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The three geometries presented in this section for trapping neutral atoms and molecules using time-varying electric fields all have their magnetic counterpart. A cylindrically symmetric magnetic ac trap was proposed for spin-polarized atomic hydrogen atoms by Lovelace, and later demonstrated for cesium atoms by Cornell
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The three geometries presented in this section for trapping neutral atoms and molecules using time-varying electric fields all have their magnetic counterpart. A cylindrically symmetric magnetic ac trap was proposed for spin-polarized atomic hydrogen atoms by Lovelace, and later demonstrated for cesium atoms by Cornell.
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Alternatively, one may apply a positive voltage to two neighbouring electrodes while the other two electrodes are kept at a negative voltage.
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Alternatively, one may apply a positive voltage to two neighbouring electrodes while the other two electrodes are kept at a negative voltage.
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When ζ and ξ are chosen such that E =0 at the center of the trap, a hexapolar field results. An attempt to calculate F by using Eq. 2 fails due to the 1/E3 term. However, as the Stark effect of any molecule is quadratic in weak fields, we should use Eq. 3 instead. From Eq. 3 F=0 at the center of the trap. As both kx, ky and kz are equal to zero the trap volume is infinitely small.
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When ζ and ξ are chosen such that E =0 at the center of the trap, a hexapolar field results. An attempt to calculate F by using Eq. 2 fails due to the 1/E3 term. However, as the Stark effect of any molecule is quadratic in weak fields, we should use Eq. 3 instead. From Eq. 3 F=0 at the center of the trap. As both kx, ky and kz are equal to zero the trap volume is infinitely small.
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Again, one may also apply a positive voltage to two neighbouring electrodes while the two electrodes in the same plane are kept at a negative voltage and the remaining two electrodes are at ground.
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Again, one may also apply a positive voltage to two neighbouring electrodes while the two electrodes in the same plane are kept at a negative voltage and the remaining two electrodes are at ground.
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Even terms will cause the force to be nonzero at the center of the trap. Peik considered a small n =2 term to compensate the gravitational force on the atoms. In the case of polar molecules, the trap depth is so large that gravity can be neglected.
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Even terms will cause the force to be nonzero at the center of the trap. Peik considered a small n =2 term to compensate the gravitational force on the atoms. In the case of polar molecules, the trap depth is so large that gravity can be neglected.
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