73 results on '"Bradley Hauer"'
Search Results
52. Wavelength transduction from a 3D microwave cavity to telecom using piezoelectric optomechanical crystals
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Kartik Srinivasan, T. J. Clark, Krishna C. Balram, C. Doolin, John P. Davis, H. Ramp, and Bradley Hauer
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Materials science ,Physics and Astronomy (miscellaneous) ,FOS: Physical sciences ,Physics::Optics ,Applied Physics (physics.app-ph) ,02 engineering and technology ,Bristol Quantum Information Institute ,01 natural sciences ,Article ,Gallium arsenide ,chemistry.chemical_compound ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,0103 physical sciences ,Dilution refrigerator ,Optomechanics ,Microwave cavity ,010302 applied physics ,Quantum Physics ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Physics - Applied Physics ,021001 nanoscience & nanotechnology ,Piezoelectricity ,Transducer ,chemistry ,Qubit ,Quantum Physics (quant-ph) ,0210 nano-technology ,Telecommunications ,business ,Microwave ,Optics (physics.optics) ,Physics - Optics - Abstract
Microwave to optical transduction has received a great deal of interest from the cavity optomechanics community as a landmark application for electro-optomechanical systems. In this Letter, we demonstrate a novel transducer that combines high-frequency mechanical motion and a microwave cavity for the first time. The system consists of a 3D microwave cavity and a gallium arsenide optomechanical crystal, which has been placed in the microwave electric field maximum. This allows the microwave cavity to actuate the gigahertz-frequency mechanical breathing mode in the optomechanical crystal through the piezoelectric effect, which is then read out using a telecom optical mode. The gallium arsenide optomechanical crystal is a good candidate for low-noise microwave-to-telecom transduction, as it has been previously cooled to the mechanical ground state in a dilution refrigerator. Moreover, the 3D microwave cavity architecture can naturally be extended to couple to superconducting qubits and to create hybrid quantum systems.
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- 2020
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53. Phonon quantum nondemolition measurements in nonlinearly coupled optomechanical cavities
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A. Metelmann, John P. Davis, and Bradley Hauer
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Quantum decoherence ,Field (physics) ,Phonon ,FOS: Physical sciences ,Physics::Optics ,Quantum measurements ,01 natural sciences ,010305 fluids & plasmas ,Quantum mechanics ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,0103 physical sciences ,010306 general physics ,Quantum ,Optomechanics ,Quantum coherence & coherence measures ,Physics ,Quantum Physics ,Mesoscopic physics ,Condensed Matter - Mesoscale and Nanoscale Physics ,3. Good health ,Coupling (physics) ,Quantum-to-classical transition ,Quantum Physics (quant-ph) ,Wave function collapse ,Optics (physics.optics) ,Physics - Optics - Abstract
In the field of cavity optomechanics, proposals for quantum nondemolition (QND) measurements of phonon number provide a promising avenue by which one can study the quantum nature of nanoscale mechanical resonators. Here, we investigate these QND measurements for an optomechanical system whereby quadratic coupling arises due to shared symmetries between a single optical resonance and a mechanical mode. We establish a relaxed limit on the amount of linear coupling that can exist in this type of system while still allowing for a QND measurement of Fock states. This new condition enables optomechanical QND measurements, which can be used to probe the decoherence of mesoscopic mechanical Fock states, providing an experimental testbed for quantum collapse theories., 11 pages, 3 figures, submitted version
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- 2018
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54. Combining Neural and Non-Neural Methods for Low-Resource Morphological Reinflection
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Leyuan Yu, Grzegorz Kondrak, Saeed Kazemi Najafi, Rashed Rubby Riyadh, and Bradley Hauer
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Low resource ,business.industry ,Computer science ,Pattern recognition ,Artificial intelligence ,business - Published
- 2018
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55. Magnetic actuation and feedback cooling of a cavity optomechanical torque sensor
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Mark R. Freeman, P. H. Kim, T. J. Clark, Bradley Hauer, Fatemeh Fani Sani, and John P. Davis
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Science ,General Physics and Astronomy ,FOS: Physical sciences ,Physics::Optics ,02 engineering and technology ,Applied Physics (physics.app-ph) ,01 natural sciences ,General Biochemistry, Genetics and Molecular Biology ,Article ,Resonator ,0103 physical sciences ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,Torque sensor ,Torque ,Sensitivity (control systems) ,010306 general physics ,lcsh:Science ,Quantum ,Optomechanics ,Physics ,Mesoscopic physics ,Quantum Physics ,Multidisciplinary ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Response time ,General Chemistry ,Physics - Applied Physics ,021001 nanoscience & nanotechnology ,Optoelectronics ,lcsh:Q ,0210 nano-technology ,business ,Quantum Physics (quant-ph) - Abstract
Cavity optomechanics has demonstrated remarkable capabilities, such as measurement and control of mechanical motion at the quantum level. Yet many compelling applications of optomechanics—such as microwave-to-telecom wavelength conversion, quantum memories, materials studies, and sensing applications—require hybrid devices, where the optomechanical system is coupled to a separate, typically condensed matter, system. Here, we demonstrate such a hybrid optomechanical system, in which a mesoscopic ferromagnetic needle is integrated with an optomechanical torsional resonator. Using this system we quantitatively extract the magnetization of the needle, not known a priori, demonstrating the potential of this system for studies of nanomagnetism. Furthermore, we show that we can magnetically dampen its torsional mode from room-temperature to 11.6 K—improving its mechanical response time without sacrificing torque sensitivity. Future extensions will enable studies of high-frequency spin dynamics and broadband wavelength conversion via torque mixing., Although optomechanics enables precision metrology, measurements beyond mechanical properties often require hybrid devices. Here, Kim et al. demonstrate that a ferromagnetic needle integrated with a torsional resonator can determine the magnetic properties and amplify or cool the resonator motion.
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- 2017
56. Two-Level System Damping in a Quasi-One-Dimensional Optomechanical Resonator
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P. H. Kim, John P. Davis, Bradley Hauer, Fabien Souris, and C. Doolin
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Physics ,Condensed Matter - Materials Science ,Quantum Physics ,Quantum decoherence ,Condensed Matter - Mesoscale and Nanoscale Physics ,Condensed matter physics ,Dimension (graph theory) ,Materials Science (cond-mat.mtrl-sci) ,FOS: Physical sciences ,02 engineering and technology ,Dissipation ,021001 nanoscience & nanotechnology ,Coupling (probability) ,01 natural sciences ,Resonator ,Quantum state ,0103 physical sciences ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,Density of states ,010306 general physics ,0210 nano-technology ,Quantum Physics (quant-ph) ,Quantum tunnelling ,Physics - Optics ,Optics (physics.optics) - Abstract
Nanomechanical resonators have demonstrated great potential for use as versatile tools in a number of emerging quantum technologies. For such applications, the performance of these systems is restricted by the decoherence of their fragile quantum states, necessitating a thorough understanding of their dissipative coupling to the surrounding environment. In bulk amorphous solids, these dissipation channels are dominated at low temperatures by parasitic coupling to intrinsic two-level system (TLS) defects, however, there remains a disconnect between theory and experiment on how this damping manifests in dimensionally-reduced nanomechanical resonators. Here, we present an optomechanically-mediated thermal ringdown technique, which we use to perform simultaneous measurements of the dissipation in four mechanical modes of a cryogenically-cooled silicon nanoresonator, with resonant frequencies ranging from 3 - 19 MHz. Analyzing the device's mechanical damping rate at fridge temperatures between 10 mK - 10 K, we demonstrate quantitative agreement with the standard tunneling model for TLS ensembles confined to one dimension. From these fits, we extract the defect density of states ($P_0 \sim$ 1 - 4 $\times$ 10$^{44}$ J$^{-1}$ m$^{-3}$) and deformation potentials ($\gamma \sim$ 1 - 2 eV), showing that each mechanical mode couples on average to less than a single thermally-active defect at 10 mK., Comment: 21 pages, 10 figures, 6 tables, submitted version
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- 2017
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57. If you can't beat them, join them: the University of Alberta system description
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Mohammad Motallebi, Grzegorz Kondrak, Garrett Nicolai, Bradley Hauer, and Saeed Kazemi Najafi
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Computer science ,business.industry ,Beat (acoustics) ,Telecommunications ,business - Published
- 2017
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58. Bootstrapping Unsupervised Bilingual Lexicon Induction
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Grzegorz Kondrak, Garrett Nicolai, and Bradley Hauer
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Basis (linear algebra) ,Computer science ,business.industry ,Lexical similarity ,Bootstrapping (linguistics) ,Context (language use) ,02 engineering and technology ,010501 environmental sciences ,Translation (geometry) ,Lexicon ,computer.software_genre ,01 natural sciences ,Task (project management) ,0202 electrical engineering, electronic engineering, information engineering ,020201 artificial intelligence & image processing ,Artificial intelligence ,business ,computer ,Natural language processing ,0105 earth and related environmental sciences ,Vector space - Abstract
The task of unsupervised lexicon induction is to find translation pairs across monolingual corpora. We develop a novel method that creates seed lexicons by identifying cognates in the vocabularies of related languages on the basis of their frequency and lexical similarity. We apply bidirectional bootstrapping to a method which learns a linear mapping between context-based vector spaces. Experimental results on three language pairs show consistent improvement over prior work.
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- 2017
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59. A general procedure for thermomechanical calibration of nano/micro-mechanical resonators
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Kevin Beach, John P. Davis, C. Doolin, and Bradley Hauer
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Physics ,Condensed Matter - Mesoscale and Nanoscale Physics ,Thermal motion ,FOS: Physical sciences ,General Physics and Astronomy ,Equations of motion ,Spectral density ,02 engineering and technology ,Function (mathematics) ,Mechanics ,021001 nanoscience & nanotechnology ,01 natural sciences ,Finite element method ,3. Good health ,Resonator ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,0103 physical sciences ,Nano ,Calibration ,010306 general physics ,0210 nano-technology - Abstract
We provide a detailed description of a general procedure by which a nano/micro-mechanical resonator can be calibrated using its thermal motion. A brief introduction to the equations of motion for such a resonator is presented, followed by a detailed derivation of the corresponding power spectral density (PSD) function. The effective masses for a number of different resonator geometries are determined using both finite element method (FEM) modeling and analytical calculations., 18 pages, 8 figures, 12 tables
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- 2013
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60. Quantitative Magneto-Mechanical Detection and Control of the Barkhausen Effect
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Bradley Hauer, Mark R. Freeman, D. Vick, A. E. Fraser, John P. Davis, Jacob A. J. Burgess, and Fatemeh Fani Sani
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Magnetometer ,magnetic nanoparticle ,mechanical theory ,film ,Focused ion beam ,law.invention ,ion therapy ,symbols.namesake ,magnetometry ,law ,Condensed Matter::Superconductivity ,Barkhausen effect ,Magneto ,energy transfer ,Multidisciplinary ,quantitative analysis ,Condensed matter physics ,quantum mechanics ,ferromagnetic material ,Magnetic storage ,torsion ,Vortex ,Characterization (materials science) ,magnetic method ,Ferromagnetism ,magnetism ,symbols - Abstract
Controlling Magnetic Noise Ferromagnetic materials contain a number of magnetic domains, with individual domains switching stochastically as the field strength is increased. As magnetic memory elements shrink in size, it is important to understand, and ultimately control, this magnetic noise. Using a magnetic vortex core integrated with a nanomechanical torsion balance, Burgess et al. (p. 1051 , published online 17 January) created a two-dimensional map of the magnetic potential within the sample with nanoscale resolution. Moreover, introducing geometric defects (dimples) in the sample allowed the magnetization to be stabilized.
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- 2013
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61. Morphological Reinflection via Discriminative String Transduction
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Grzegorz Kondrak, Garrett Nicolai, Bradley Hauer, and Adam St Arnaud
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Discriminative model ,Computer science ,String (computer science) ,Transduction (psychology) ,Neuroscience - Published
- 2016
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62. Approaching the Standard Quantum Limit of Mechanical Torque Sensing
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P. H. Kim, C. Doolin, Bradley Hauer, Fabien Souris, and John P. Davis
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Science ,General Physics and Astronomy ,Physics::Optics ,FOS: Physical sciences ,02 engineering and technology ,01 natural sciences ,Article ,General Biochemistry, Genetics and Molecular Biology ,Optics ,0103 physical sciences ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,Torque ,Torque sensor ,Mechanical resonance ,Sensitivity (control systems) ,010306 general physics ,Optomechanics ,Physics ,Multidisciplinary ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Quantum limit ,Quantum noise ,General Chemistry ,Moment of inertia ,021001 nanoscience & nanotechnology ,Condensed Matter - Other Condensed Matter ,Astrophysics::Earth and Planetary Astrophysics ,0210 nano-technology ,business ,Physics - Optics ,Other Condensed Matter (cond-mat.other) ,Optics (physics.optics) - Abstract
Mechanical transduction of torque has been key to probing a number of physical phenomena, such as gravity, the angular momentum of light, the Casimir effect, magnetism, and quantum oscillations. Following similar trends as mass and force sensing, mechanical torque sensitivity can be dramatically improved by scaling down the physical dimensions, and therefore moment of inertia, of a torsional spring. Yet now, through precision nanofabrication and sub-wavelength cavity optomechanics, we have reached a point where geometric optimization can only provide marginal improvements to torque sensitivity. Instead, nanoscale optomechanical measurements of torque are overwhelmingly hindered by thermal noise. Here we present cryogenic measurements of a cavity-optomechanical torsional resonator cooled in a dilution refrigerator to a temperature of 25 mK, corresponding to an average phonon occupation of = 35, that demonstrate a record-breaking torque sensitivity of 2.9 yNm/Hz^{1/2}. This a 270-fold improvement over previous optomechanical torque sensors and just over an order of magnitude from its standard quantum limit. Furthermore, we demonstrate that mesoscopic test samples, such as micron-scale superconducting disks, can be integrated with our cryogenic optomechanical torque sensing platform, in contrast to other cryogenic optomechanical devices, opening the door for mechanical torque spectroscopy of intrinsically quantum systems., Comment: 25 pages, 7 figures
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- 2016
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63. Microfluidic and Nanofluidic Cavities for Quantum Fluids Experiments
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T. S. Biswas, Bradley Hauer, A. Suhel, A. Duh, John P. Davis, P. H. Kim, and R. Saeedi
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Quantum fluid ,Materials science ,Condensed Matter - Mesoscale and Nanoscale Physics ,Microfluidics ,Fluid Dynamics (physics.flu-dyn) ,FOS: Physical sciences ,Nanotechnology ,Physics - Fluid Dynamics ,Condensed Matter Physics ,01 natural sciences ,Atomic and Molecular Physics, and Optics ,3. Good health ,010305 fluids & plasmas ,Characterization (materials science) ,Condensed Matter - Other Condensed Matter ,Physics::Fluid Dynamics ,Nanolithography ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,0103 physical sciences ,General Materials Science ,010306 general physics ,Nanoscopic scale ,Microscale chemistry ,Other Condensed Matter (cond-mat.other) - Abstract
The union of quantum fluids research with nanoscience is rich with opportunities for new physics. The relevant length scales in quantum fluids, 3He in particular, are comparable to those possible using microfluidic and nanofluidic devices. In this article, we will briefly review how the physics of quantum fluids depends strongly on confinement on the microscale and nanoscale. Then we present devices fabricated specifically for quantum fluids research, with cavity sizes ranging from 30 nm to 11 microns deep, and the characterization of these devices for low temperature quantum fluids experiments., 12 pages, 3 figures, Accepted to Journal of Low Temperature Physics
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- 2012
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64. Nonlinear Power Spectral Densities for the Harmonic Oscillator
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John P. Davis, Joseph Maciejko, and Bradley Hauer
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Quantum nondemolition measurement ,Physics ,Quantum Physics ,Field (physics) ,Condensed Matter - Mesoscale and Nanoscale Physics ,Autocorrelation ,FOS: Physical sciences ,General Physics and Astronomy ,Spectral density ,01 natural sciences ,010305 fluids & plasmas ,Condensed Matter - Other Condensed Matter ,Nonlinear system ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,0103 physical sciences ,Correspondence principle ,Statistical physics ,Quantum Physics (quant-ph) ,010306 general physics ,Quantum ,Harmonic oscillator ,Other Condensed Matter (cond-mat.other) - Abstract
In this paper, we discuss a general procedure by which nonlinear power spectral densities (PSDs) of the harmonic oscillator can be calculated in both the quantum and classical regimes. We begin with an introduction of the damped and undamped classical harmonic oscillator, followed by an overview of the quantum mechanical description of this system. A brief review of both the classical and quantum autocorrelation functions (ACFs) and PSDs follow. We then introduce a general method by which the kth-order PSD for the harmonic oscillator can be calculated, where $k$ is any positive integer. This formulation is verified by first reproducing the known results for the $k = 1$ case of the linear PSD. It is then extended to calculate the second-order PSD, useful in the field of quantum measurement, corresponding to the $k = 2$ case of the generalized method. In this process, damping is included into each of the quantum linear and quadratic PSDs, producing realistic models for the PSDs found in experiment. These quantum PSDs are shown to obey the correspondence principle by matching with what was calculated for their classical counterparts in the high temperature, high-Q limit. Finally, we demonstrate that our results can be reproduced using the fluctuation-dissipation theorem, providing an independent check of our resultant PSDs., 27 pages, 5 figures
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- 2015
65. Optical microscope and tapered fiber coupling apparatus for a dilution refrigerator
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Greg Popowich, P. Doolin, Xavier Rojas, Bradley Hauer, A. Fredrick, John P. Davis, P. H. Kim, and A. J. R. MacDonald
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Quantum Physics ,Optical fiber ,Materials science ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Physics::Optics ,FOS: Physical sciences ,Cryogenics ,law.invention ,Condensed Matter - Other Condensed Matter ,Coupling (electronics) ,Resonator ,Optical microscope ,law ,Bundle ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,Optoelectronics ,Fiber ,Dilution refrigerator ,business ,Quantum Physics (quant-ph) ,Instrumentation ,Physics - Optics ,Other Condensed Matter (cond-mat.other) ,Optics (physics.optics) - Abstract
We have developed a system for tapered fiber measurements of optomechanical resonators inside a dilution refrigerator, which is compatible with both on- and off-chip devices. Our apparatus features full three-dimensional control of the taper-resonator coupling conditions enabling critical coupling, with an overall fiber transmission efficiency of up to 70%. Notably, our design incorporates an optical microscope system consisting of a coherent bundle of 37,000 optical fibers for real-time imaging of the experiment at a resolution of $\sim$1 $\mu$m. We present cryogenic optical and optomechanical measurements of resonators coupled to tapered fibers at temperatures as low as 9 mK., Comment: 7 pages, 7 figures
- Published
- 2015
66. Multiple System Combination for Transliteration
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Bradley Hauer, Adam St Arnaud, Mohammad Salameh, Lei Yao, Garrett Nicolai, Ying Xu, and Grzegorz Kondrak
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Focus (computing) ,System combination ,Computer science ,business.industry ,media_common.quotation_subject ,InformationSystems_INFORMATIONSTORAGEANDRETRIEVAL ,Context (language use) ,computer.software_genre ,Base (topology) ,Task (project management) ,ComputingMethodologies_PATTERNRECOGNITION ,Transliteration ,Quality (business) ,Artificial intelligence ,business ,computer ,Natural language processing ,media_common - Abstract
We report the results of our experiments in the context of the NEWS 2015 Shared Task on Transliteration. We focus on methods of combining multiple base systems, and leveraging transliterations from multiple languages. We show error reductions over the best base system of up to 10% when using supplemental transliterations, and up to 20% when using system combination. We also discuss the quality of the shared task datasets.
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- 2015
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67. Optomechanics and thermometry of cryogenic silica microresonators
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Xavier Rojas, Bradley Hauer, P. H. Kim, John P. Davis, Greg Popowich, and A. J. R. MacDonald
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Physics ,Quantum Physics ,Condensed Matter - Mesoscale and Nanoscale Physics ,Sideband ,Phonon ,business.industry ,Physics::Optics ,FOS: Physical sciences ,02 engineering and technology ,021001 nanoscience & nanotechnology ,01 natural sciences ,Resonator ,Quality (physics) ,Optics ,Thermalisation ,0103 physical sciences ,Thermal ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,Optoelectronics ,010306 general physics ,0210 nano-technology ,business ,Ground state ,Quantum Physics (quant-ph) ,Optomechanics - Abstract
We present measurements of silica optomechanical resonators, known as bottle resonators, passively cooled in a cryogenic environment. These devices possess a suite of properties that make them advantageous for preparation and measurement in the mechanical ground state, including high mechanical frequency, high optical and mechanical quality factors, and optomechanical sideband resolution. Performing thermometry of the mechanical motion, we find that the optical and mechanical modes demonstrate quantitatively similar laser-induced heating, limiting the lowest average phonon occupation observed to just ~1500. Thermalization to the 9 mK thermal bath would facilitate quantum measurements on these promising nanogram-scale mechanical resonators., Comment: 10 pages, 8 figues, submission version
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- 2015
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68. Ultrasonic interferometer for first-sound measurements of confined liquidHe4
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Bradley Hauer, John P. Davis, A. J. R. MacDonald, Y. Yang, P. Saberi, and Xavier Rojas
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Scaling law ,Materials science ,Microfluidics ,FOS: Physical sciences ,02 engineering and technology ,01 natural sciences ,Measure (mathematics) ,Superconductivity (cond-mat.supr-con) ,Superfluidity ,Optics ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,0103 physical sciences ,Point (geometry) ,010306 general physics ,Sound (geography) ,geography ,geography.geographical_feature_category ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Condensed Matter - Superconductivity ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Electronic, Optical and Magnetic Materials ,Interferometry ,Ultrasonic sensor ,0210 nano-technology ,business - Abstract
We present a new technique for probing the properties of quantum fluids in restricted geometries. We have confined liquid 4He within microfluidic devices formed from glass wafers, in which one dimension is on the micro scale. Using an ultrasonic analog to Fabry-Perot interferometry, we have measured the first-sound of the confined liquid 4He, which can be a probe of critical behavior near the lambda point ($T_{\lambda}$). All thermodynamic properties of liquid $^4$He can be derived from first-sound and heat capacity measurements, and although quite a bit of experimental work has been done on the latter, no measurement of first-sound has been reported for a precisely confined geometry smaller than a few tens of micrometers. In this work, we report measurements of isobaric first sound in liquid $^4$He confined in cavities as small as ~ 5 ${\mu}$m. Our experimental set-up allows us to pressurize the liquid up to ~ 25 bar without causing deformation of the confined geometry, a pressure which is about 4 times larger than previously reported with similar microfluidic devices. Our preliminary results indicate that one can possibly observe finite-size effects and verify scaling laws, by using similar devices with smaller confinement., Comment: 9 pages, 11 figures
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- 2014
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69. On-chip cavity optomechanical coupling
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P. H. Kim, A. J. R. MacDonald, C. Doolin, John P. Davis, H. Ramp, and Bradley Hauer
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Coupling ,Physics ,Physics - Instrumentation and Detectors ,Optical fiber ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Single-mode optical fiber ,FOS: Physical sciences ,Instrumentation and Detectors (physics.ins-det) ,law.invention ,law ,Optical cavity ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,Optoelectronics ,Fiber ,business ,Instrumentation ,Optomechanics ,Optics (physics.optics) ,Physics - Optics - Abstract
On-chip cavity optomechanics, in which strong co-localization of light and mechanical motion is engineered, relies on efficient coupling of light both into and out of the on-chip optical resonator. Here we detail our particular style of tapered and dimpled optical fibers, pioneered by the Painter group at Caltech, which are a versatile and reliable solution to efficient on-chip coupling. First, a brief overview of tapered, single mode fibers is presented, in which the single mode cutoff diameter is highlighted. The apparatus used to create a dimpled tapered fiber is then described, followed by a comprehensive account of the procedure by which a dimpled tapered fiber is produced and mounted in our system. The custom-built optical access vacuum chambers in which our on-chip optomechanical measurements are performed are then discussed. Finally, the process by which our optomechanical devices are fabricated and the method by which we explore their optical and mechanical properties is explained. It is our expectation that this manuscript will enable the novice to develop advanced optomechanical experiments., 31 pages, 9 figures
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- 2014
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70. High-Q Gold and Silicon Nitride Bilayer Nanostrings
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A. Suhel, John P. Davis, Kevin Beach, T. S. Biswas, A. Palomino, and Bradley Hauer
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Materials science ,Physics and Astronomy (miscellaneous) ,Sensing applications ,FOS: Physical sciences ,02 engineering and technology ,Edge (geometry) ,01 natural sciences ,Thermal expansion ,law.invention ,Overlayer ,chemistry.chemical_compound ,Thermoelastic damping ,law ,0103 physical sciences ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,010306 general physics ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Bilayer ,021001 nanoscience & nanotechnology ,Condensed Matter - Other Condensed Matter ,Silicon nitride ,chemistry ,Optoelectronics ,0210 nano-technology ,Alternating current ,business ,Other Condensed Matter (cond-mat.other) - Abstract
Low-mass, high-Q, silicon nitride nanostrings are at the cutting edge of nanomechanical devices for sensing applications. Here we show that the addition of a chemically functionalizable gold overlayer does not adversely affect the Q of the fundamental out-of-plane mode. Instead the device retains its mechanical responsiveness while gaining sensitivity to molecular bonding. Furthermore, differences in thermal expansion within the bilayer give rise to internal stresses that can be electrically controlled. In particular, an alternating current excites resonant motion of the nanostring. This AC thermoelastic actuation is simple, robust, and provides an integrated approach to sensor actuation., Comment: 5 pages, 4 figures + supplementary material
- Published
- 2012
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71. Multidimensional optomechanical cantilevers for high-frequency force sensing
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Bradley Hauer, John P. Davis, C. Doolin, P. H. Kim, and A. J. R. MacDonald
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Physics ,Cantilever ,business.industry ,Atomic force microscopy ,Bandwidth (signal processing) ,Force spectroscopy ,General Physics and Astronomy ,Optoelectronics ,Time resolution ,business - Abstract
High-frequency atomic force microscopy has enabled extraordinary new science through large bandwidth, high-speed measurements of atomic and molecular structures. However, traditional optical detection schemes restrict the dimensions, and therefore the frequency, of the cantilever?ultimately setting a limit to the time resolution of experiments. Here we demonstrate optomechanical detection of low-mass, high-frequency nanomechanical cantilevers (up to 20 MHz) and anticipate their use for single-molecule force measurements. These cantilevers achieve 2 fm displacement noise floors, and force sensitivity down to 132 aN . Furthermore, the ability to resolve both in-plane and out-of-plane motion of our cantilevers makes them excellent candidates for ultrasensitive multidimensional force spectroscopy, and optomechanical interactions, such as tuning of the cantilever frequency in situ, provide opportunities in high-speed, high-resolution experiments.
- Published
- 2014
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72. Nanoscale torsional optomechanics
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Mark R. Freeman, P. H. Kim, Bradley Hauer, A. J. R. MacDonald, Paul E. Barclay, John P. Davis, and C. Doolin
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Optical fiber ,Materials science ,Physics and Astronomy (miscellaneous) ,Nanophotonics ,FOS: Physical sciences ,02 engineering and technology ,Noise floor ,Opto-mechanics ,01 natural sciences ,law.invention ,Optomechanical ,Resonator ,Physical measurement ,law ,On chips ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,0103 physical sciences ,Nanotechnology ,Integrated device ,Optical fibers ,Resonators ,Fiber ,010306 general physics ,Optomechanics ,Fiber-based systems ,Microdisk whispering galleries ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Torsional resonator ,021001 nanoscience & nanotechnology ,Optical fiber probe ,Optoelectronics ,Nano scale ,Whispering-gallery wave ,0210 nano-technology ,business ,Nanomechanics ,Optics (physics.optics) ,Physics - Optics - Abstract
Optomechanical transduction is demonstrated for nanoscale torsional resonators evanescently coupled to optical microdisk whispering gallery mode resonators. The on-chip, integrated devices are measured using a fully fiber-based system, including a tapered and dimpled optical fiber probe. With a thermomechanically calibrated optomechanical noise floor down to 7 fm/sqrt(Hz), these devices open the door for a wide range of physical measurements involving extremely small torques, as little as 4x10^-20 N*m., 4 pages, 4 figures - Accepted to APL Oct 22nd, 2012. To appear in February 4th issue - as cover article
- Published
- 2013
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73. Dissipation mechanisms in thermomechanically driven silicon nitride nanostrings
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T. S. Biswas, Bradley Hauer, A. Suhel, John P. Davis, and Kevin Beach
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Materials science ,Physics and Astronomy (miscellaneous) ,FOS: Physical sciences ,02 engineering and technology ,Bending ,01 natural sciences ,chemistry.chemical_compound ,Quality (physics) ,Nanosensor ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,0103 physical sciences ,010306 general physics ,Condensed Matter - Mesoscale and Nanoscale Physics ,business.industry ,Dissipation ,021001 nanoscience & nanotechnology ,3. Good health ,Condensed Matter - Other Condensed Matter ,Silicon nitride ,chemistry ,Molecular vibration ,Q factor ,Optoelectronics ,0210 nano-technology ,business ,Displacement (fluid) ,Other Condensed Matter (cond-mat.other) - Abstract
High-stress silicon nitride nanostrings are a promising system for sensing applications because of their ultra-high mechanical quality factors (Qs). By performing thermomechanical calibration across multiple vibrational modes, we are able to assess the roles of the various dissipation mechanisms in these devices. Specifically, we possess a set of nanostrings in which all measured modes fall upon a single curve of peak displacement versus frequency. This allows us to rule out bulk bending and intrinsic loss mechanisms as dominant sources of dissipation and to conclude that the most significant contribution to dissipation in high-stress nanostrings occurs at the anchor points., Comment: 4 pages (+3 supplementary), 3 figures, accepted to Applied Physics Letters
- Published
- 2012
- Full Text
- View/download PDF
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