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T-junction ion trap array for two-dimensional ion shuttling, storage, and manipulation

dc.contributor.authorHensinger, W. K.en_US
dc.contributor.authorOlmschenk, Steven Matthewen_US
dc.contributor.authorStick, Daniel Lynnen_US
dc.contributor.authorHucul, D.en_US
dc.contributor.authorYeo, M.en_US
dc.contributor.authorActon, Marken_US
dc.contributor.authorDeslauriers, L.en_US
dc.contributor.authorMonroe, C.en_US
dc.contributor.authorRabchuk, J. A.en_US
dc.date.accessioned2011-11-15T16:08:38Z
dc.date.available2011-11-15T16:08:38Z
dc.date.issued2006-01-16en_US
dc.identifier.citationHensinger, W. K.; Olmschenk, S.; Stick, D.; Hucul, D.; Yeo, M.; Acton, M.; Deslauriers, L.; Monroe, C.; Rabchuk, J. (2006). "T-junction ion trap array for two-dimensional ion shuttling, storage, and manipulation." Applied Physics Letters 88(3): 034101-034101-3. <http://hdl.handle.net/2027.42/87785>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/87785
dc.description.abstractWe demonstrate a two-dimensional 11-zone ion trap array, where individual laser-cooled atomic ions are stored, separated, shuttled, and swapped. The trap geometry consists of two linear rf-ion trap sections that are joined at a 90° angle to form a T-shaped structure. We shuttle a single ion around the corners of the T-junction and swap the positions of two crystallized ions using voltage sequences designed to accommodate the nontrivial electrical potential near the junction. Full two-dimensional control of multiple ions demonstrated in this system may be crucial for the realization of scalable ion trap quantum computation and the implementation of quantum networks.en_US
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleT-junction ion trap array for two-dimensional ion shuttling, storage, and manipulationen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumFOCUS Center and Department of Physics, University of Michigan, Ann Arbor, Michigan 48109en_US
dc.contributor.affiliationotherDepartment of Physics, Western Illinois University, Macomb, Illinois 61455en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/87785/2/034101_1.pdf
dc.identifier.doi10.1063/1.2164910en_US
dc.identifier.sourceApplied Physics Lettersen_US
dc.identifier.citedreferenceD. J. Wineland, C. Monroe, W. M. Itano, D. Leibfried, B. E. King, and D. M. Meekhof, J. Res. Natl. Inst. Stand. Technol. 103, 259 (1998).en_US
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dc.identifier.citedreferenceJ. Chiaverini, J. Britton, D. Leibfried, E. Knill, M. D. Barrett, R. B. Blakestad, W. M. Itano, J. D. Jost, C. Langer, R. Ozeri, T. Schaetz, and D. J. Wineland, Science 308, 997 (2005).en_US
dc.identifier.citedreferenceJ. Chiaverini, D. Leibfried, T. Schaetz, M. D. Barrett, R. B. Blakestad, J. Britton, W. M. Itano, J. D. Jost, E. Knill, C. Langer, R. Ozeri, and D. J. Wineland, Nature (London) 432, 602 (2004).en_US
dc.identifier.citedreferenceK. A. Brickman, P. C. Haljan, P. J. Lee, M. Acton, L. Deslauriers, and C. Monroe, Phys. Rev. A 72, 050306 (2005).en_US
dc.identifier.citedreferenceD. Kielpinski, C. Monroe, and D. J. Wineland, Nature (London) 417, 709 (2002).en_US
dc.identifier.citedreferenceA. M. Steane, quant-ph/0412165.en_US
dc.identifier.citedreferenceM. A. Rowe, A. Ben-Kish, B. DeMarco, D. Leibfried, V. Meyer, J. Beall, J. Britton, J. Hughes, W. M. Itano, B. Jelenkovic, C. Langer, T. Rosenband, and D. J. Wineland, Quantum Inf. Comput. 2, 257 (2002).en_US
dc.identifier.citedreferenceL. Deslauriers, P. C. Haljan, P. J. Lee, K.-A. Brickman, B. B. Blinov, M. J. Madsen, and C. Monroe, Phys. Rev. A 70, 043408 (2004).en_US
dc.identifier.citedreferenceJ. Chiaverini, R. B. Blakestad, J. Britton, J. D. Jost, C. Langer, D. Leibfried, R. Ozeri, and D. J. Wineland, Quantum Inf. Comput. 5, 419 (2005).en_US
dc.identifier.citedreferenceThe voltages are produced using analog output cards (National Instruments 6733), amplified using high-voltage operational-amplifier circuits (Apex, PA85A) and can be slewed over 10 V10V in about 1 μs1μs.en_US
dc.identifier.citedreferenceIt is not necessary to simulate the ion dynamics using quantum evolution as the typical action of motion is much larger than Planck’s constant, see, e.g., W. K. Hensinger, N. R. Heckenberg, G. J. Milburn, and H. Rubinsztein-Dunlop, J. Opt. B: Quantum Semiclassical Opt. 5, R83 (2003).en_US
dc.identifier.citedreferenceBackground heating rates during shuttling operations are neglected here, as they are expected to act on a much slower timescale; however, spectral noise densities for shallow traps (that may occur during shuttling) are expected to be larger, with concomitant heating rates. Future studies will address these issues.en_US
dc.identifier.citedreferenceAsymmetries between left- and right-turn voltage sequences are observed and may be attributed to static bias fields or known misalignments of the three electrode layers resulting from the manual trap assembly.en_US
dc.identifier.citedreferenceJ. P. Home and A. M. Steane, quant-ph/0411102.en_US
dc.owningcollnamePhysics, Department of


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