Abstract:Laser-cooled neutral atoms from a low-velocity atomic source are guided via a magnetic field generated between two parallel wires on a glass substrate. The atoms bend around three curves, each with a 15-cm radius of curvature, while traveling along a 10-cm-long track. A maximum flux of 2 · 10 6 atoms/sec is achieved with a current density of 3 · 10 4 A/cm 2 in the 100 × 100-µm-cross-section wires. The kinetic energy of the guided atoms in one transverse dimension is measured to be 42 µK. PACS numbers: 03.75.B,… Show more
“…By accounting for gravity, atomic fountains can increase the interrogation time during which the interferometry phase shifts accumulate [2]; alternatively one can use magnetic dipole forces to balance the force of gravity [3]. Magnetic waveguides [4,5] can trap atoms for times longer than a second, suggesting the possibility of measuring energy differences between interfering wave packets with an uncertainty <h/(1 s) ∼ 10 −34 J; however, this remarkable precision cannot be obtained if the decoherence time of the atoms is much shorter than the trap lifetime. Early atom interferometry experiments using atoms confined in magnetic waveguides showed that the external state coherence of the atoms decayed quite quickly, limiting interferometric measurements to times <10 ms [6,7].…”
A standing-wave light-pulse sequence is demonstrated that places atoms into a superposition of wave packets with precisely controlled displacements that remain constant for times as long as 1 s. The separated wave packets are subsequently recombined, resulting in atom interference patterns that probe energy differences of ≈10 −34 J and can provide acceleration measurements that are insensitive to platform vibrations.
“…By accounting for gravity, atomic fountains can increase the interrogation time during which the interferometry phase shifts accumulate [2]; alternatively one can use magnetic dipole forces to balance the force of gravity [3]. Magnetic waveguides [4,5] can trap atoms for times longer than a second, suggesting the possibility of measuring energy differences between interfering wave packets with an uncertainty <h/(1 s) ∼ 10 −34 J; however, this remarkable precision cannot be obtained if the decoherence time of the atoms is much shorter than the trap lifetime. Early atom interferometry experiments using atoms confined in magnetic waveguides showed that the external state coherence of the atoms decayed quite quickly, limiting interferometric measurements to times <10 ms [6,7].…”
A standing-wave light-pulse sequence is demonstrated that places atoms into a superposition of wave packets with precisely controlled displacements that remain constant for times as long as 1 s. The separated wave packets are subsequently recombined, resulting in atom interference patterns that probe energy differences of ≈10 −34 J and can provide acceleration measurements that are insensitive to platform vibrations.
“…It is now known that this "Fermi-Bose duality" is a very general property of identical particles in 1D, not restricted to the hard-sphere model, and relating strongly interacting bosons to weakly-interacting fermions and vice versa. In recent years this esoteric subject has become highly relevant through experiments on ultracold atomic vapors in atom waveguides [3][4][5][6][7][8][9][10][11]. An understanding of their properties is important for atom interferometry [12,13] and integrated atom optics [11,14,15], which are potentially important for development of ultrasensitive detectors of accelerations and gravitational anomalies.…”
Derivation of effective zero-range one-dimensional (1D) interactions between atoms in tight waveguides is reviewed, as is the Fermi-Bose mapping method for determination of exact and stronglycorrelated many-body ground states of ultracold bosonic and fermionic atomic vapors in such waveguides, including spin degrees of freedom. Odd-wave 1D interactions derived from 3D p-wave scattering are included as well as the usual even-wave interactions derived from 3D s-wave scattering, with emphasis on the role of 3D Feshbach resonances for selectively enhancing s-wave or p-wave scattering so as to reach 1D confinement-induced resonances of the even and odd-wave interactions. A duality between 1D fermions and bosons with zero-range interactions suggested by Cheon and Shigehara is shown to hold for the effective 1D dynamics of a spinor Fermi gas with both even and odd-wave interactions and that of a spinor Bose gas with even and odd-wave interactions, with even(odd)-wave Bose coupling constants inversely related to odd(even)-wave Fermi coupling constants. Some recent applications of Fermi-Bose mapping to determination of many-body ground states of Bose gases and of both magnetically trapped, spin-aligned and optically trapped, spin-free Fermi gases are described, and a new generalized Fermi-Bose mapping is used to determine the phase diagram of ground-state total spin of the spinor Fermi gas as a function of its even and odd-wave coupling constants.
“…Since the first realization of magnetic traps [1,2] and guides [3,4] with current-carrying conductors on a chip, a large variety of magnetic potentials have become experimentally accessible, which would be impractical or even impossible to realize with macroscopic coils. The splitting of two-dimensionally trapped atom clouds has been demonstrated [5,6], and recently, we were able to split and unite a three-dimensionally trapped cloud of rubidium atoms in a chip trap [7].…”
We propose a configuration of a magnetic microtrap which can be used as an interferometer for three-dimensionally trapped atoms. The interferometer is realized via a dynamic splitting potential that transforms from a single well into two separate wells and back. The ports of the interferometer are neighboring vibrational states in the single well potential. We present a one-dimensional model of this interferometer and compute the probability of unwanted vibrational excitations for a realistic magnetic potential. We optimize the speed of the splitting process in order suppress these excitations and conclude that such interferometer device should be feasible with currently available microtrap technique. 03.75.-b, 03.65.-w, 39.20.+q, 39.25.+k, 39.90.+d
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