Search results for "Larmor precession"

showing 10 items of 26 documents

Systematic and statistical uncertainties of the hilbert-transform based high-precision FID frequency extraction method.

2021

Abstract Pulsed nuclear magnetic resonance (NMR) is widely used in high-precision magnetic field measurements. The absolute value of the magnetic field is determined from the precession frequency of nuclear magnetic moments. The Hilbert transform is one of the methods that have been used to extract the phase function from the observed free induction decay (FID) signal and then its frequency. In this paper, a detailed implementation of a Hilbert-transform based FID frequency extraction method is described, and it is briefly compared with other commonly used frequency extraction methods. How artifacts and noise level in the FID signal affect the extracted phase function are derived analytical…

010302 applied physicsLarmor precessionPhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and Detectors010308 nuclear & particles physicsNoise (signal processing)Covariance matrixMathematical analysisBiophysicsFOS: Physical sciencesAbsolute valueInstrumentation and Detectors (physics.ins-det)Condensed Matter Physics01 natural sciencesBiochemistrySignalFree induction decaysymbols.namesake0103 physical sciencessymbolsHilbert transformUncertainty analysisJournal of magnetic resonance (San Diego, Calif. : 1997)
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A Precessing Ferromagnetic Needle Magnetometer

2016

A ferromagnetic needle is predicted to precess about the magnetic field axis at a Larmor frequency $\Omega$ under conditions where its intrinsic spin dominates over its rotational angular momentum, $N\hbar \gg I\Omega$ ($I$ is the moment of inertia of the needle about the precession axis and $N$ is the number of polarized spins in the needle). In this regime the needle behaves as a gyroscope with spin $N\hbar$ maintained along the easy axis of the needle by the crystalline and shape anisotropy. A precessing ferromagnetic needle is a correlated system of $N$ spins which can be used to measure magnetic fields for long times. In principle, by taking advantage of rapid averaging of quantum unce…

Angular momentumMagnetometerPhysics::Medical PhysicsFOS: Physical sciencesGeneral Physics and Astronomy02 engineering and technology01 natural scienceslaw.inventionComputer Science::RoboticslawMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciences010306 general physicsSpin (physics)PhysicsLarmor precessionQuantum PhysicsCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsMoment of inertia021001 nanoscience & nanotechnologyMagnetic fieldMagnetic anisotropyPhysics::Space PhysicsPrecessionQuantum Physics (quant-ph)0210 nano-technology
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Ferromagnetic gyroscopes for tests of fundamental physics

2020

A ferromagnetic gyroscope (FG) is a ferromagnet whose angular momentum is dominated by electron spin polarization and that will precess under the action of an external torque, such as that due to a magnetic field. Here we model and analyze FG dynamics and sensitivity, focusing on practical schemes for experimental realization. In the case of a freely floating FG, we model the transition from dynamics dominated by libration in relatively high externally applied magnetic fields, to those dominated by precession at relatively low applied fields. Measurement of the libration frequency enables in situ measurement of the magnetic field and a technique to reduce the field below the threshold for w…

Angular momentumgyroscopePhysics and Astronomy (miscellaneous)Field (physics)Atomic Physics (physics.atom-ph)Materials Science (miscellaneous)physics beyond the standard modelFOS: Physical sciencesApplied Physics (physics.app-ph)01 natural sciences530Physics - Atomic Physics010305 fluids & plasmasMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesLibrationddc:530Electrical and Electronic Engineering010306 general physicsLarmor precessionSuperconductivityPhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsMeissner effectFerromagnetism gyroscope physics beyond the standard model Meissner effectPhysics - Applied PhysicsferromagnetismAtomic and Molecular Physics and OpticsMagnetic fieldMeissner effectFerromagnetismPrecessionQuantum Physics (quant-ph)
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Experimental benchmarking of quantum control in zero-field nuclear magnetic resonance

2017

Zero-field nuclear magnetic resonance (NMR) provides complementary analysis modalities to those of high-field NMR and allows for ultra-high-resolution spectroscopy and measurement of untruncated spin-spin interactions. Unlike for the high-field case, however, universal quantum control -- the ability to perform arbitrary unitary operations -- has not been experimentally demonstrated in zero-field NMR. This is because the Larmor frequency for all spins is identically zero at zero field, making it challenging to individually address different spin species. We realize a composite-pulse technique for arbitrary independent rotations of $^1$H and $^{13}$C spins in a two-spin system. Quantum-inform…

Atomic Physics (physics.atom-ph)FOS: Physical sciencesQuantum simulator02 engineering and technology01 natural sciencesPhysics - Atomic PhysicsNuclear magnetic resonanceControlled NOT gatePhysics - Chemical Physics0103 physical sciencesQuantum metrology010306 general physicsSpin (physics)Chemical Physics (physics.chem-ph)Larmor precessionPhysicsQuantum PhysicsMultidisciplinarySpins500Nuclear magnetic resonance spectroscopy021001 nanoscience & nanotechnologyCondensed Matter::Strongly Correlated Electronsddc:500Quantum Physics (quant-ph)0210 nano-technologyRealization (systems)
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Polarization-driven spin precession of mesospheric sodium atoms

2018

We report experimental results on the first on-sky observation of atomic spin precession of mesospheric sodium driven by polarization modulation of a continuous-wave laser. The magnetic resonance was remotely detected from the ground by observing the enhancement of induced fluorescence when the driving frequency approached the precession frequency of sodium in the mesosphere, between 85 km and 100 km altitude. The experiment was performed at La Palma, and the uncertainty in the measured Larmor frequency ($\approx$260 kHz) corresponded to an error in the geomagnetic field of 0.4 mG. The results are consistent with geomagnetic field models and with the theory of light-atom interaction in the …

Atomic Physics (physics.atom-ph)Sodiumchemistry.chemical_elementFOS: Physical sciences7. Clean energy01 natural scienceslaw.inventionPhysics::GeophysicsPhysics - Atomic Physics010309 opticsOpticslaw0103 physical sciencesPhysics::Atomic Physics010306 general physicsSpin (physics)Circular polarizationLarmor precessionPhysicsbusiness.industryLaserPolarization (waves)Atomic and Molecular Physics and OpticsMagnetic fieldEarth's magnetic fieldchemistryPhysics::Space PhysicsAstrophysics::Earth and Planetary AstrophysicsAtomic physicsbusiness
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Motion of an electric charge in a terrestrial laboratory.

1995

The equation of motion for a charge in an electromagnetic field is written in the Fermi coordinates of an observer moving with a constant acceleration g=9.8 m/${\mathrm{s}}^{2}$ (${10}^{\mathrm{\ensuremath{-}}18}$ ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$ in units such that c=1). This is involved in the equation of motion not only as a Newtonian term g\ensuremath{\rightarrow}, but also as a relativistic correction of the form ``-2(g\ensuremath{\rightarrow}\ensuremath{\cdot}v\ensuremath{\rightarrow})v\ensuremath{\rightarrow}.'' We have studied the effect of this term under the conditions of an accelerator of particles. To this end, we have considered a constant and uniform magnetic field, a…

Electromagnetic fieldPhysicsLarmor precessionParticle physicsElectric fieldEquations of motionFermi coordinatesCharge (physics)Atomic physicsElectric chargeMagnetic fieldPhysical review. D, Particles and fields
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Optimal control of the inversion of two spins in Nuclear Magnetic Resonance

2012

International audience; We investigate the optimal control of the inversion of two spin 1/2 particles in Nuclear Magnetic Resonance. The two spins, which differ by their resonance offset, are controlled by the same radio frequency magnetic field. Using the Pontryagin Maximum Principle, we compute the optimal control sequence which allows to reach the target state in a given time, while minimizing the energy of the magnetic field. A comparison with the time-optimal solution for bounded control amplitude realizing the same control in the same time is made. An experimental illustration is done using techniques of Nuclear Magnetic Resonance.

Larmor precessionPhysics010304 chemical physicsSpinsPulsed EPRGeneral Physics and AstronomyBROAD-BAND EXCITATIONOptimal control01 natural sciencesNMRMagnetic fieldPULSESFree induction decayNuclear magnetic resonance2-LEVEL QUANTUM-SYSTEMSBloch equationsOPTIMAL-CONTROL DESIGN0103 physical sciencesRadio frequencyPhysical and Theoretical Chemistry010306 general physicsPOPULATION
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Measurement of the Permanent Electric Dipole Moment of the $^{129}$Xe Atom

2019

We report on a measurement of the $CP$-violating permanent electric dipole moment (EDM) of the neutral $^{129}\mathrm{Xe}$ atom. Our experimental approach is based on the detection of the free precession of co-located nuclear spin-polarized $^{3}\mathrm{He}$ and $^{129}\mathrm{Xe}$ samples. The EDM measurement sensitivity benefits strongly from long spin coherence times of several hours achieved in diluted gases and homogeneous weak magnetic fields of about 400 nT. A finite EDM is indicated by a change in the precession frequency, as an electric field is periodically reversed with respect to the magnetic guiding field. Our result $(\ensuremath{-}4.7\ifmmode\pm\else\textpm\fi{}6.4)\ifmmode\t…

Larmor precessionPhysicsField (physics)Atomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciences010305 fluids & plasmasMagnetic fieldPhysics - Atomic PhysicsElectric dipole momentElectric field0103 physical sciencesAtomddc:530Sensitivity (control systems)Atomic physics010306 general physicsSpin (physics)
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Probing Lorentz invariance and other fundamental symmetries in3He/129Xe clock-comparison experiments

2011

We discuss the design and performance of a very sensitive low-field magnetometer based on the detection of free spin precession of gaseous, nuclear polarized 3He or 129Xe samples with a SQUID as magnetic flux detector. Characteristic spin precession times T*2 of up to 60 h were measured in low magnetic fields (about 1μT) and in the regime of motional narrowing. With the detection of the free precession of co-located 3He/129Xe nuclear spins (clock comparison), the device can be used as ultra-sensitive probe for non-magnetic spin interactions, since the magnetic dipole interaction (Zeeman-term) drops out in the weighted frequency difference, i.e., Δω = ωHe− γHe/γXe·ωXe. We report on searches …

Larmor precessionPhysicsHistorySpin polarizationLorentz covarianceComputer Science ApplicationsEducationMagnetic fieldThomas precessionClassical mechanicsQuantum electrodynamicsPrecessionSpin (physics)Magnetic dipoleJournal of Physics: Conference Series
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Spin dynamics in the single-ion magnet [Er(W5O18)2]9−

2018

In this work we present a detailed NMR and ${\ensuremath{\mu}}^{+}\mathrm{SR}$ investigation of the spin dynamics in the new hydrated sodium salt containing the single-ion magnet ${[\mathrm{Er}{({\mathrm{W}}_{5}{\mathrm{O}}_{18})}_{2}]}^{9\ensuremath{-}}$. The $^{1}\mathrm{H}\phantom{\rule{0.16em}{0ex}}\mathrm{NMR}$ absorption spectra at various applied magnetic fields present a line broadening on decreasing temperature which indicates a progressive spin freezing of the single-molecule magnetic moments. The onset of quasistatic local magnetic fields, due to spin freezing, is observed also in the muon relaxation curves at low temperature. Both techniques yield a local field distribution of t…

Larmor precessionPhysicsMuonMagnetic momentMagnetism02 engineering and technologyMuon spin spectroscopy021001 nanoscience & nanotechnology01 natural sciencesDipolesymbols.namesake0103 physical sciencessymbolsAtomic physics010306 general physics0210 nano-technologyHamiltonian (quantum mechanics)Local fieldPhysical Review B
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