupler exploiting the framework of adiabatic passage for two level atomic systems with configuration dependent Allen-Eberly scheme. Recently developed shortcut to adiabatic passage method (STA), which uses transitionless quantum driving algorithm, is applied to the coupler. The study shows that it is possible to reduce the device length significantly using STA, keeping the efficiency of power transfer100%.Shortcut approach shows much superiority in terms of robustness and fidelity in power switching compared to the adiabatic one.
On the topology of adiabatic passage  [PDF]
L. P. Yatsenko,S Guerin,H. R. Jauslin
Physics , 2001, DOI: 10.1103/PhysRevA.65.043407
Abstract: We examine the topology of eigenenergy surfaces characterizing the population transfer processes based on adiabatic passage. We show that this topology is the essential feature for the analysis of the population transfers and the prediction of its final result. We reinterpret diverse known processes, such as stimulated Raman adiabatic passage (STIRAP), frequency-chirped adiabatic passage and Stark-chirped rapid adiabatic passage (SCRAP). Moreover, using this picture, we display new related possibilities of transfer. In particular, we show that we can selectively control the level which will be populated in STIRAP process in Lambda or V systems by the choice of the peak amplitudes or the pulse sequence.
Robustness of adiabatic quantum computation  [PDF]
Andrew M. Childs,Edward Farhi,John Preskill
Physics , 2001, DOI: 10.1103/PhysRevA.65.012322
Abstract: We study the fault tolerance of quantum computation by adiabatic evolution, a quantum algorithm for solving various combinatorial search problems. We describe an inherent robustness of adiabatic computation against two kinds of errors, unitary control errors and decoherence, and we study this robustness using numerical simulations of the algorithm.
Interferometry using spatial adiabatic passage in quantum dot networks  [PDF]
Lenneke M Jong,Andrew D. Greentree
Physics , 2009, DOI: 10.1103/PhysRevB.81.035311
Abstract: We show that techniques of spatial adiabatic passage can be used to realise an electron interferometer in a geometry analogous to a conventional Aharonov-Bohm ring, with transport of the particle through the device modulated using coherent transport adiabatic passage. This device shows an interesting interplay between the adiabatic and non-adiabatic behaviour of the system. The transition between non-adiabatic and adiabatic behaviour may be tuned via system parameters and the total time over which the protocol is enacted. Interference effects in the final state populations analogous to the electrostatic Aharonov-Bohm effect are observed.
Robustness of the adiabatic quantum search  [PDF]
Johan ?berg,David Kult,Erik Sj?qvist
Physics , 2004, DOI: 10.1103/PhysRevA.71.060312
Abstract: The robustness of the local adiabatic quantum search to decoherence in the instantaneous eigenbasis of the search Hamiltonian is examined. We demonstrate that the asymptotic time-complexity of the ideal closed case is preserved, as long as the Hamiltonian dynamics is present. In the special case of pure decoherence where the environment monitors the search Hamiltonian, it is shown that the local adiabatic quantum search performs as the classical search.
Optimum pulse shapes for stimulated Raman adiabatic passage  [PDF]
G. S. Vasilev,A. Kuhn,N. V. Vitanov
Physics , 2009,
Abstract: Stimulated Raman adiabatic passage (STIRAP), driven with pulses of optimum shape and delay has the potential of reaching fidelities high enough to make it suitable for fault-tolerant quantum information processing. The optimum pulse shapes are obtained upon reduction of STIRAP to effective two-state systems. We use the Dykhne-Davis-Pechukas (DDP) method to minimize nonadiabatic transitions and to maximize the fidelity of STIRAP. This results in a particular relation between the pulse shapes of the two fields driving the Raman process. The DDP-optimized version of STIRAP maintains its robustness against variations in the pulse intensities and durations, the single-photon detuning and possible losses from the intermediate state.
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