2015
DOI: 10.1103/physics.8.72
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Towards an Atomtronic Diode

Abstract: We report on the observation of negative differential conductivity (NDC) in a quantum transport device for neutral atoms employing a multimode tunneling junction. The system is realized with a Bose-Einstein condensate loaded in a one-dimensional optical lattice with high site occupancy. We induce an initial difference in chemical potential at one site by local atom removal. The ensuing transport dynamics are governed by the interplay between the tunneling coupling, the interaction energy, and intrinsic collisi… Show more

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Cited by 6 publications
(5 citation statements)
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“…For future work, there is much room to optimize barrier shapes and scattering length to boost tunneling asymmetry in order to steer the dynamics of a BEC; this is a natural and direct extension of efforts to optimize scattering length to control transmission [26]. This approach may enable atomtronic diodes [50], facilitate BEC driven interferometers [51], and gravimetry [52]. The analytic treatment in section 5 suggests at least three strategies for obtaining large tunneling asymmetry already in the weak-interaction regime: (a) large tunneling asymmetry may naturally be obtained when a relatively small number of quantum states participate in the dynamics, (b) tunneling asymmetry is enhanced when the tunneling rate, potential asymmetry, and BEC interaction strength are all comparable, in appropriate units, and (c) tunneling asymmetry is enhanced for fast, repeated tunneling back and forth through a barrier as compared to a slow single pass.…”
Section: Discussionmentioning
confidence: 99%
“…For future work, there is much room to optimize barrier shapes and scattering length to boost tunneling asymmetry in order to steer the dynamics of a BEC; this is a natural and direct extension of efforts to optimize scattering length to control transmission [26]. This approach may enable atomtronic diodes [50], facilitate BEC driven interferometers [51], and gravimetry [52]. The analytic treatment in section 5 suggests at least three strategies for obtaining large tunneling asymmetry already in the weak-interaction regime: (a) large tunneling asymmetry may naturally be obtained when a relatively small number of quantum states participate in the dynamics, (b) tunneling asymmetry is enhanced when the tunneling rate, potential asymmetry, and BEC interaction strength are all comparable, in appropriate units, and (c) tunneling asymmetry is enhanced for fast, repeated tunneling back and forth through a barrier as compared to a slow single pass.…”
Section: Discussionmentioning
confidence: 99%
“…There is much room to optimize barrier shapes and scattering length to boost asymmetry to steer dynamics of BEC, which is a direct expansion upon efforts to optimize scattering length to control transmission [24]. This may enable atomtronic diodes [40] and facilitate BEC driven interferometers [41].…”
Section: Discussionmentioning
confidence: 99%
“…In the technique of atomtronics, atoms can be controlled and manipulated analogous to the operation in electronics [1][2][3][4][5][6][7][8][9]. One kind of devices in this field is atomic battery.…”
mentioning
confidence: 99%