Advancing Quantum Information Science: National Challenges and Opportunities
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Key Concepts for Future QIS Learners Workshop Output Published Online May 13, 2020
Key Concepts for Future QIS Learners Workshop output published online May 13, 2020 Background and Overview On behalf of the Interagency Working Group on Workforce, Industry and Infrastructure, under the NSTC Subcommittee on Quantum Information Science (QIS), the National Science Foundation invited 25 researchers and educators to come together to deliberate on defining a core set of key concepts for future QIS learners that could provide a starting point for further curricular and educator development activities. The deliberative group included university and industry researchers, secondary school and college educators, and representatives from educational and professional organizations. The workshop participants focused on identifying concepts that could, with additional supporting resources, help prepare secondary school students to engage with QIS and provide possible pathways for broader public engagement. This workshop report identifies a set of nine Key Concepts. Each Concept is introduced with a concise overall statement, followed by a few important fundamentals. Connections to current and future technologies are included, providing relevance and context. The first Key Concept defines the field as a whole. Concepts 2-6 introduce ideas that are necessary for building an understanding of quantum information science and its applications. Concepts 7-9 provide short explanations of critical areas of study within QIS: quantum computing, quantum communication and quantum sensing. The Key Concepts are not intended to be an introductory guide to quantum information science, but rather provide a framework for future expansion and adaptation for students at different levels in computer science, mathematics, physics, and chemistry courses. As such, it is expected that educators and other community stakeholders may not yet have a working knowledge of content covered in the Key Concepts. -
Exercises in Classical Mechanics 1 Moments of Inertia 2 Half-Cylinder
Exercises in Classical Mechanics CUNY GC, Prof. D. Garanin No.1 Solution ||||||||||||||||||||||||||||||||||||||||| 1 Moments of inertia (5 points) Calculate tensors of inertia with respect to the principal axes of the following bodies: a) Hollow sphere of mass M and radius R: b) Cone of the height h and radius of the base R; both with respect to the apex and to the center of mass. c) Body of a box shape with sides a; b; and c: Solution: a) By symmetry for the sphere I®¯ = I±®¯: (1) One can ¯nd I easily noticing that for the hollow sphere is 1 1 X ³ ´ I = (I + I + I ) = m y2 + z2 + z2 + x2 + x2 + y2 3 xx yy zz 3 i i i i i i i i 2 X 2 X 2 = m r2 = R2 m = MR2: (2) 3 i i 3 i 3 i i b) and c): Standard solutions 2 Half-cylinder ϕ (10 points) Consider a half-cylinder of mass M and radius R on a horizontal plane. a) Find the position of its center of mass (CM) and the moment of inertia with respect to CM. b) Write down the Lagrange function in terms of the angle ' (see Fig.) c) Find the frequency of cylinder's oscillations in the linear regime, ' ¿ 1. Solution: (a) First we ¯nd the distance a between the CM and the geometrical center of the cylinder. With σ being the density for the cross-sectional surface, so that ¼R2 M = σ ; (3) 2 1 one obtains Z Z 2 2σ R p σ R q a = dx x R2 ¡ x2 = dy R2 ¡ y M 0 M 0 ¯ 2 ³ ´3=2¯R σ 2 2 ¯ σ 2 3 4 = ¡ R ¡ y ¯ = R = R: (4) M 3 0 M 3 3¼ The moment of inertia of the half-cylinder with respect to the geometrical center is the same as that of the cylinder, 1 I0 = MR2: (5) 2 The moment of inertia with respect to the CM I can be found from the relation I0 = I + Ma2 (6) that yields " µ ¶ # " # 1 4 2 1 32 I = I0 ¡ Ma2 = MR2 ¡ = MR2 1 ¡ ' 0:3199MR2: (7) 2 3¼ 2 (3¼)2 (b) The Lagrange function L is given by L('; '_ ) = T ('; '_ ) ¡ U('): (8) The potential energy U of the half-cylinder is due to the elevation of its CM resulting from the deviation of ' from zero. -
Quantum Non-Demolition Measurements
Quantum non-demolition measurements: Concepts, theory and practice Unnikrishnan. C. S. Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India Abstract This is a limited overview of quantum non-demolition (QND) mea- surements, with brief discussions of illustrative examples meant to clar- ify the essential features. In a QND measurement, the predictability of a subsequent value of a precisely measured observable is maintained and any random back-action from uncertainty introduced into a non- commuting observable is avoided. The fundamental ideas, relevant theory and the conditions and scope for applicability are discussed with some examples. Precision measurements have indeed gained from developing QND measurements. Some implementations in quantum optics, gravitational wave detectors and spin-magnetometry are dis- cussed. Heisenberg Uncertainty, Standard quantum limit, Quantum non-demolition, Back-action evasion, Squeezing, Gravitational Waves. 1 Introduction Precision measurements on physical systems are limited by various sources of noise. Of these, limits imposed by thermal noise and quantum noise are arXiv:1811.09613v1 [quant-ph] 22 Nov 2018 fundamental and unavoidable. There are metrological methods developed to circumvent these limitations in specific situations of measurement. Though the thermal noise can be reduced by cryogenic techniques and some band- limiting strategies, quantum noise dictated by the uncertainty relations is universal and cannot be reduced. However, since it applies to the product of the -
Quantum Mechanics As a Limiting Case of Classical Mechanics
View metadata, citation and similar papers at core.ac.uk brought to you by CORE Quantum Mechanics As A Limiting Case provided by CERN Document Server of Classical Mechanics Partha Ghose S. N. Bose National Centre for Basic Sciences Block JD, Sector III, Salt Lake, Calcutta 700 091, India In spite of its popularity, it has not been possible to vindicate the conven- tional wisdom that classical mechanics is a limiting case of quantum mechan- ics. The purpose of the present paper is to offer an alternative point of view in which quantum mechanics emerges as a limiting case of classical mechanics in which the classical system is decoupled from its environment. PACS no. 03.65.Bz 1 I. INTRODUCTION One of the most puzzling aspects of quantum mechanics is the quantum measurement problem which lies at the heart of all its interpretations. With- out a measuring device that functions classically, there are no ‘events’ in quantum mechanics which postulates that the wave function contains com- plete information of the system concerned and evolves linearly and unitarily in accordance with the Schr¨odinger equation. The system cannot be said to ‘possess’ physical properties like position and momentum irrespective of the context in which such properties are measured. The language of quantum mechanics is not that of realism. According to Bohr the classicality of a measuring device is fundamental and cannot be derived from quantum theory. In other words, the process of measurement cannot be analyzed within quantum theory itself. A simi- lar conclusion also follows from von Neumann’s approach [1]. -
Quantum Computation and Complexity Theory
Quantum computation and complexity theory Course given at the Institut fÈurInformationssysteme, Abteilung fÈurDatenbanken und Expertensysteme, University of Technology Vienna, Wintersemester 1994/95 K. Svozil Institut fÈur Theoretische Physik University of Technology Vienna Wiedner Hauptstraûe 8-10/136 A-1040 Vienna, Austria e-mail: [email protected] December 5, 1994 qct.tex Abstract The Hilbert space formalism of quantum mechanics is reviewed with emphasis on applicationsto quantum computing. Standardinterferomeric techniques are used to construct a physical device capable of universal quantum computation. Some consequences for recursion theory and complexity theory are discussed. hep-th/9412047 06 Dec 94 1 Contents 1 The Quantum of action 3 2 Quantum mechanics for the computer scientist 7 2.1 Hilbert space quantum mechanics ..................... 7 2.2 From single to multiple quanta Ð ªsecondº ®eld quantization ...... 15 2.3 Quantum interference ............................ 17 2.4 Hilbert lattices and quantum logic ..................... 22 2.5 Partial algebras ............................... 24 3 Quantum information theory 25 3.1 Information is physical ........................... 25 3.2 Copying and cloning of qbits ........................ 25 3.3 Context dependence of qbits ........................ 26 3.4 Classical versus quantum tautologies .................... 27 4 Elements of quantum computatability and complexity theory 28 4.1 Universal quantum computers ....................... 30 4.2 Universal quantum networks ........................ 31 4.3 Quantum recursion theory ......................... 35 4.4 Factoring .................................. 36 4.5 Travelling salesman ............................. 36 4.6 Will the strong Church-Turing thesis survive? ............... 37 Appendix 39 A Hilbert space 39 B Fundamental constants of physics and their relations 42 B.1 Fundamental constants of physics ..................... 42 B.2 Conversion tables .............................. 43 B.3 Electromagnetic radiation and other wave phenomena ......... -
The Uncertainty Principle (Stanford Encyclopedia of Philosophy) Page 1 of 14
The Uncertainty Principle (Stanford Encyclopedia of Philosophy) Page 1 of 14 Open access to the SEP is made possible by a world-wide funding initiative. Please Read How You Can Help Keep the Encyclopedia Free The Uncertainty Principle First published Mon Oct 8, 2001; substantive revision Mon Jul 3, 2006 Quantum mechanics is generally regarded as the physical theory that is our best candidate for a fundamental and universal description of the physical world. The conceptual framework employed by this theory differs drastically from that of classical physics. Indeed, the transition from classical to quantum physics marks a genuine revolution in our understanding of the physical world. One striking aspect of the difference between classical and quantum physics is that whereas classical mechanics presupposes that exact simultaneous values can be assigned to all physical quantities, quantum mechanics denies this possibility, the prime example being the position and momentum of a particle. According to quantum mechanics, the more precisely the position (momentum) of a particle is given, the less precisely can one say what its momentum (position) is. This is (a simplistic and preliminary formulation of) the quantum mechanical uncertainty principle for position and momentum. The uncertainty principle played an important role in many discussions on the philosophical implications of quantum mechanics, in particular in discussions on the consistency of the so-called Copenhagen interpretation, the interpretation endorsed by the founding fathers Heisenberg and Bohr. This should not suggest that the uncertainty principle is the only aspect of the conceptual difference between classical and quantum physics: the implications of quantum mechanics for notions as (non)-locality, entanglement and identity play no less havoc with classical intuitions. -
Analysis of Nonlinear Dynamics in a Classical Transmon Circuit
Analysis of Nonlinear Dynamics in a Classical Transmon Circuit Sasu Tuohino B. Sc. Thesis Department of Physical Sciences Theoretical Physics University of Oulu 2017 Contents 1 Introduction2 2 Classical network theory4 2.1 From electromagnetic fields to circuit elements.........4 2.2 Generalized flux and charge....................6 2.3 Node variables as degrees of freedom...............7 3 Hamiltonians for electric circuits8 3.1 LC Circuit and DC voltage source................8 3.2 Cooper-Pair Box.......................... 10 3.2.1 Josephson junction.................... 10 3.2.2 Dynamics of the Cooper-pair box............. 11 3.3 Transmon qubit.......................... 12 3.3.1 Cavity resonator...................... 12 3.3.2 Shunt capacitance CB .................. 12 3.3.3 Transmon Lagrangian................... 13 3.3.4 Matrix notation in the Legendre transformation..... 14 3.3.5 Hamiltonian of transmon................. 15 4 Classical dynamics of transmon qubit 16 4.1 Equations of motion for transmon................ 16 4.1.1 Relations with voltages.................. 17 4.1.2 Shunt resistances..................... 17 4.1.3 Linearized Josephson inductance............. 18 4.1.4 Relation with currents................... 18 4.2 Control and read-out signals................... 18 4.2.1 Transmission line model.................. 18 4.2.2 Equations of motion for coupled transmission line.... 20 4.3 Quantum notation......................... 22 5 Numerical solutions for equations of motion 23 5.1 Design parameters of the transmon................ 23 5.2 Resonance shift at nonlinear regime............... 24 6 Conclusions 27 1 Abstract The focus of this thesis is on classical dynamics of a transmon qubit. First we introduce the basic concepts of the classical circuit analysis and use this knowledge to derive the Lagrangians and Hamiltonians of an LC circuit, a Cooper-pair box, and ultimately we derive Hamiltonian for a transmon qubit. -
Quantum Mechanics
Quantum Mechanics Richard Fitzpatrick Professor of Physics The University of Texas at Austin Contents 1 Introduction 5 1.1 Intendedaudience................................ 5 1.2 MajorSources .................................. 5 1.3 AimofCourse .................................. 6 1.4 OutlineofCourse ................................ 6 2 Probability Theory 7 2.1 Introduction ................................... 7 2.2 WhatisProbability?.............................. 7 2.3 CombiningProbabilities. ... 7 2.4 Mean,Variance,andStandardDeviation . ..... 9 2.5 ContinuousProbabilityDistributions. ........ 11 3 Wave-Particle Duality 13 3.1 Introduction ................................... 13 3.2 Wavefunctions.................................. 13 3.3 PlaneWaves ................................... 14 3.4 RepresentationofWavesviaComplexFunctions . ....... 15 3.5 ClassicalLightWaves ............................. 18 3.6 PhotoelectricEffect ............................. 19 3.7 QuantumTheoryofLight. .. .. .. .. .. .. .. .. .. .. .. .. .. 21 3.8 ClassicalInterferenceofLightWaves . ...... 21 3.9 QuantumInterferenceofLight . 22 3.10 ClassicalParticles . .. .. .. .. .. .. .. .. .. .. .. .. .. .. 25 3.11 QuantumParticles............................... 25 3.12 WavePackets .................................. 26 2 QUANTUM MECHANICS 3.13 EvolutionofWavePackets . 29 3.14 Heisenberg’sUncertaintyPrinciple . ........ 32 3.15 Schr¨odinger’sEquation . 35 3.16 CollapseoftheWaveFunction . 36 4 Fundamentals of Quantum Mechanics 39 4.1 Introduction .................................. -
Arxiv:Quant-Ph/0412078V1 10 Dec 2004 Lt Eemnto Fteps-Esrmn Tt.When State
Quantum-Enhanced Measurements: A B Beating the Standard Quantum Limit Vittorio Giovannetti1, Seth Lloyd2, Lorenzo Maccone3 ∆ x ∆ x ∆ p 1 NEST-INFM & Scuola Normale Superiore, Piazza dei Cavalieri 7, I-56126, Pisa, Italy. p x x 2 MIT, Research Laboratory of Electronics and Dept. of Mechanical Engineering, 77 Massachusetts Ave., Cambridge, MA 02139, USA. CD 3 QUIT - Quantum Information Theory Group, Dip. di Fisica “A. Volta”, Universit`adi Pavia, via A. Bassi 6 I-27100, Pavia, Italy. One sentence summary: To attain the limits to measurement preci- sion imposed by quantum mechanics, ‘quantum tricks’ are often required. p p x x Abstract: Quantum mechanics, through the Heisen- Figure 1: The Heisenberg uncertainty relation. In quan- berg uncertainty principle, imposes limits to the pre- tum mechanics the outcomes x1, x2, etc. of the measurements cision of measurement. Conventional measurement of a physical quantity x are statistical variables; that is, they techniques typically fail to reach these limits. Con- are randomly distributed according to a probability determined ventional bounds to the precision of measurements by the state of the system. A measure of the “sharpness” of a such as the shot noise limit or the standard quan- measurement is given by the spread ∆x of the outcomes: An tum limit are not as fundamental as the Heisenberg example is given in (A), where the outcomes (tiny triangles) are limits, and can be beaten using quantum strategies distributed according to a Gaussian probability with standard that employ ‘quantum tricks’ such as squeezing and deviation ∆x. The Heisenberg uncertainty relation states that entanglement. when simultaneously measuring incompatible observables such as position x and momentum p the product of the spreads is lower bounded: ∆x ∆p ≥ ~/2, where ~ is the Planck constant. -
Al Transmon Qubits on Silicon-On-Insulator for Quantum Device Integration Andrew J
Al transmon qubits on silicon-on-insulator for quantum device integration Andrew J. Keller, Paul B. Dieterle, Michael Fang, Brett Berger, Johannes M. Fink, and Oskar Painter Citation: Appl. Phys. Lett. 111, 042603 (2017); doi: 10.1063/1.4994661 View online: http://dx.doi.org/10.1063/1.4994661 View Table of Contents: http://aip.scitation.org/toc/apl/111/4 Published by the American Institute of Physics Articles you may be interested in Superconducting noise bolometer with microwave bias and readout for array applications Applied Physics Letters 111, 042601 (2017); 10.1063/1.4995981 A silicon nanowire heater and thermometer Applied Physics Letters 111, 043504 (2017); 10.1063/1.4985632 Graphitization of self-assembled monolayers using patterned nickel-copper layers Applied Physics Letters 111, 043102 (2017); 10.1063/1.4995412 Perfectly aligned shallow ensemble nitrogen-vacancy centers in (111) diamond Applied Physics Letters 111, 043103 (2017); 10.1063/1.4993160 Broadband conversion of microwaves into propagating spin waves in patterned magnetic structures Applied Physics Letters 111, 042404 (2017); 10.1063/1.4995991 Ferromagnetism in graphene due to charge transfer from atomic Co to graphene Applied Physics Letters 111, 042402 (2017); 10.1063/1.4994814 APPLIED PHYSICS LETTERS 111, 042603 (2017) Al transmon qubits on silicon-on-insulator for quantum device integration Andrew J. Keller,1,2 Paul B. Dieterle,1,2 Michael Fang,1,2 Brett Berger,1,2 Johannes M. Fink,1,2,3 and Oskar Painter1,2,a) 1Kavli Nanoscience Institute and Thomas J. Watson Laboratory of Applied Physics, California Institute of Technology, Pasadena, California 91125, USA 2Institute for Quantum Information and Matter, California Institute of Technology, Pasadena, California 91125, USA 3Institute for Science and Technology Austria, 3400 Klosterneuburg, Austria (Received 3 April 2017; accepted 5 July 2017; published online 25 July 2017) We present the fabrication and characterization of an aluminum transmon qubit on a silicon-on-insulator substrate. -
The Quantum Bases for Human Expertise, Knowledge, and Problem-Solving (Extended Version with Applications)
A Service of Leibniz-Informationszentrum econstor Wirtschaft Leibniz Information Centre Make Your Publications Visible. zbw for Economics Bickley, Steve J.; Chan, Ho Fai; Schmidt, Sascha Leonard; Torgler, Benno Working Paper Quantum-sapiens: The quantum bases for human expertise, knowledge, and problem-solving (Extended version with applications) CREMA Working Paper, No. 2021-14 Provided in Cooperation with: CREMA - Center for Research in Economics, Management and the Arts, Zürich Suggested Citation: Bickley, Steve J.; Chan, Ho Fai; Schmidt, Sascha Leonard; Torgler, Benno (2021) : Quantum-sapiens: The quantum bases for human expertise, knowledge, and problem- solving (Extended version with applications), CREMA Working Paper, No. 2021-14, Center for Research in Economics, Management and the Arts (CREMA), Zürich This Version is available at: http://hdl.handle.net/10419/234629 Standard-Nutzungsbedingungen: Terms of use: Die Dokumente auf EconStor dürfen zu eigenen wissenschaftlichen Documents in EconStor may be saved and copied for your Zwecken und zum Privatgebrauch gespeichert und kopiert werden. personal and scholarly purposes. Sie dürfen die Dokumente nicht für öffentliche oder kommerzielle You are not to copy documents for public or commercial Zwecke vervielfältigen, öffentlich ausstellen, öffentlich zugänglich purposes, to exhibit the documents publicly, to make them machen, vertreiben oder anderweitig nutzen. publicly available on the internet, or to distribute or otherwise use the documents in public. Sofern die Verfasser die Dokumente unter Open-Content-Lizenzen (insbesondere CC-Lizenzen) zur Verfügung gestellt haben sollten, If the documents have been made available under an Open gelten abweichend von diesen Nutzungsbedingungen die in der dort Content Licence (especially Creative Commons Licences), you genannten Lizenz gewährten Nutzungsrechte. -
Newtonian Mechanics Is Most Straightforward in Its Formulation and Is Based on Newton’S Second Law
CLASSICAL MECHANICS D. A. Garanin September 30, 2015 1 Introduction Mechanics is part of physics studying motion of material bodies or conditions of their equilibrium. The latter is the subject of statics that is important in engineering. General properties of motion of bodies regardless of the source of motion (in particular, the role of constraints) belong to kinematics. Finally, motion caused by forces or interactions is the subject of dynamics, the biggest and most important part of mechanics. Concerning systems studied, mechanics can be divided into mechanics of material points, mechanics of rigid bodies, mechanics of elastic bodies, and mechanics of fluids: hydro- and aerodynamics. At the core of each of these areas of mechanics is the equation of motion, Newton's second law. Mechanics of material points is described by ordinary differential equations (ODE). One can distinguish between mechanics of one or few bodies and mechanics of many-body systems. Mechanics of rigid bodies is also described by ordinary differential equations, including positions and velocities of their centers and the angles defining their orientation. Mechanics of elastic bodies and fluids (that is, mechanics of continuum) is more compli- cated and described by partial differential equation. In many cases mechanics of continuum is coupled to thermodynamics, especially in aerodynamics. The subject of this course are systems described by ODE, including particles and rigid bodies. There are two limitations on classical mechanics. First, speeds of the objects should be much smaller than the speed of light, v c, otherwise it becomes relativistic mechanics. Second, the bodies should have a sufficiently large mass and/or kinetic energy.