1998
DOI: 10.1103/physrevlett.80.2027
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Optical Confinement of a Bose-Einstein Condensate

Abstract: Bose-Einstein condensates of sodium atoms have been confined in an optical dipole trap using a single focused infrared laser beam. This eliminates the restrictions of magnetic traps for further studies of atom lasers and Bose-Einstein condensates. More than five million condensed atoms were transferred into the optical trap. Densities of up to $3 \times 10^{15} cm^{-3}$ of Bose condensed atoms were obtained, allowing for a measurement of the three-body decay rate constant for sodium condensates as $K_3 = (1.1 … Show more

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Cited by 1,069 publications
(1,060 citation statements)
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“…In oblate traps with ω z ≫ ω ⊥ , however, the spin-gauge effect can be significant (Ω s could be comparable with ω ⊥ for large enough values of ω z ). Recently, the MIT group has succeeded in trapping a 23 Na Bose condensate by purely optical means [158,159]. In contrast to a magnetic trap, the spins of the alkali atoms in such an optical trap are essentially free, so that the spinor nature of the alkali Bose condensate can be fully realized.…”
Section: A Basic Phenomenamentioning
confidence: 99%
“…In oblate traps with ω z ≫ ω ⊥ , however, the spin-gauge effect can be significant (Ω s could be comparable with ω ⊥ for large enough values of ω z ). Recently, the MIT group has succeeded in trapping a 23 Na Bose condensate by purely optical means [158,159]. In contrast to a magnetic trap, the spins of the alkali atoms in such an optical trap are essentially free, so that the spinor nature of the alkali Bose condensate can be fully realized.…”
Section: A Basic Phenomenamentioning
confidence: 99%
“…In contrast, a far-off-resonant optical trap confines atoms regardless of their hyperfine state [44]. Thus, the atomic spin is liberated from the requirements of magnetic trapping and becomes a new degree of freedom.…”
Section: Spinor Bose-einstein Condensatesmentioning
confidence: 99%
“…First, magnetically-trapped Bose-Einstein condensates were produced in the |F = 1, m F = −1 hyperfine state and transferred to an optical trap [44]. Then, we pulsed on rf fields of variable strength which were swept in frequency to distribute the optically-trapped atoms among the F = 1 hyperfine sublevels by the method of adiabatic rapid passage [106].…”
Section: Experimental Methods For the Study Of Spinor Condensatesmentioning
confidence: 99%
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