David R. Leibrandt
Massachusetts Institute of Technology
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Featured researches published by David R. Leibrandt.
Physical Review Letters | 2008
Jaroslaw Labaziewicz; Yufei Ge; Paul Antohi; David R. Leibrandt; Kenneth R. Brown; Isaac L. Chuang
Dense arrays of trapped ions provide one way of scaling up ion trap quantum information processing. However, miniaturization of ion traps is currently limited by sharply increasing motional state decoherence at sub-100 mum ion-electrode distances. We characterize heating rates in cryogenically cooled surface-electrode traps, with characteristic sizes in the 75 to 150 mum range. Upon cooling to 6 K, the measured rates are suppressed by 7 orders of magnitude, 2 orders of magnitude below previously published data of similarly sized traps operated at room temperature. The observed noise depends strongly on the fabrication process, which suggests further improvements are possible.
Physical Review A | 2006
C. E. Pearson; David R. Leibrandt; Waseem Bakr; W. J. Mallard; Kenneth R. Brown; Isaac L. Chuang
Chiaverini et al. [Quantum Inf. Comput. 5, 419 (2005)] recently suggested a linear Paul trap geometry for ion-trap quantum computation that places all of the electrodes in a plane. Such planar ion traps are compatible with modern semiconductor fabrication techniques and can be scaled to make compact, many-zone traps. In this paper we present an experimental realization of planar ion traps using electrodes on a printed circuit board to trap linear chains of tens of charged particles of
Physical Review Letters | 2008
Jaroslaw Labaziewicz; Yufei Ge; David R. Leibrandt; Shannon X. Wang; Ruth Shewmon; Isaac L. Chuang
0.44\phantom{\rule{0.3em}{0ex}}\mathrm{\ensuremath{\mu}}\mathrm{m}
Physical Review Letters | 2009
David R. Leibrandt; Jaroslaw Labaziewicz; Vladan Vuletic; Isaac L. Chuang
diameter in a vacuum of
The Astrophysical Journal | 2009
C. C. Kuranz; R. P. Drake; E. C. Harding; M.J. Grosskopf; H. F. Robey; B. A. Remington; M. J. Edwards; A. R. Miles; T. S. Perry; B.E. Blue; T. Plewa; Nathan Charles Hearn; J. P. Knauer; David Arnett; David R. Leibrandt
15\phantom{\rule{0.3em}{0ex}}\mathrm{Pa}\phantom{\rule{0.3em}{0ex}}({10}^{\ensuremath{-}1}\phantom{\rule{0.3em}{0ex}}\mathrm{torr})
Physical Review A | 2007
Kenneth R. Brown; Robert J. Clark; Jaroslaw Labaziewicz; Philip Richerme; David R. Leibrandt; Isaac L. Chuang
. With these traps we address concerns about the low trap depth of planar ion traps and develop control electrode layouts for moving ions between trap zones without facing some of the technical difficulties involved in an atomic ion-trap experiment. Specifically, we use a trap with 36 zones (77 electrodes) arranged in a cross to demonstrate loading from a traditional four-rod linear Paul trap, linear ion movement, splitting and joining of ion chains, and movement of ions through intersections. We further propose an additional dc-biased electrode above the trap which increases the trap depth dramatically, and a planar ion-trap geometry that generates a two-dimensional lattice of point Paul traps.
Physical Review A | 2013
David R. Leibrandt; James C. Bergquist; T. Rosenband
Electric field noise from fluctuating patch potentials is a significant problem for a broad range of precision experiments, including trapped ion quantum computation and single spin detection. Recent results demonstrated strong suppression of this noise by cryogenic cooling, suggesting an underlying thermal process. We present measurements characterizing the temperature and frequency dependence of the noise from 7 to 100 K, using a single Sr+ ion trapped 75 mum above the surface of a gold plated surface electrode ion trap. The noise amplitude is observed to have an approximate 1/f spectrum around 1 MHz, and grows rapidly with temperature as T;{beta} for beta from 2 to 4. The data are consistent with microfabricated cantilever measurements of noncontact friction but do not extrapolate to the dc measurements with neutral atoms or contact potential probes.
Nature | 2017
Chin-Wen Chou; Christoph Kurz; D. B. Hume; Philipp N. Plessow; David R. Leibrandt; D. Leibfried
We report a demonstration and quantitative characterization of one-dimensional cavity cooling of a single trapped (88)Sr(+) ion in the resolved-sideband regime. We measure the spectrum of cavity transitions, the rates of cavity heating and cooling, and the steady-state cooling limit. The cavity cooling dynamics and cooling limit of 22.5(3) motional quanta, limited by the moderate coupling between the ion and the cavity, are consistent with a simple model [Phys. Rev. A 64, 033405 (2001)] without any free parameters, validating the rate equation model for cavity cooling.
Physical Review Letters | 2011
Lukas Lamata; David R. Leibrandt; Isaac L. Chuang; J. Ignacio Cirac; Mikhail D. Lukin; Vladan Vuletic; Susanne F. Yelin
This paper shows results from experiments diagnosing the development of the Rayleigh-Taylor instability with two-dimensional initial conditions at an embedded, decelerating interface. Experiments are performed at the Omega Laser and use ~5 kJ of energy to create a planar blast wave in a dense, plastic layer that is followed by a lower density foam layer. The single-mode interface has a wavelength of 50 μm and amplitude of 2.5 μm. Some targets are supplemented with additional modes. The interface is shocked then decelerated by the foam layer. This initially produces the Richtmyer-Meshkov instability followed and then dominated by Rayleigh-Taylor growth that quickly evolves into the nonlinear regime. The experimental conditions are scaled to be hydrodynamically similar to SN1987A in order to study the instabilities that are believed to occur at the He/H interface during the blast-wave-driven explosion phase of the star. Simulations of the experiment were performed using the FLASH hydrodynamics code.
Physical Review Letters | 2015
Shon M. Cook; T. Rosenband; David R. Leibrandt
We demonstrate a method for loading surface electrode ion traps by electron impact ionization. The method relies on the property of surface electrode geometries that the trap depth can be increased at the cost of more micromotion. By introducing a buffer gas, we can counteract the rf heating assocated with the micromotion and benefit from the larger trap depth. After an initial loading of the trap, standard compensation techniques can be used to cancel the stray fields resulting from charged dielectric and allow for the loading of the trap at ultra-high vacuum.