6533b7d4fe1ef96bd1263390

RESEARCH PRODUCT

Production and detection of atomic hexadecapole at Earth's magnetic field

James M. HigbieSimon M. RochesterDmitry BudkerVictor M. AcostaD. F. Jackson KimballPjotrs GrišinsWojciech GawlikL. KrzemienMarcis AuzinshValeriy V. YashchukSzymon PustelnyMicah P. Ledbetter

subject

Angular momentumLightEarth PlanetMagnetometerAtomic Physics (physics.atom-ph)TransducersPopulationFOS: Physical sciencesRadiation Dosagelaw.inventionPhysics - Atomic PhysicsMagneticssymbols.namesakelawPhysical Sciences and MathematicsScattering RadiationComputer SimulationPhysics::Atomic PhysicsRadiometryAnisotropyeducationPhysicseducation.field_of_studyZeeman effectEquipment DesignModels TheoreticalPolarization (waves)Atomic and Molecular Physics and OpticsAtomic clockMagnetic fieldEquipment Failure AnalysisBudker [BRII recipient]symbolsComputer-Aided DesignAtomic physicsEnvironmental Monitoring

description

Anisotropy of atomic states is characterized by population differences and coherences between Zeeman sublevels. It can be efficiently created and probed via resonant interactions with light, the technique which is at the heart of modern atomic clocks and magnetometers. Recently, nonlinear magneto-optical techniques have been developed for selective production and detection of higher polarization moments, hexadecapole and hexacontatetrapole, in the ground states of the alkali atoms. Extension of these techniques into the range of geomagnetic fields is important for practical applications. This is because hexadecapole polarization corresponding to the $\Delta M=4$ Zeeman coherence, with maximum possible $\Delta M$ for electronic angular momentum $J=1/2$ and nuclear spin $I=3/2$, is insensitive to the nonlinear Zeeman effect (NLZ). This is of particular interest because NLZ normally leads to resonance splitting and systematic errors in atomic magnetometers. However, optical signals due to the hexadecapole moment decline sharply as a function of magnetic field. We report a novel method that allows selective creation of a macroscopic long-lived ground-state hexadecapole polarization. The immunity of the hexadecapole signal to NLZ is demonstrated with F=2 $^{87}$Rb atoms at Earth's field.

10.1364/oe.16.011423http://arxiv.org/abs/0709.4283