Search results for "quant-ph"

showing 10 items of 1378 documents

Revealing Hidden Quantum Correlations in an Electromechanical Measurement.

2018

Under a strong quantum measurement, the motion of an oscillator is disturbed by the measurement back-action, as required by the Heisenberg uncertainty principle. When a mechanical oscillator is continuously monitored via an electromagnetic cavity, as in a cavity optomechanical measurement, the back-action is manifest by the shot noise of incoming photons that becomes imprinted onto the motion of the oscillator. Following the photons leaving the cavity, the correlations appear as squeezing of quantum noise in the emitted field. Here we observe such "ponderomotive" squeezing in the microwave domain using an electromechanical device made out of a superconducting resonator and a drumhead mechan…

PhotonUncertainty principleField (physics)General Physics and AstronomyFOS: Physical sciencesPhysics::Optics01 natural sciences010305 fluids & plasmasResonatorElectromagnetic cavity0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)kvanttimekaniikka010306 general physicsQuantumPhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale Physicsta114quantum measurementsQuantum noiseShot noisesqueezing of quantum noiseoptomechanicsoptiset laitteetQuantum electrodynamicsQuantum Physics (quant-ph)Physical review letters
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Bounds on mixed state entanglement

2020

In the general framework of d 1 &times

Physical systemFOS: Physical sciencesGeneral Physics and Astronomylcsh:AstrophysicsQuantum entanglementCharacterization (mathematics)01 natural sciencesArticle010305 fluids & plasmas[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical scienceslcsh:QB460-466negativityStatistical physics010306 general physicslcsh:ScienceQuantumThermal entanglementPhysicsQuantum PhysicsState (functional analysis)lcsh:QC1-999Bipartite graphComputer Science::Programming Languageslcsh:QQuantum Physics (quant-ph)entanglementlcsh:PhysicsCurse of dimensionality
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Entanglement transfer, accumulation and retrieval via quantum-walk-based qubit-qudit dynamics

2020

The generation and control of quantum correlations in high-dimensional systems is a major challenge in the present landscape of quantum technologies. Achieving such non-classical high-dimensional resources will potentially unlock enhanced capabilities for quantum cryptography, communication and computation. We propose a protocol that is able to attain entangled states of $d$-dimensional systems through a quantum-walk-based {\it transfer \& accumulate} mechanism involving coin and walker degrees of freedom. The choice of investigating quantum walks is motivated by their generality and versatility, complemented by their successful implementation in several physical systems. Hence, given t…

Physical systemGeneral Physics and AstronomyFOS: Physical sciencesQuantum entanglementPhysics and Astronomy(all)Topology01 natural sciences010305 fluids & plasmasquantum information/dk/atira/pure/subjectarea/asjc/31000103 physical sciencesquantum walksQuantum walkentanglement accumulationQuantum information010306 general physicsQuantumPhysicsQuantum Physicsentanglement accumulation; entanglement transfer; high-dimensional entanglement; quantum walksTheoryofComputation_GENERALentanglement transferQuantum technologyQuantum cryptographyQubitentanglement transfer; entanglement accumulation; high-dimensional entanglement; quantum walksQuantum Physics (quant-ph)entanglementhigh-dimensional entanglement
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Demonstration of diamond nuclear spin gyroscope

2021

Description

Physics - Instrumentation and DetectorsFOS: Physical sciencesengineering.materiallaw.inventionlawMesoscale and Nanoscale Physics (cond-mat.mes-hall)Physical and Materials SciencesApplied PhysicsPhysicsQuantum PhysicsMultidisciplinarySpinsCondensed Matter - Mesoscale and Nanoscale PhysicsRotation sensorbusiness.industryPhysicsDiamond500SciAdv r-articlesGyroscopeOptical polarizationInstrumentation and Detectors (physics.ins-det)engineeringOptoelectronicsddc:500businessQuantum Physics (quant-ph)Research ArticleScience Advances
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Miniature Cavity-Enhanced Diamond Magnetometer

2017

We present a highly sensitive miniaturized cavity-enhanced room-temperature magnetic-field sensor based on nitrogen-vacancy (NV) centers in diamond. The magnetic resonance signal is detected by probing absorption on the 1042\,nm spin-singlet transition. To improve the absorptive signal the diamond is placed in an optical resonator. The device has a magnetic-field sensitivity of 28 pT/$\sqrt{\rm{Hz}}$, a projected photon shot-noise-limited sensitivity of 22 pT/$\sqrt{\rm{Hz}}$ and an estimated quantum projection-noise-limited sensitivity of 0.43 pT/$\sqrt{\rm{Hz}}$ with the sensing volume of $\sim$ 390 $\mu$m $\times$ 4500 $\mu$m$^{2}$. The presented miniaturized device is the basis for an e…

Physics - Instrumentation and DetectorsPhotonMaterials scienceMagnetometerGeneral Physics and AstronomyFOS: Physical sciences02 engineering and technologyengineering.material01 natural sciencesSignallaw.inventionlaw0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)[ PHYS.PHYS.PHYS-GEN-PH ] Physics [physics]/Physics [physics]/General Physics [physics.gen-ph][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsAbsorption (electromagnetic radiation)[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Quantum PhysicsCondensed Matter - Mesoscale and Nanoscale Physicsbusiness.industryDiamondInstrumentation and Detectors (physics.ins-det)021001 nanoscience & nanotechnology[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Highly sensitiveOptical cavityengineeringOptoelectronics0210 nano-technologybusinessQuantum Physics (quant-ph)Sensitivity (electronics)
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Quantum sensitivity limits of nuclear magnetic resonance experiments searching for new fundamental physics

2021

Nuclear magnetic resonance is a promising experimental approach to search for ultra-light axion-like dark matter. Searches such as the cosmic axion spin-precession experiments (CASPEr) are ultimately limited by quantum-mechanical noise sources, in particular, spin-projection noise. We discuss how such fundamental limits can potentially be reached. We consider a circuit model of a magnetic resonance experiment and quantify three noise sources: spin-projection noise, thermal noise, and amplifier noise. Calculation of the total noise spectrum takes into account the modification of the circuit impedance by the presence of nuclear spins, as well as the circuit back-action on the spin ensemble. S…

Physics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Materials Science (miscellaneous)Dark matterFOS: Physical sciences01 natural sciencesNoise (electronics)010305 fluids & plasmasNuclear magnetic resonanceHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Sensitivity (control systems)Electrical and Electronic Engineering010306 general physicsAxionQuantumElectrical impedanceSpin-½PhysicsQuantum PhysicsSpinsInstrumentation and Detectors (physics.ins-det)Atomic and Molecular Physics and OpticsCondensed Matter - Other Condensed MatterHigh Energy Physics - PhenomenologyQuantum Physics (quant-ph)Other Condensed Matter (cond-mat.other)
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The cosmic axion spin precession experiment (CASPEr): a dark-matter search with nuclear magnetic resonance

2017

The Cosmic Axion Spin Precession Experiment (CASPEr) is a nuclear magnetic resonance experiment (NMR) seeking to detect axion and axion-like particles which could make up the dark matter present in the universe. We review the predicted couplings of axions and axion-like particles with baryonic matter that enable their detection via NMR. We then describe two measurement schemes being implemented in CASPEr. The first method, presented in the original CASPEr proposal, consists of a resonant search via continuous-wave NMR spectroscopy. This method offers the highest sensitivity for frequencies ranging from a few Hz to hundreds of MHz, corresponding to masses $ m_{\rm a} \sim 10^{-14}$--$10^{-6}…

Physics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsMagnetometerMaterials Science (miscellaneous)Dark matterFOS: Physical sciencesApplied Physics (physics.app-ph)7. Clean energy01 natural scienceslaw.inventionHigh Energy Physics - Phenomenology (hep-ph)Nuclear magnetic resonancelaw0103 physical sciencesElectrical and Electronic Engineering010306 general physicsAxionPhysicsQuantum PhysicsCOSMIC cancer database010308 nuclear & particles physicsBandwidth (signal processing)RangingInstrumentation and Detectors (physics.ins-det)Physics - Applied PhysicsNuclear magnetic resonance spectroscopyAtomic and Molecular Physics and OpticsBaryonHigh Energy Physics - PhenomenologyPhysics - Data Analysis Statistics and ProbabilityQuantum Physics (quant-ph)Data Analysis Statistics and Probability (physics.data-an)Quantum Science and Technology
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Foundations of quantum mechanics and their impact on contemporary society

2018

Nearing a century since its inception, quantum mechanics is as lively as ever. Its signature manifestations, such as superposition, wave-particle duality, uncertainty principle, entanglement and nonlocality, were long confronted as weird predictions of an incomplete theory, paradoxes only suitable for philosophical discussions, or mere mathematical artifacts with no counterpart in the physical reality. Nevertheless, decades of progress in the experimental verification and control of quantum systems have routinely proven detractors wrong. While fundamental questions still remain wide open on the foundations and interpretations of quantum mechanics, its modern technological applications have …

Physics - Physics and SocietyUncertainty principle010504 meteorology & atmospheric sciencesGeneral MathematicsPhysics - History and Philosophy of PhysicsGeneral Physics and AstronomyFOS: Physical sciencesQuantum entanglementPhysics and Society (physics.soc-ph)Quantum technologieQuantum mechanics01 natural sciencesSettore FIS/03 - Fisica Della Materia[SHS.HISPHILSO]Humanities and Social Sciences/History Philosophy and Sociology of SciencesQuantum nonlocalityQuantum mechanics0103 physical sciencesHistory and Philosophy of Physics (physics.hist-ph)SociologyContemporary society010306 general physicsQuantum0105 earth and related environmental sciencesQuantum PhysicsIntroductionQuantum foundationGeneral EngineeringInterpretations of quantum mechanics16. Peace & justicePhysics::History of PhysicsDuality (electricity and magnetism)Transformative learningQuantum Physics (quant-ph)[PHYS.PHYS.PHYS-HIST-PH]Physics [physics]/Physics [physics]/History of Physics [physics.hist-ph]
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Non-Markovian dynamics from band edge effects and static disorder

2017

It was recently shown [S. Lorenzo et al., Sci. Rep. 7, 42729 (2017)] that the presence of static disorder in a bosonic bath - whose normal modes thus become all Anderson-localised - leads to non-Markovianity in the emission of an atom weakly coupled to it (a process which in absence of disorder is fully Markovian). Here, we extend the above analysis beyond the weak-coupling regime for a finite-band bath so as to account for band edge effects. We study the interplay of these with static disorder in the emergence of non-Markovian behaviour in terms of a suitable non-Markovianity measure.

Physics and Astronomy (miscellaneous)Anderson localizactionMarkov processNon-MarkovianityFOS: Physical sciencesEdge (geometry)01 natural sciencesMeasure (mathematics)Static disorderCondensed Matter::Disordered Systems and Neural NetworksSettore FIS/03 - Fisica Della Materia010305 fluids & plasmassymbols.namesakeNormal modeQuantum mechanicsAtom (measure theory)0103 physical sciencesband edge mode010306 general physicsband edge modesPhysicsQuantum PhysicsDynamics (mechanics)disordersymbolsQuantum Physics (quant-ph)Anderson localizaction; band edge modes; disorder; Non-Markovianity; Physics and Astronomy (miscellaneous)
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Quantum non-Markovianity induced by Anderson localization

2017

As discovered by P. W. Anderson, excitations do not propagate freely in a disordered lattice, but, due to destructive interference, they localise. As a consequence when an atom interacts with a disordered lattice one indeed observes, a non-trivial excitation exchange between atom and lattice. Such non-trivial atomic dynamics will in general be characterised also by a non-trivial quantum information backflow, a clear signature of non-Markovian dynamics. To investigate the above scenario we consider a quantum emitter, or atom, weakly coupled to a uniform coupled-cavity array (CCA). If initially excited, in the absence of disorder, the emitter undergoes a Markovian spontaneous emission by rele…

Physics---Anderson localizationQuantum PhysicsMultidisciplinaryFOS: Physical sciences01 natural sciencesArticleSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasNormal modeExcited stateQuantum mechanics0103 physical sciencesPhenomenological modelAtomSpontaneous emissionQuantum information010306 general physicsQuantum Physics (quant-ph)QuantumScientific Reports
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