Search results for "ADIABATIC PASSAGE"

showing 10 items of 28 documents

Roadmap on STIRAP applications

2019

STIRAP (stimulated Raman adiabatic passage) is a powerful laser-based method, usually involving two photons, for efficient and selective transfer of populations between quantum states. A particularly interesting feature is the fact that the coupling between the initial and the final quantum states is via an intermediate state, even though the lifetime of the latter can be much shorter than the interaction time with the laser radiation. Nevertheless, spontaneous emission from the intermediate state is prevented by quantum interference. Maintaining the coherence between the initial and final state throughout the transfer process is crucial. STIRAP was initially developed with applications in …

PhotonAtomic Physics (physics.atom-ph)Digital storageStimulated Raman adiabatic passage02 engineering and technologyStimulated Raman adiabatic passage (STIRAP)01 natural scienceslaw.inventionPhysics - Atomic PhysicsFTIR SPECTROSCOPYstimulated Raman adiabatic passage (STIRAP)lawStereochemistryRare earthsStatistical physicsMetal ionsmolecular Rydberg statesQCparity violationPhysicseducation.field_of_studyQuantum PhysicsElectric dipole momentsCoherent population transfer021001 nanoscience & nanotechnologyCondensed Matter Physicsacoustic waves; molecular Rydberg states; nuclear coherent population transfer; parity violation; spin waves; stimulated Raman adiabatic passage (STIRAP); ultracold moleculesADIABATIC PASSAGEAtomic and Molecular Physics and OpticsChemical DynamicsMolecular beamsVIOLATING ENERGY DIFFERENCEResearch group A. Pálffy – Division C. H. KeitelStimulated emission0210 nano-technologyCoherence (physics)Experimental parametersPopulationFOS: Physical sciencesacoustic waves530spin wavesMolecular Rydberg statesELECTROMAGNETICALLY INDUCED TRANSPARENCYSINGLE PHOTONSQuantum statePhysics - Chemical Physics0103 physical sciencesUltracold moleculesSpontaneous emissionddc:530Nuclear coherent population transfer010306 general physicseducationStimulated Raman adiabatic passageChemical Physics (physics.chem-ph)Rare-earth-ion doped crystalsPhotonsQuantum opticsnuclear coherent population transferBROAD-BANDControlled manipulationsPOLAR-MOLECULESMoleculesRydberg statesLaserSuperconducting quantum circuitAcoustic wavesParity violationstimulated Raman adiabatic passage (STIRAP); ultracold molecules; parity violation; spin waves; acoustic waves; molecular Rydberg states; nuclear coherent population transferDewey Decimal Classification::500 | Naturwissenschaften::530 | Physikultracold moleculesQuantum Physics (quant-ph)QUANTUM GASSpin waves
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Topology of adiabatic passage

2002

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. Moreover, using this picture, we display new related possibilities of transfer. In particular, we show that we can selectively control the level that will be populated in STIRAP process in $\ensuremath{\Lambda}$ or V systems by the choice of the peak amplitudes or …

Physicseducation.field_of_studyPopulationStimulated Raman adiabatic passagePulse sequenceLambdaAdiabatic quantum computationTopologyAtomic and Molecular Physics and OpticsAmplitudeQuantum mechanicsPhysics::Atomic and Molecular ClustersAdiabatic processeducationTopology (chemistry)Physical Review A
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Two-laser multiphoton adiabatic passage in the frame of the Floquet theory. Applications to (1+1) and (2+1) STIRAP

1998

We develop an adiabatic two-mode Floquet theory to analyse multiphoton coherent population transfer in N-level systems by two delayed laser pulses, which is a generalization of the three-state stimulated Raman adiabatic passage (STIRAP). The main point is that, under conditions of non-crossing and adiabaticity, the outcome and feasibility of a STIRAP process can be determined by the analysis of two features: (i) the lifting of degeneracy of dressed states at the beginning and at the end of the laser pulses, and (ii) the connectivity of these degeneracy-lifted branches in the quasienergy diagram. Both features can be determined by stationnary perturbation theory in the Floquet representation…

Floquet theoryPhysicsStimulated Raman adiabatic passageOptical physicsAtomic and Molecular Physics and Opticssymbols.namesakeStark effectQuantum mechanicssymbolsRotating wave approximationPhysics::Atomic PhysicsPerturbation theoryDegeneracy (mathematics)Adiabatic processThe European Physical Journal D
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Rovibrational controlled-NOT gates using optimized stimulated Raman adiabatic passage techniques and optimal control theory

2009

Implementation of quantum controlled-NOT (CNOT) gates in realistic molecular systems is studied using stimulated Raman adiabatic passage (STIRAP) techniques optimized in the time domain by genetic algorithms or coupled with optimal control theory. In the first case, with an adiabatic solution (a series of STIRAP processes) as starting point, we optimize in the time domain different parameters of the pulses to obtain a high fidelity in two realistic cases under consideration. A two-qubit CNOT gate constructed from different assignments in rovibrational states is considered in diatomic (NaCs) or polyatomic $({\text{SCCl}}_{2})$ molecules. The difficulty of encoding logical states in pure rota…

Physics010304 chemical physicsField (physics)Stimulated Raman adiabatic passageRotational–vibrational spectroscopyOptimal control01 natural sciencesAtomic and Molecular Physics and OpticsControlled NOT gateQuantum mechanics0103 physical sciencesPhysics::Atomic and Molecular ClustersTime domain010306 general physicsAdiabatic processQuantum computerPhysical Review A
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Arbitrary qudit gates by adiabatic passage

2013

We derive an adiabatic technique that implements the most general SU($d$) transformation in a quantum system of $d$ degenerate states, featuring a qudit. This technique is based on the factorization of the SU($d$) transformation into $d$ generalized quantum Householder reflections, each of which is implemented by a two-shot stimulated Raman adiabatic passage with appropriate static phases. The energy of the lasers needed to synthesize a single Householder reflection is shown to be remarkably constant as a function of $d$. This technique is directly applicable to a linear trapped ion system with $d+1$ ions. We implement the quantum Fourier transform numerically in a qudit with $d=4$ (defined…

PhysicsHouseholder transformationQuantum mechanicsDegenerate energy levelsQuantum systemStimulated Raman adiabatic passageQuantum Fourier transformAdiabatic processQuantumAtomic and Molecular Physics and OpticsQuantum computerPhysical Review A
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Design of a Lambda system for population transfer in superconducting nanocircuits

2013

The implementation of a Lambda scheme in superconducting artificial atoms could allow detec- tion of stimulated Raman adiabatic passage (STIRAP) and other quantum manipulations in the microwave regime. However symmetries which on one hand protect the system against decoherence, yield selection rules which may cancel coupling to the pump external drive. The tradeoff between efficient coupling and decoherence due to broad-band colored Noise (BBCN), which is often the main source of decoherence is addressed, in the class of nanodevices based on the Cooper pair box (CPB) design. We study transfer efficiency by STIRAP, showing that substantial efficiency is achieved for off-symmetric bias only i…

Quantum decoherenceStimulated Raman adiabatic passageFOS: Physical sciencesSINGLE COOPER PAIR ADIABATIC PASSAGE QUANTUM STATES FLUX QUBIT SPECTROSCOPY MOLECULES CIRCUIT ATOMS NOISE BOX01 natural sciencesNoise (electronics)Settore FIS/03 - Fisica Della Materia010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)Quantum mechanics0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)010306 general physicsQuantumQuantum computerPhysicsCouplingQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed Matter - SuperconductivityCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsColors of noiseCooper pairQuantum Physics (quant-ph)
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Connection between optimal control theory and adiabatic-passage techniques in quantum systems

2012

This work explores the relationship between optimal control theory and adiabatic passage techniques in quantum systems. The study is based on a geometric analysis of the Hamiltonian dynamics constructed from the Pontryagin Maximum Principle. In a three-level quantum system, we show that the Stimulated Raman Adiabatic Passage technique can be associated to a peculiar Hamiltonian singularity. One deduces that the adiabatic pulse is solution of the optimal control problem only for a specific cost functional. This analysis is extended to the case of a four-level quantum system.

DYNAMICSN-LEVEL SYSTEMSStimulated Raman adiabatic passageFOS: Physical sciences01 natural sciencesPULSE SEQUENCES010305 fluids & plasmasOpen quantum systemDESIGNQuantum mechanicsPhysics - Chemical Physics0103 physical sciences010306 general physicsAdiabatic processPhysicsChemical Physics (physics.chem-ph)Quantum PhysicsALGORITHMSAdiabatic quantum computationAtomic and Molecular Physics and OpticsNMRClassical mechanicsGeometric phaseAdiabatic invariantPOPULATION TRANSFERQuantum algorithmSTIRAPQuantum Physics (quant-ph)Hamiltonian (control theory)
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INFLUENCE OF UNEQUAL OSCILLATOR STRENGTHS ON STIMULATED RAMAN ADIABATIC PASSAGE THROUGH BRIGHT STATE

2012

In the present work an analytical and numerical analysis of the b -STIRAP process in a medium with unequal oscillator strengths is performed. It is shown that the length of population transfer can be considerably increased by an appropriate choice of the dipole transitions.

Work (thermodynamics)DipoleChemistryOscillator strengthNumerical analysisStimulated Raman adiabatic passagePopulation transferAtomic physicsBright stateInternational Journal of Modern Physics: Conference Series
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Ultrafast stimulated Raman parallel adiabatic passage by shaped pulses

2009

We present a general and versatile technique of population transfer based on {\it parallel adiabatic passage} by femtosecond shaped pulses. Their amplitude and phase are specifically designed to optimize the adiabatic passage corresponding to parallel eigenvalues at all times. We show that this technique allows the robust adiabatic population transfer in a Raman system with the total pulse area as low as 3 $\pi$, corresponding to a fluence of one order of magnitude below the conventional stimulated Raman adiabatic passage process. This process of short duration, typically pico- and subpicosecond, is easily implementable with the modern pulse shaper technology and opens the possibility of ul…

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Stimulated Raman adiabatic passageFOS: Physical sciences01 natural sciences010309 opticssymbols.namesakeOptics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical sciences010306 general physicsAdiabatic process[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]ComputingMilieux_MISCELLANEOUSPhysicsQuantum Physicsbusiness.industryAtomic and Molecular Physics and OpticsPulse (physics)PicosecondFemtosecondsymbolsAtomic physicsQuantum Physics (quant-ph)businessRaman spectroscopyUltrashort pulseRaman scattering
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Generation of entanglement in systems of intercoupled qubits

2014

We consider systems of two and three qubits, mutually coupled by Heisenberg-type exchange interaction and interacting with external laser fields. We show that these systems allow one to create maximally entangled Bell states, as well as three qubit Greenberger-Horne-Zeilinger and W states. In particular, we point out that some of the target states are the eigenstates of the initial bare system. Due to this, one can create entangled states by means of pulse area and adiabatic techniques, when starting from a separable (non-entangled) ground state. On the other hand, for target states, not present initially in the eigensystem of the model, we apply the robust stimulated Raman adiabatic passag…

PhysicsQuantum PhysicsBell stateStimulated Raman adiabatic passageFOS: Physical sciencesQuantum PhysicsQuantum entanglement01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmasPulse (physics)Separable spaceQuantum mechanicsQubit0103 physical sciencesW stateQuantum Physics (quant-ph)010306 general physicsAdiabatic processPhysical Review A
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