Editors Quantum Physics And Geometry - Web Education

3y ago
23 Views
2 Downloads
2.70 MB
177 Pages
Last View : 18d ago
Last Download : 3m ago
Upload by : Madison Stoltz
Transcription

Lecture Notes of the Unione Matematica ItalianaEdoardo BallicoAlessandra BernardiIacopo CarusottoSonia MazzucchiValter Moretti EditorsQuantumPhysics andGeometry

Lecture Notes ofthe Unione Matematica ItalianaMore information about this series at http://www.springer.com/series/717225

Editorial BoardCiro Ciliberto(Editor in Chief)Dipartimento di MatematicaUniversità di Roma Tor VergataVia della Ricerca Scientifica00133 Roma, Italye-mail: cilibert@axp.mat.uniroma2.itFranco FlandoliDipartimento diMatematica ApplicataUniversità di PisaVia Buonarroti 1c56127 Pisa, Italye-mail: flandoli@dma.unipi.itSusanna Terracini(Co-editor in Chief)Università degli Studi di TorinoDipartimento di Matematica “Giuseppe Peano”Via Carlo Alberto 1010123 Torino, Italye-mail: susanna.teraccini@unito.itAngus MaclntyreQueen Mary University of LondonSchool of Mathematical SciencesMile End RoadLondon E1 4NS, United Kingdome-mail: a.macintyre@qmul.ac.ukAdolfo Ballester-BollinchesDepartment d’ÀlgebraFacultat de MatemàtiquesUniversitat de ValènciaDr. Moliner, 5046100 Burjassot (València), Spaine-mail: Adolfo.Ballester@uv.esAnnalisa BuffaIMATI – C.N.R. PaviaVia Ferrata 127100 Pavia, Italye-mail: annalisa@imati.cnr.itLucia CaporasoDipartimento di MatematicaUniversità Roma TreLargo San Leonardo MurialdoI-00146 Roma, Italye-mail: caporaso@mat.uniroma3.itFabrizio CataneseMathematisches InstitutUniversitätstraÿe 3095447 Bayreuth, Germanye-mail: fabrizio.catanese@uni-bayreuth.deCorrado De ConciniDipartimento di MatematicaUniversità di Roma “La Sapienza”Piazzale Aldo Moro 500185 Roma, Italye-mail: deconcin@mat.uniroma1.itCamillo De LellisSchool of MathematicsInstitute for Advanced StudyEinstein DriveSimonyi HallPrinceton, NJ 08540, USAe-mail: camillo.delellis@math.ias.eduGiuseppe MingioneDipartimento di Matematica e InformaticaUniversità degli Studi di ParmaParco Area delle Scienze, 53/a (Campus)43124 Parma, Italye-mail: giuseppe.mingione@math.unipr.itMario PulvirentiDipartimento di MatematicaUniversità di Roma “La Sapienza”P.le A. Moro 200185 Roma, Italye-mail: pulvirenti@mat.uniroma1.itFulvio RicciScuola Normale Superiore di PisaPiazza dei Cavalieri 756126 Pisa, Italye-mail: fricci@sns.itValentino TosattiNorthwestern UniversityDepartment of Mathematics2033 Sheridan RoadEvanston, IL 60208, USAe-mail: tosatti@math.northwestern.eduCorinna UlcigraiForschungsinstitut für MathematikHG G 44.1Rämistrasse 1018092 Zürich, Switzerlande-mail: corinna.ulcigrai@bristol.ac.ukThe Editorial Policy can be foundat the back of the volume.

Edoardo Ballico Alessandra Bernardi Iacopo Carusotto Sonia Mazzucchi Valter MorettiEditorsQuantum Physicsand Geometry123

EditorsEdoardo BallicoDipartimento di MatematicaUniversità di TrentoTrento, ItalyAlessandra BernardiDipartimento di MatematicaUniversità di TrentoTrento, ItalyIacopo CarusottoBEC CenterINO-CNRTrento, ItalySonia MazzucchiDipartimento di MatematicaUniversità di TrentoTrento, ItalyValter MorettiDipartimento di MatematicaUniversità di TrentoTrento, ItalyISSN 1862-9113ISSN 1862-9121 (electronic)Lecture Notes of the Unione Matematica ItalianaISBN 978-3-030-06121-0ISBN 978-3-030-06122-7 brary of Congress Control Number: 2019932799Mathematics Subject Classification (2010): Primary: 81-XX, Secondary: 14-XX Springer Nature Switzerland AG 2019This work is subject to copyright. All rights are reserved by the Publisher, whether the whole or part ofthe material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation,broadcasting, reproduction on microfilms or in any other physical way, and transmission or informationstorage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodologynow known or hereafter developed.The use of general descriptive names, registered names, trademarks, service marks, etc. in this publicationdoes not imply, even in the absence of a specific statement, that such names are exempt from the relevantprotective laws and regulations and therefore free for general use.The publisher, the authors and the editors are safe to assume that the advice and information in this bookare believed to be true and accurate at the date of publication. Neither the publisher nor the authors orthe editors give a warranty, express or implied, with respect to the material contained herein or for anyerrors or omissions that may have been made. The publisher remains neutral with regard to jurisdictionalclaims in published maps and institutional affiliations.This Springer imprint is published by the registered company Springer Nature Switzerland AGThe registered company address is: Gewerbestrasse 11, 6330 Cham, Switzerland

Contents1Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .Edoardo Ballico, Alessandra Bernardi, Iacopo Carusotto,Sonia Mazzucchi, and Valter Moretti2 A Very Brief Introduction to Quantum Computingand Quantum Information Theory for Mathematicians . . . . . . . . . . . . . . . .Joseph M. Landsberg153 Entanglement, CP-Maps and Quantum Communications . . . . . . . . . . . . . .Davide Pastorello434 Frontiers of Open Quantum System Dynamics. . . . . . . . . . . . . . . . . . . . . . . . .Bassano Vacchini715 Geometric Constructions over C and F2 for Quantum Information . . .Frédéric Holweck876 Hilbert Functions and Tensor Analysis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 125Luca Chiantini7 Differential Geometry of Quantum States, Observablesand Evolution . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 153F. M. Ciaglia, A. Ibort, and G. Marmov

ContributorsEdoardo Ballico Dipartimento di Matematica, Università di Trento, Trento, ItalyAlessandra Bernardi Dipartimento di Matematica, Università di Trento, Trento,ItalyIacopo Carusotto BEC Center, INO-CNR, Trento, ItalyLuca Chiantini Dipartimento di Ingegneria dell’Informazione e Scienze Matematiche, Università di Siena, Siena, ItalyF. M. Ciaglia Sezione INFN di Napoli and Dipartimento di Fisica E. Pancinidell’Universitá Federico II di Napoli, Complesso Universitario di Monte S. Angelo,Naples, ItalyFrédéric Holweck Laboratoire Interdisciplinaire Carnot de Bourgogne, UniversityBourgogne Franche-Comté, Belfort, FranceA. Ibort ICMAT, Instituto de Ciencias Matemáticas (CSIC-UAM-UC3M-UCM)and Depto. de Matemáticas, Univ. Carlos III de Madrid, Leganés, Madrid, SpainJoseph M. Landsberg Department of Mathematics, Texas A&M University,College Station, TX, USAG. Marmo Sezione INFN di Napoli and Dipartimento di Fisica E. Pancinidell’Universitá Federico II di Napoli, Complesso Universitario di Monte S. Angelo,Naples, ItalySonia Mazzucchi Dipartimento di Matematica, Università di Trento, Trento, ItalyValter Moretti Dipartimento di Matematica, Università di Trento, Trento, ItalyDavide Pastorello Department of Mathematics, University of Trento, TrentoInstitute for Fundamental Physics and Applications (TIFPA), Povo, Trento, ItalyBassano Vacchini Dipartimento di Fisica “Aldo Pontremoli”, Università degliStudi di Milano, Milan, ItalyINFN, Sezione di Milano, Milan, Italyvii

Chapter 1IntroductionEdoardo Ballico, Alessandra Bernardi, Iacopo Carusotto,Sonia Mazzucchi, and Valter MorettiThe development of quantum mechanics has been one of the greatest scientificachievements of the early twentieth century. In spite of its remarkable success inexplaining and predicting an amazing number of properties of our physical world, itsinterpretation has raised strong controversies among a wide community of scientistsand philosophers. One of the hottest points of discussion is the meaning of the socalled quantum entanglement that, for systems of two or many particles, allows inparticular the possibility for each particle of the system to be simultaneously locatedat different spatial positions. Entangled states display a special kind of correlations.Generally speaking, differently from the statistical correlations that are usuallyfound in classical probability theory, quantum entanglement cannot be understood interms of statistically distributed hidden variables and must involve the possibility forquantum systems of particles to be simultaneously in different single particle purequantum states. Entangled states therefore present facets of the quantum worldswhich are even more complicated than the famous example of a superposition ofstates in the so-called Schrödinger’s cat which is simultaneously classically deadand alive. The peculiar phenomenology of quantum mechanics goes far beyondthis paradoxical case: in contrast to the usual chain rules of classical conditionalprobability, the probability for a physical event to occur in a quantum frameworkE. Ballico · A. Bernardi ( )Dipartimento di Matematica, Università di Trento, Trento, Italye-mail: edoardo.ballico@unitn.it; alessandra.bernardi@unitn.itI. CarusottoBEC Center, INO-CNR, Trento, Italye-mail: iacopo.carusotto@unitn.itS. Mazzucchi · V. MorettiDipartimento di Matematica, Università di Trento, Trento, Italye-mail: sonia.mazzucchi@unitn.it; valter.moretti@unitn.it Springer Nature Switzerland AG 2019E. Ballico et al. (eds.), Quantum Physics and Geometry,Lecture Notes of the Unione Matematica Italiana 25,https://doi.org/10.1007/978-3-030-06122-7 11

2E. Ballico et al.is computed by the interference of the complex-valued amplitudes correspondingto the different classical states. In dynamical processes, these classical positionalstates are described by paths that the system can follow during its evolution. Thisdescription of the physical world is commonly known as Feynman integral andimplicitly requires that the system be simultaneously in different classical statesat all intermediate times [1]. The mathematical counterpart of this picture is thatquantum states of a composite system are described by a tensor product structurewhere each product entry represents a component of the system. In this picture,entanglement is encoded in quantum superpositions, that is linear combinationsof completely decomposed tensors. In this sense, if the tensor product involvesdifferent states of a given component which are localized in far and causallyseparated spatial regions, a single component of the system may be simultaneouslylocated in different places.While the observable consequences of quantum mechanics have been experimentally explored all along the twentieth century, starting from the discreteenergy levels of the hydrogen atom towards superconductivity and superfluidityin quantum condensed matter physics and precision measurements in quantumrelativistic particle physics, the most basic and profound features of entanglementand its philosophical consequences have started being investigated only much morerecently. A crucial step in this development was the formulation in 1935 of the socalled Einstein-Podolsky-Rosen (EPR) paradox raising doubts on the completenessof the quantum mechanical description of the physical world [2] in view of theexistence of entangled states in the formalism of quantum theory and the Ludersvon Neumann postulate on the instantaneous collapse of the wavefunction after ameasurement procedure. The subsequent derivation in 1964 of the so-called Bellinequalities [3] was the milestone, which offered a quantitative criterion to testquantum mechanics against alternative hidden variable theories satisfying a localrealism principle and essentially ruling out entangled states as proposed in theEPR paper. So far, the outcome of all experiments carried out along these linesstarting from Aspect’s 1982 one on cascaded photon emission [4] has been astrong confirmation of the predictions of quantum mechanics predicting violationof Bell’s inequalities and ruling out the local realism principle. In the followingyears, the experiments have been gradually improved to better deal with varioushidden assumptions or loopholes pointed out by various scientists. In 2015, for thefirst time, the violation of Bell’s inequalities was corroborated by an experimentaltest of Bell’s theorem by R. Hanson et al. certifying the absence of any additionalassumptions or loophole [5].In addition to a revolution in our philosophical understanding of the physicalworld around us, the success of quantum mechanics in describing these amazingfeatures of the microscopic world has then given a dramatic boost into theexploration of their possible use in technological applications, e.g. to the quantumcommunication and quantum information processing, two new branches of sciencebased on a dramatic change in perspective in logics and computation. As onecan easily imagine, this paradigm shift is accompanied by the need of newmathematical and computer science tools for the description and the control of

1 Introduction3quantum mechanical systems and, more practically, for the full exploitation of thenew possibilities opened by entanglement for communication and computation.This special volume was prepared in the wake of the “International workshop on Quantum Physics and Geometry” organized during July 2017 in LevicoTerme (Trento, Italy) (http://www.science.unitn.it/ carusott/QUANTUMGEO17/index.html) on these topics. This event, sponsored by CIRM with the precioussupport of INDAM, University of Trento, TIFPA-INFN and the INO-CNR BECCenter gathered world specialists in both physical sciences and in mathematics, withthe aim of exploring possible interdisciplinary links between quantum informationand geometry and contributing to the creation of a community of researcherstrying to export advanced mathematical concepts to this new applicative field. Theobjective was to convey to a single event leading experts from the two fields, soto explore interdisciplinary connections and contribute establishing an active andlong-lasting community. On the physics side, a conductive thread of the eventhas been the characterization of entanglement; on the mathematics one, differenttools to describe it from different perspectives have been covered, including tensordecomposition, the classification of the orbit closures of some Lie groups, tensornetwork representations, and topological properties of the quantum states. Thearticles that follow give a hint of the rich developments that one may expect toresult from this meeting of different worlds. While all contributions present excitingstate-of-the-art results, they are also meant to offer a general, mathematics-orientedintroduction to quantum science and technologies and to their latest developments.The first contribution by J.M. Landsberg on “A very brief introduction toquantum computing and quantum information theory for mathematicians” summarizes the PhD course on “Quantum Information and Geometry” that he hasgiven at Trento University with the support of INDAM during the months ofJune and July 2017 surrounding the Levico workshop. In combination with therecorded lectures that are available under request (https://drive.google.com/open?id 0B2Y1CpIKbFuSR1hVT3BfNmtTSFU), this long article aims at giving a complete coverage of the background material from both physics and computer science.The contribution by D. Pastorello on “Entanglement, CP-maps and quantumcommunications” reviews basic concepts of quantum mechanics and entanglementand then focuses on the potential of quantum entanglement as a resource incommunication systems. The contribution by B. Vacchini on “Frontiers of openquantum system dynamics” presents important developments on the dynamics ofquantum systems coupled to environments, which generalize to a wider context thequantum evolution in terms of the well-known Schrödinger equation. Mathematicalresults on the use of advanced geometrical concepts in quantum information theoryare presented in the contribution by F. Holweck on “Geometric constructions overC and F2 for Quantum Information”, with a special attention to the entanglementof pure multipartite systems and to contextuality issues [6]. In both problems,a central role is played by representation theory, which is respectively used toclassify entanglement in terms of the closure diagram of the orbits in tensorspaces and for the description of commutation relations of the generalized N-qubitPauli group. The contribution by L. Chiantini on “Hilbert functions and tensor

4E. Ballico et al.analysis” illustrates the power of geometric methods for the decomposition oftensors and, in particular, offers a survey-style introduction to the important problemof the uniqueness of the decomposition (the so called “identifiability”), useful forsignal processing and, possibly, for the representation of quantum states of manyindistinguishable particles. As a final point, some extension to the famous Kruskal’scriterion is proposed. Finally, the contribution by M. Ciaglia, A. Ibort and G.Marmo on “Differential Geometry of Quantum States, Observables and Evolution”summarizes an alternative geometric description of quantum mechanical systems interms of the Kähler geometry of the space of pure states of a closed quantum systemand discusses how the composition of systems and the resulting entanglement canbe captured in this new setting.We hope that this volume will trigger an active interest from the mathematicalcommunity towards the exciting challenges that quantum science and technology israising to scientists of all disciplines.References1. R.P. Feynman, QED: The Strange Theory of Light and Matter (Princeton University Press,Princeton, 2006)2. A. Einstein, B. Podolsky, N. Rosen, Can quantum-mechanical description of physical reality beconsidered complete? Phys. Rev. 47, 777 (1935)3. J.S. Bell, Speakable and Unspeakable in Quantum Mechanics (Cambridge University Press,Cambridge, 1987)4. A. Aspect, P. Grangier, G. Roger, Experimental realization of Einstein-Podolsky-Rosen-BohmGedankenexperiment: a new violation of Bell’s inequalities. Phys. Rev. Lett. 49, 91 (1982)5. R. Hanson et al., Loophole-free Bell inequality violation using electron spins separated by 1.3kilometers. Nature 526, 682 (2015)6. S. Kochen, E.P. Specker, The problem of hidden variables in quantum mechanics, in The LogicoAlgebraic Approach to Quantum Mechanics (Springer, Dordrecht, 1975), pp. 293–328

Chapter 2A Very Brief Introduction to QuantumComputing and Quantum InformationTheory for MathematiciansJoseph M. LandsbergAbstract This is a very brief introduction to quantum computing and quantuminformation theory, primarily aimed at geometers. Beyond basic definitions andexamples, I emphasize aspects of interest to geometers, especially connections withasymptotic representation theory. Proofs can be found in standard references such asKitaev et al. (Classical and quantum computation, vol. 47. American MathematicalSociety, Providence, 2002) and Nielson and Chuang (Quantum computation andquantum information. Cambridge University Press, Cambridge, 2000) as well asLandsberg (Quantum computation and information: Notes for fall 2017 TAMUclass, 2017).2.1 OverviewI begin, in Sect. 2.2, by presenting the postulates of quantum mechanics as a naturalgeneralization of probability theory. In Sect. 2.3 I describe basic entanglementphenomena of “super dense coding”, “teleportation”, and Bell’s confirmation of the“paradox” proposed by Einstein-Podolsky-Rosen. In Sect. 2.4 I outline aspects ofthe basic quantum algorithms, emphasizing the geometry involved. Section 2.5 is adetour into classical information theory, which is the basis of its quantum cousinbriefly discussed in Sect. 2.7. Before that, in Sect. 2.6, I reformulate quantum theoryin terms of density operators, which facilitates the discussion of quantum information theory. Critical to quantum information theory is von Neumann entropy and inSect. 2.8 I elaborate on some of its properties. A generalization of “teleportation”is discussed in Sec

e-mail:cilibert@axp.mat.uniroma2.it SusannaTerracini (Co-editorinChief) . The publisher, the authors and the editors are safe to assume that the advice and information in this book are believed to be true and accurate at the date of publication. Neither the publisher nor the authors or the editors give a warranty, express or implied, with .

Related Documents:

For example, quantum cryptography is a direct application of quantum uncertainty and both quantum teleportation and quantum computation are direct applications of quantum entanglement, the con-cept underlying quantum nonlocality (Schro dinger, 1935). I will discuss a number of fundamental concepts in quantum physics with direct reference to .

The Quantum Nanoscience Laboratory (QNL) bridges the gap between fundamental quantum physics and the engineering approaches needed to scale quantum devices into quantum machines. The team focuses on the quantum-classical interface and the scale-up of quantum technology. The QNL also applies quantum technology in biomedicine by pioneering new

According to the quantum model, an electron can be given a name with the use of quantum numbers. Four types of quantum numbers are used in this; Principle quantum number, n Angular momentum quantum number, I Magnetic quantum number, m l Spin quantum number, m s The principle quantum

1. Quantum bits In quantum computing, a qubit or quantum bit is the basic unit of quantum information—the quantum version of the classical binary bit physically realized with a two-state device. A qubit is a two-state (or two-level) quantum-mechanical system, one of the simplest quantum systems displaying the peculiarity of quantum mechanics.

terpretation of quantum physics. It gives new foundations that connect all of quantum physics (including quantum mechanics, statistical mechanics, quantum field theory and their applications) to experiment. Quantum physics, as it is used in practice, does much more than predicting probabili

Physics 20 General College Physics (PHYS 104). Camosun College Physics 20 General Elementary Physics (PHYS 20). Medicine Hat College Physics 20 Physics (ASP 114). NAIT Physics 20 Radiology (Z-HO9 A408). Red River College Physics 20 Physics (PHYS 184). Saskatchewan Polytechnic (SIAST) Physics 20 Physics (PHYS 184). Physics (PHYS 182).

Quantum computing is a subfield of quantum information science— including quantum networking, quantum sensing, and quantum simulation—which harnesses the ability to generate and use quantum bits, or qubits. Quantum computers have the potential to solve certain problems much more quickly t

1.3.7 Example: quantum teleportation 26 1.4 Quantum algorithms 28 1.4.1 Classical computations on a quantum computer 29 1.4.2 Quantum parallelism 30 1.4.3 Deutsch's algorithm 32 1.4.4 The Deutsch-Jozsa algorithm 34 1.4.5 Quantum algorithms summarized 36 1.5 Experimental quantum information processing 42 1.5.1 The Stern-Gerlach experiment 43