Resolvent Positive Linear Operators Exhibit the Reduction Phenomenon

Total Page:16

File Type:pdf, Size:1020Kb

Resolvent Positive Linear Operators Exhibit the Reduction Phenomenon Resolvent positive linear operators exhibit the reduction phenomenon Lee Altenberg1 Associate Editor, BioSystems, 2605 Lioholo Place, Kihei, HI 96753-7118 Edited by Joel E. Cohen, The Rockefeller University, New York, NY, and approved December 6, 2011 (received for review August 23, 2011) The spectral bound, sðαA þ βVÞ, of a combination of a resolvent xðt þ 1Þ¼½ð1 − αÞI þ αPDxðtÞ; [1] positive linear operator A and an operator of multiplication V, was shown by Kato to be convex in β ∈ R. Kato's result is shown where xðtÞ is a vector of the rare allele’s frequency at time t among here to imply, through an elementary “dual convexity” lemma, that different population subdivisions, α is the rate of dispersal be- sðαA þ βVÞ is also convex in α > 0, and notably, ∂sðαA þ βVÞ∕ tween subdivisions, P is the stochastic matrix representing the ∂α ≤ sðAÞ. Diffusions typically have sðAÞ ≤ 0, so that for diffusions pattern of dispersal, and D is a diagonal matrix of the growth rates with spatially heterogeneous growth or decay rates, greater mix- of the allele in each subdivision. The allele is protected from ing reduces growth. Models of the evolution of dispersal in parti- extinction if its asymptotic growth rate when rare is greater than cular have found this result when A is a Laplacian or second-order 1. This asymptotic growth rate is the spectral radius, elliptic operator, or a nonlocal diffusion operator, implying selec- tion for reduced dispersal. These cases are shown here to be part rðAÞ≔ supfjλj: λ ∈ σðAÞg; [2] of a single, broadly general, “reduction” phenomenon. where σðAÞ is the set of eigenvalues of matrix A. perturbation theory ∣ positive semigroup ∣ reduction principle ∣ Karlin discovered that for MðαÞ≔½ð1 − αÞI þ αP, the spectral non-self-adjoint ∣ Schrödinger operator radius, rðMðαÞDÞ, is a decreasing function of the dispersal rate α, for arbitrary strongly connected dispersal pattern: he main result to be shown here is that the growth bound, TωðαA þ VÞ, of a positive semigroup generated by αA þ V Theorem 1. (Karlin's Theorem 5.2) [(16), pp. 194–196] Let P be changes with positive scalar α at a rate less than or equal to ωðAÞ, an arbitrary nonnegative irreducible stochastic matrix. Consider where A is also a generator, and V is an operator of multiplica- the family of matrices tion. Movement of a reactant in a heterogeneous environment is M α 1 − α I αP; 0 < α < 1. often of this form, where V represents the local growth or decay ð Þ¼ð Þ þ α rate, and represents the rate of mixing. Lossless mixing means Then for any diagonal matrix D with positive terms on the diagonal, ω 0 ω 0 ðAÞ¼ , while lossy mixing means ðAÞ < , so this result im- the spectral radius plies that greater mixing reduces the reactant’s asymptotic growth rate, or increases its asymptotic decay rate. Decreased growth or rðαÞ¼rðMðαÞDÞ increased decay are familiar results when A is a diffusion opera- α D ≠ I tor, so what is new here is the generality shown for this phenom- is decreasing as increases (strictly provided d ). ’ enon. At the root of this result is a theorem by Kingman on the Karlin s Theorem 5.2 means that greater mixing between sub- M α D “superconvexity” of the spectral radius of nonnegative matrices divisions produces lower rð ð Þ Þ, and if it goes below 1, the (1). The logical route progresses from Kingman through Cohen allele will go extinct. While this theorem was motivated by the (2) to Kato (3). The historical route begins in population genetics. issue of genetic diversity in a subdivided population, its form ap- In early theoretical work to understand the evolution of genet- plies generally to situations where differential growth is combined D ic systems, Feldman, colleagues, and others kept finding a com- with mixing. could just as well represent the investment returns P D mon result from each model they examined (4–14)—be they on different assets and a pattern of portfolio rebalancing. Or models for the evolution of recombination, or of mutation, or could represent the decay rates of reactant in different parts of a P of dispersal. Evolution favored reduced levels of these processes reactor, and a pattern of stirring within the reactor. In a very in populations near equilibrium under constant environments, general interpretation, Theorem 5.2 means that greater mixing and this result was called the Reduction Principle (11). reduces growth and hastens decay. α MATHEMATICS These results were found for finite-dimensional models. But If the dispersal rate is not an extrinsic parameter, but is a the same reduction result has also been found in models for variable which is itself controlled by a gene, then a gene which α the evolution of unconditional dispersal in continuous space, in decreases will have a growth advantage over its competitor which matrices are replaced by linear operators. This finding alleles. The action of such modifier genes produces a process raises the questions of whether this common result, discovered that will reduce the rates of dispersal in a population. Therefore, in such a diversity of models, reflects a single mathematical phe- Theorem 5.2 also means that differential growth selects for reduced nomenon. Here, the question is answered affirmatively. mixing. The mathematical underpinnings of the reduction principle In the evolutionary context, the generality of the mixing pat- P ’ for finite-dimensional models were discovered by Sam Karlin tern in Karlin s Theorem 5.2 makes it applicable to other kinds POPULATION BIOLOGY (15, 16) [although he did not realize it, and he had earlier pro- posed an alternate to the reduction principle—the mean fitness Dedicated to Sir John F. C. Kingman on the fiftieth anniversary of his theorem on the principle (17), which was found to have counterexamples (18)]. “superconvexity” of the spectral radius (1), which is at the root of the results presented Karlin wanted to understand the effect of population subdivision here. on the maintenance of genetic variation. Genetic variation is Author contributions: L.A. designed research, performed research, and wrote the paper. preserved if an allele has a positive growth rate when it is rare, The author declares no conflict of interest. protecting it from extinction. The dynamics of a rare allele are This article is a PNAS Direct Submission. approximately linear, and of the form 1E-mail: [email protected]. www.pnas.org/cgi/doi/10.1073/pnas.1113833109 PNAS ∣ March 6, 2012 ∣ vol. 109 ∣ no. 10 ∣ 3705–3710 Downloaded by guest on September 27, 2021 of “mixing” besides dispersal. The pattern matrix P can just as BðXÞ represents the set of all bounded linear operators well refer to the pattern of mutations between genotypes, and A: X → X. α P ⊂ then refers to the mutation rate. Or can represent the pattern A is a positive operator if AXþ X þ. of transmission when two loci recombine, and then α represents The resolvent of A is Rðξ;AÞ≔ðξ − AÞ−1, the operator inverse of the recombination rate. The early models for the evolution of ξ − A, ξ ∈ C. recombination and mutation that exhibited the reduction princi- The resolvent set ρðAÞ ⊂ C are those values of ξ for which ple in fact had the same form as Eq. 1 for the dynamics of a rare ξ − A is invertible. modifier allele. Once this commonality of form was recognized The spectrum of A ∈ BðXÞ, σðAÞ, is the complement of the (19–21), it was clear that Karlin’s theorem explained the repeated resolvent set, ρðAÞ. appearance of the reduction result in the different contexts, and The spectral bound of closed linear operator A, not necessarily generalized the result to a whole class of genetic transmission bounded, is patterns beyond the special cases that had been analyzed. The dynamics of movement in space have been long modeled supfReðλÞ: λ ∈ σðAÞg if σðAÞ ≠ ∅ sðAÞ≔ : by infinite-dimensional models, where space is continuous and −∞ if σðAÞ¼∅ the concentrations of a quantity at each point are represented as a function. The dynamics of change in the concentration are The type (growth bound) of an infinitesimal generator, A,ofa modeled as diffusions, where the Laplacian or elliptic differential tA 0 operator or nonlocal integral operator takes the place of the strongly continuous (C0) semigroup, fe : t> g,is matrix P in the finite-dimensional case. When the substance 1 grows or decays at rates that are a function of its location, the ωðAÞ≔lim log ∥etA∥ ¼ log rðeAÞ: t→∞ t system is often referred to as a reaction diffusion. In reaction- diffusion models for the evolution of dispersal, the reduction Generally, −∞ ≤ sðAÞ ≤ ωðAÞ < ∞, but conditions for principle again makes its appearance (22) (23, Lemma 5.2) (24, sðAÞ¼ωðAÞ or sðAÞ < ωðAÞ are part of a more involved theory Lemma 2.1) (25). In nonlocal diffusion models, again the reduc- for the asymptotic growth of semigroups (see refs. 36–38). tion principle appears (26). This repeated occurrence points to the possibility of an underlying mathematical unity. Here, a broad characterization of this “reduction phenomen- Definition 1: Operator A is resolvent positive if there is ξ0 such that on” is established by generalizing Karlin’s theorem to linear ðξ0;∞Þ ⊂ ρðAÞ and Rðξ;AÞ is positive for all ξ > ξ0 (39). operators. The reduction results previously found for various The relationship of the resolvent positive property to other linear operators are, therefore, seen to be special cases of a familiar operator properties includes the following list of key general phenomenon. This result is actually implicit in Kato’s generalization (3) of results: Cohen’s theorem (2) on the convexity of the spectral bound of ≥ 1.
Recommended publications
  • Criss-Cross Type Algorithms for Computing the Real Pseudospectral Abscissa
    CRISS-CROSS TYPE ALGORITHMS FOR COMPUTING THE REAL PSEUDOSPECTRAL ABSCISSA DING LU∗ AND BART VANDEREYCKEN∗ Abstract. The real "-pseudospectrum of a real matrix A consists of the eigenvalues of all real matrices that are "-close to A. The closeness is commonly measured in spectral or Frobenius norm. The real "-pseudospectral abscissa, which is the largest real part of these eigenvalues for a prescribed value ", measures the structured robust stability of A. In this paper, we introduce a criss-cross type algorithm to compute the real "-pseudospectral abscissa for the spectral norm. Our algorithm is based on a superset characterization of the real pseudospectrum where each criss and cross search involves solving linear eigenvalue problems and singular value optimization problems. The new algorithm is proved to be globally convergent, and observed to be locally linearly convergent. Moreover, we propose a subspace projection framework in which we combine the criss-cross algorithm with subspace projection techniques to solve large-scale problems. The subspace acceleration is proved to be locally superlinearly convergent. The robustness and efficiency of the proposed algorithms are demonstrated on numerical examples. Key words. eigenvalue problem, real pseudospectra, spectral abscissa, subspace methods, criss- cross methods, robust stability AMS subject classifications. 15A18, 93B35, 30E10, 65F15 1. Introduction. The real "-pseudospectrum of a matrix A 2 Rn×n is defined as R n×n (1) Λ" (A) = fλ 2 C : λ 2 Λ(A + E) with E 2 R ; kEk ≤ "g; where Λ(A) denotes the eigenvalues of a matrix A and k · k is the spectral norm. It is also known as the real unstructured spectral value set (see, e.g., [9, 13, 11]) and it can be regarded as a generalization of the more standard complex pseudospectrum (see, e.g., [23, 24]).
    [Show full text]
  • On the Linear Stability of Plane Couette Flow for an Oldroyd-B Fluid and Its
    J. Non-Newtonian Fluid Mech. 127 (2005) 169–190 On the linear stability of plane Couette flow for an Oldroyd-B fluid and its numerical approximation Raz Kupferman Institute of Mathematics, The Hebrew University, Jerusalem, 91904, Israel Received 14 December 2004; received in revised form 10 February 2005; accepted 7 March 2005 Abstract It is well known that plane Couette flow for an Oldroyd-B fluid is linearly stable, yet, most numerical methods predict spurious instabilities at sufficiently high Weissenberg number. In this paper we examine the reasons which cause this qualitative discrepancy. We identify a family of distribution-valued eigenfunctions, which have been overlooked by previous analyses. These singular eigenfunctions span a family of non- modal stress perturbations which are divergence-free, and therefore do not couple back into the velocity field. Although these perturbations decay eventually, they exhibit transient amplification during which their “passive" transport by shearing streamlines generates large cross- stream gradients. This filamentation process produces numerical under-resolution, accompanied with a growth of truncation errors. We believe that the unphysical behavior has to be addressed by fine-scale modelling, such as artificial stress diffusivity, or other non-local couplings. © 2005 Elsevier B.V. All rights reserved. Keywords: Couette flow; Oldroyd-B model; Linear stability; Generalized functions; Non-normal operators; Stress diffusion 1. Introduction divided into two main groups: (i) numerical solutions of the boundary value problem defined by the linearized system The linear stability of Couette flow for viscoelastic fluids (e.g. [2,3]) and (ii) stability analysis of numerical methods is a classical problem whose study originated with the pi- for time-dependent flows, with the objective of understand- oneering work of Gorodtsov and Leonov (GL) back in the ing how spurious solutions emerge in computations.
    [Show full text]
  • Proquest Dissertations
    RICE UNIVERSITY Magnetic Damping of an Elastic Conductor by Jeffrey M. Hokanson A THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE Master of Arts APPROVED, THESIS COMMITTEE: IJU&_ Mark Embread Co-chair Associate Professor of Computational and Applied M/jmematics Steven J. Cox, (Co-chair Professor of Computational and Applied Mathematics David Damanik Associate Professor of Mathematics Houston, Texas April, 2009 UMI Number: 1466785 INFORMATION TO USERS The quality of this reproduction is dependent upon the quality of the copy submitted. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleed-through, substandard margins, and improper alignment can adversely affect reproduction. In the unlikely event that the author did not send a complete manuscript and there are missing pages, these will be noted. Also, if unauthorized copyright material had to be removed, a note will indicate the deletion. UMI® UMI Microform 1466785 Copyright 2009 by ProQuest LLC All rights reserved. This microform edition is protected against unauthorized copying under Title 17, United States Code. ProQuest LLC 789 East Eisenhower Parkway P.O. Box 1346 Ann Arbor, Ml 48106-1346 ii ABSTRACT Magnetic Damping of an Elastic Conductor by Jeffrey M. Hokanson Many applications call for a design that maximizes the rate of energy decay. Typical problems of this class include one dimensional damped wave operators, where energy dissipation is caused by a damping operator acting on the velocity. Two damping operators are well understood: a multiplication operator (known as viscous damping) and a scaled Laplacian (known as Kelvin-Voigt damping). Paralleling the analysis of viscous damping, this thesis investigates energy decay for a novel third operator known as magnetic damping, where the damping is expressed via a rank-one self-adjoint operator, dependent on a function a.
    [Show full text]
  • Computation of Pseudospectral Abscissa for Large-Scale Nonlinear
    IMA Journal of Numerical Analysis (2017) 37, 1831–1863 doi: 10.1093/imanum/drw065 Advance Access publication on January 11, 2017 Computation of pseudospectral abscissa for large-scale nonlinear eigenvalue problems Downloaded from https://academic.oup.com/imajna/article-abstract/37/4/1831/2894467 by Koc University user on 20 August 2019 Karl Meerbergen Department of Computer Science, KU Leuven, University of Leuven, Heverlee 3001, Belgium Emre Mengi∗ Department of Mathematics, Ko¸c University, Rumelifeneri Yolu, Sarıyer-Istanbul˙ 34450, Turkey ∗Corresponding author: [email protected] and Wim Michiels and Roel Van Beeumen Department of Computer Science, KU Leuven, University of Leuven, Heverlee 3001, Belgium [Received on 26 June 2015; revised on 21 October 2016] We present an algorithm to compute the pseudospectral abscissa for a nonlinear eigenvalue problem. The algorithm relies on global under-estimator and over-estimator functions for the eigenvalue and singular value functions involved. These global models follow from eigenvalue perturbation theory. The algorithm has three particular features. First, it converges to the globally rightmost point of the pseudospectrum, and it is immune to nonsmoothness. The global convergence assertion is under the assumption that a global lower bound is available for the second derivative of a singular value function depending on one parameter. It may not be easy to deduce such a lower bound analytically, but assigning large negative values works robustly in practice. Second, it is applicable to large-scale problems since the dominant cost per iteration stems from computing the smallest singular value and associated singular vectors, for which efficient iterative solvers can be used.
    [Show full text]
  • Lecture Notes on Spectra and Pseudospectra of Matrices and Operators
    Lecture Notes on Spectra and Pseudospectra of Matrices and Operators Arne Jensen Department of Mathematical Sciences Aalborg University c 2009 Abstract We give a short introduction to the pseudospectra of matrices and operators. We also review a number of results concerning matrices and bounded linear operators on a Hilbert space, and in particular results related to spectra. A few applications of the results are discussed. Contents 1 Introduction 2 2 Results from linear algebra 2 3 Some matrix results. Similarity transforms 7 4 Results from operator theory 10 5 Pseudospectra 16 6 Examples I 20 7 Perturbation Theory 27 8 Applications of pseudospectra I 34 9 Applications of pseudospectra II 41 10 Examples II 43 1 11 Some infinite dimensional examples 54 1 Introduction We give an introduction to the pseudospectra of matrices and operators, and give a few applications. Since these notes are intended for a wide audience, some elementary concepts are reviewed. We also note that one can understand the main points concerning pseudospectra already in the finite dimensional case. So the reader not familiar with operators on a separable Hilbert space can assume that the space is finite dimensional. Let us briefly outline the contents of these lecture notes. In Section 2 we recall some results from linear algebra, mainly to fix notation, and to recall some results that may not be included in standard courses on linear algebra. In Section 4 we state some results from the theory of bounded operators on a Hilbert space. We have decided to limit the exposition to the case of bounded operators.
    [Show full text]
  • Resolvent Conditions for the Control of Parabolic Equations Thomas Duyckaerts, Luc Miller
    Resolvent conditions for the control of parabolic equations Thomas Duyckaerts, Luc Miller To cite this version: Thomas Duyckaerts, Luc Miller. Resolvent conditions for the control of parabolic equations. Jour- nal of Functional Analysis, Elsevier, 2012, 263 (11), pp.3641-3673. 10.1016/j.jfa.2012.09.003. hal- 00620870v2 HAL Id: hal-00620870 https://hal.archives-ouvertes.fr/hal-00620870v2 Submitted on 5 Sep 2012 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. RESOLVENT CONDITIONS FOR THE CONTROL OF PARABOLIC EQUATIONS THOMAS DUYCKAERTS1 AND LUC MILLER2 Abstract. Since the seminal work of Russell and Weiss in 1994, resolvent conditions for various notions of admissibility, observability and controllability, and for various notions of linear evolution equations have been investigated in- tensively, sometimes under the name of infinite-dimensional Hautus test. This paper sets out resolvent conditions for null-controllability in arbitrary time: necessary for general semigroups, sufficient for analytic normal semigroups. For a positive self-adjoint operator A, it gives a sufficient condition for the null-controllability of the semigroup generated by −A which is only logarithmi- cally stronger than the usual condition for the unitary group generated by iA.
    [Show full text]
  • Estimates for the Resolvent and Spectral Gaps for Non Self-Adjoint Operators
    Estimates for the resolvent and spectral gaps for non self-adjoint operators Vesselin Petkov University Bordeaux Mathematics Days in Sofia, July 9, 2014 Vesselin Petkov (University BordeauxEstimates) for the resolvent and spectral gaps for non self-adjoint operators 1 / 29 Outline 1. Holomorphic functions without zeros in a strip. 2. Estimates for (I + B(z))−1. 3. The cut-off resolvent and the scattering operator. 4. Spectral gap for generators of semigroupes. 5. Dynamical zeta function. Vesselin Petkov (University BordeauxEstimates) for the resolvent and spectral gaps for non self-adjoint operators 2 / 29 1. Holomorphic functions without zeros in a strip 1. Holomorphic functions without zeros in a strip We start with the following question. Let f (z) be a holomorphic function in + C = {z ∈ C : Im z > 0} such that for some α ≥ 0, C > 0, M ∈ N we have M α Im z |f (z)| ≤ C(1 + |z|) e , z ∈ C+. (1) i Assume that f (z) 6= 0 in the strip 0 < Im z < 1 and consider z = x + 2 . What is the 1 optimal estimate for |f (x+i/2)| . Theorem 1 (Borichev, -P.) + Let f (z) be a holomorphic function in C satisfying (1). Assume that f (z) 6= 0 for 0 < Im z < 1. Then log |f (x + i/2)| lim = 0. (2) |x|→∞ x 2 It is clear that (2) implies for every 0 < 1 the estimate 1 2 ≤ C e|x| , x ∈ . |f (x + i/2)| R Vesselin Petkov (University BordeauxEstimates) for the resolvent and spectral gaps for non self-adjoint operators 3 / 29 1.
    [Show full text]
  • Newton's Method for Concave Operators with Resolvent Positive
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Linear Algebra and its Applications 363 (2003) 43–64 www.elsevier.com/locate/laa Newton’s method for concave operators with resolvent positive derivatives in ordered Banach spaces T. Damm a,∗, D. Hinrichsen b aZentrum Mathematik, TU München, D-80333 München, Germany bInstitut für Dynamische Systeme, Universität Bremen, D-28334 Bremen, Germany Received 23 March 2001; accepted 13 February 2002 Submitted by R. Nabben Abstract We prove a non-local convergence result for Newton’s method applied to a class of nonlin- ear equations in ordered real Banach spaces. The key tools in our approach are special notions of concavity and the spectral theory of resolvent positive operators. © 2002 Published by Elsevier Science Inc. AMS classification: 65J15; 47J25; 47H07; 15A24 Keywords: Newton’s method; Positive operators; Concave operators; Riccati equation 1. Introduction A standard method to solve nonlinear equations is the Newton iteration. Its appli- cability to operator equations in normed spaces was first established by Kantorovich [16]. In the operator-theoretic setup the method is therefore often referred to as the Newton–Kantorovich procedure. Kantorovich specified boundedness conditions on the first and second Fréchet derivatives of the nonlinear operator, which guarantee convergence of the Newton iteration starting in a small neighbourhood of the actual solution. These results can be simplified and generalized, if the underlying space is ordered and the sequence produced by the iteration can be shown to be monotonic ∗ Corresponding author. E-mail addresses: [email protected] (T.
    [Show full text]
  • Eventually, Essentially and Exponentially Nonnegative Matrices
    1 Some notation and definitions Given an n × n matrix A, the spectrum of A is denoted by σ(A) and its spectral radius by ρ(A) = maxfjλj j λ 2 σ(A)g. An eigenvalue λ of A is said to be dominant if jλj = ρ(A). The spectral abscissa of A is defined and denoted by λ(A) := maxfRe λ j λ 2 σ(A)g. 2 Eventually nonnegative states and matrices In the theory and applications of dynamical systems, one is frequently interested in qual- itative information regarding state evolution. In particular, due to physical and modeling constraints arising in engineering, biological, medical and economic applications, it is com- monly of interest to impose or consider conditions for nonnegativity of the states; see, e.g., [6, 17]. Such applications typically draw on the theory, or even directly take the form of a linear differential system n×n n x_(t) = Ax(t);A 2 R ; x(0) = x0 2 R ; t ≥ 0; (2.1) tA whose solution is given by x(t) = e x0. We shall refer here to the set tA fx(t) = e x0 j t 2 [0; 1)g as the trajectory emanating from x0 and say that x0 gives rise to this trajectory. It is proposed that we consider conditions for the entrywise nonnegativity of the trajectories associated with (2.1). A main concern is the following `hit and hold' problem: When does the trajectory emanating from an initial point x0 become (entrywise) nonnegative and remain nonnegative for all time thereafter? More specifically, we propose to seek characterizations of system parameters that lead to n a trajectory becoming nonnegative at a finite time (reachability of R+) and remaining 1 n nonnegative for all time thereafter (holdability of R+).
    [Show full text]
  • Arxiv:Quant-Ph/0302028V1 4 Feb 2003 .Muodain,Mte .A Ai,Admsiiin .Sa F
    Quantum Tomography G. Mauro D’Ariano, Matteo G. A. Paris, and Massimiliano F. Sacchi February 1, 2008 arXiv:quant-ph/0302028v1 4 Feb 2003 Contents 1 Introduction 4 2 Wigner functions and elements of detection theory 8 2.1 Wignerfunctions ........................... 8 2.2 Photodetection ............................ 11 2.3 Balancedhomodynedetection . 13 2.4 Heterodynedetection . 16 3 General tomographic method 20 3.1 Briefhistoricalexcursus . 21 3.2 Conventionaltomographicimaging . 22 3.2.1 Extensiontothequantumdomain . 23 3.3 Generalmethodofquantumtomography . 24 3.3.1 Basicstatistics .. .. .. .. .. .. .. .. .. .. 24 3.3.2 Characterizationofthequorum . 26 3.3.3 Quantum estimation for harmonic-oscillator systems ... 28 3.3.4 Somegeneralizations. 31 3.3.5 Quantumestimationforspinsystems . 32 3.3.6 Quantum estimation for a free particle . 34 3.4 Noise deconvolution and adaptive tomography . 34 3.4.1 Noisedeconvolution . 34 3.4.2 Adaptivetomography . 36 4 Universal homodyning 38 4.1 Homodyningobservables. 38 4.2 Noiseintomographicmeasurements . 41 4.2.1 Field-Intensity .. .. .. .. .. .. .. .. .. .. 42 4.2.2 RealField........................... 43 4.2.3 Fieldamplitude.. .. .. .. .. .. .. .. .. .. 43 4.2.4 Phase ............................. 44 4.3 Comparison between homodyne tomography and heterodyning . 47 1 5 Multimode homodyne tomography 49 5.1 Thegeneralmethod ......................... 50 5.1.1 Numerical results for two-mode fields . 53 6 Applications to quantum measurements 59 6.1 Measuring the nonclassicality of a quantum state . ... 59 6.1.1 Single-modenonclassicality . 60 6.1.2 Two-modenonclassicality . 63 6.2 Testofstatereduction . 64 6.3 Tomography of coherent signals and applications . ... 68 7 Tomography of a quantum device 74 7.1 Themethod.............................. 75 7.2 Anexampleintheopticaldomain . 76 8 Maximum-likelihood method in quantum estimation 79 8.1 Maximum likelihood principle .
    [Show full text]
  • EVENTUAL CONE INVARIANCE∗ 1. Introduction. Perron-Frobenius
    Electronic Journal of Linear Algebra, ISSN 1081-3810 A publication of the International Linear Algebra Society Volume 32, pp. 204-216, July 2017. EVENTUAL CONE INVARIANCE∗ MICHAEL KASIGWAy AND MICHAEL J. TSATSOMEROSy Abstract. Eventually nonnegative matrices are square matrices whose powers become and remain (entrywise) nonnegative. Using classical Perron-Frobenius theory for cone preserving maps, this notion is generalized to matrices whose powers eventually n m leave a proper cone K ⊂ R invariant, that is, A K ⊆ K for all sufficiently large m. Also studied are the related notions of eventual cone invariance by the matrix exponential, as well as other generalizations of M-matrix and dynamical system notions. Key words. Eventually nonnegative matrix, Exponentially nonnegative matrix, Perron-Frobenius, Proper cone. AMS subject classifications. 15A48, 93B03. 1. Introduction. Perron-Frobenius theory commonly refers to the study of square (entrywise) non- negative matrices A. The name reflects the basic properties of such matrices, which are the tenets of the celebrated Perron-Frobenius theorem; that is, in its simplest form, the spectral radius is necessarily an eigen- value of A corresponding to a nonnegative eigenvector. More generally, however, Perron-Frobenius theory encompasses the study of matrices A that leave a proper cone K ⊂ Rn invariant, namely AK ⊆ K. This in- n deed generalizes nonnegative matrices, which leave the nonnegative orthant, R+, invariant. One can include in this area the study of functionals and operators in finite or infinite dimensions, in contexts where the main tenets of the Perron-Frobenius theory apply. One such instance is the study of eventually nonnegative matrices A, namely, matrices for which Am is nonnegative for all sufficiently large m.
    [Show full text]
  • Eventual Cone Invariance
    EVENTUAL CONE INVARIANCE By MICHAEL KASIGWA A dissertation submitted in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY WASHINGTON STATE UNIVERSITY Department of Mathematics JULY 2017 To the Faculty of Washington State University: The members of the Committee appointed to examine the dissertation of MICHAEL KASIGWA find it satisfactory and recommend that it be accepted. Michael Tsatsomeros, Ph.D., Chair Judith McDonald, Ph.D. Nikos Voulgarakis, Ph.D. ii Acknowledgments Thanks to all in the Ndoleriire family for your steadfast love and support, to my adviser for your invaluable guidance and to all the committee members for your support and dedication. iii EVENTUAL CONE INVARIANCE Abstract by Michael Kasigwa, Ph.D. Washington State University July 2017 Chair: Michael Tsatsomeros n If K is a proper cone in R some results in the theory of eventually (entrywise) nonneg- ative matrices have equivalent analogues in eventual K-invariance. We develop these analogues using the classical Perron-Frobenius theory for cone preserving maps. Using an ice-cream cone we n×n demonstrate that unlike the entrywise nonnegative case of a matrix A 2 R , eventual cone invari- ance and eventual exponential cone invariance are not equivalent. The notions of inverse positivity of M-matrices, M-type and Mv-matrices are extended to Mv;K -matrices (operators), that have the form A = sI − B, where B is eventually K-nonnegative, that is, BmK ⊆ K for all sufficiently large m. Eventual positivity of semigroups of linear operators on Banach spaces ordered by a cone can be investigated using resolvents or resolvent type operators constructed from the generators.
    [Show full text]