DOCSLIB.ORG

Measures on Banach Manifolds, Random Surfaces, and Nonperturbative String Field Theory with Cut-Offs

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Measures on Banach Manifolds, Random Surfaces, and Nonperturbative String Field Theory with Cut-Offs MEASURES ON BANACH MANIFOLDS, RANDOM SURFACES, AND NONPERTURBATIVE STRING FIELD THEORY WITH CUT-OFFS JONATHAN WEITSMAN Abstract. We construct a cut-off version of nonpertubative closed Bosonic string field theory in the light-cone gauge with imaginary string coupling constant. We show that the partition function is a continuous function of the string coupling constant, and conjecture a relation between the formal power series expansion of this partition function and Riemann Surfaces. 1. Introduction Recent work of Schnabl [11], confirming conjectures of Sen [12], has given strong evidence for string field theory as a candidate for nonperturbative string theory. This may indicate that string field theory provides a framework for the advances in nonperturbative string theory which have influenced both mathematics and physics. In view of this fact, and of the important role of non- perturbative string theory in mathematics, it seems reasonable to ask to what extent string field theory can be understood mathematically. In this paper we will show that in the simple case of the light cone closed Bosonic string field theory, and once appropriate cut-offs have been introduced, such a mathematical interpretation is possible.∗ 1.1. Free string field theory for the closed Bosonic string: Formal path integrals. Free field theory for the closed Bosonic string in light cone gauge was described by Kaku and Kikkawa y [7]. The string field Ψ(t; `; φ) is formally a complex-valued function of time t 2 R, string length 1 d d ` 2 (0; 1), and a map φ : S ! R , which may be thought of as a loop or \string" in R 1 d z (more properly φ should be considered as a distribution on S with values in R ). In view of the Schrodinger representationx L (S0(S1; ) ⊗ d; dµp ) 'F; 2 R R −(d2=dx2)+m2 (where m > 0; see Appendix A) which identifies functions on distributions on S1 with elements of Fock space F; we may formally think of the string field as a distribution Ψ(t; `) on R × [0; 1) with values in some completion of Fock space. In these terms a cut-off version of Kaku and Kikkawa's [7] formal free string path integral is given by arXiv:0807.2069v1 [math-ph] 14 Jul 2008 D E Z R L1 R 1 d L d` −∞ dt Ψ(t;`); i dt −H`;m Ψ(t;`) (1.1) dΨ e 0 F ; where H`;m is the Hamiltonian on Fock space of mass m > 0 (see Appendix A) and L0;L1; with 0 < L0 < L1 < 1; correspond to the maximum and minimum allowed string lengths. 2000 Mathematics Subject Classification. Primary . Supported in part by NSF grant DMS 04/05670. June 15, 2021. ∗For another mathematical study of string field theory, see Dimock [3]. yIn the light cone gauge this string length appears as the momentum conjugate to the light cone coordinate X+; see [7]. z d+1;1 This model corresponds to a gauge-fixed theory of strings propagating in R ; see e.g. [10]. xIn this paper all vector spaces are complex unless specifically denoted otherwise. 1 2 JONATHAN WEITSMAN To try to interpret an expression of the type (1.1) as a measure, we compute correlation functions. 0 0 1 0 If we take t; t 2 (−∞; 1), g; g 2 C ([L0;L1]), and v; v 2 F, and set Z L1 D E Φv;g;t(Ψ) = g(`) Ψ(t; `); v d`; F L0 then the expression (1.1) gives rise to the formal computation D E R L1 R 1 d Z d` dt Ψ(t;`); i −H`;m Ψ(t;`) L0 −∞ dt (1.2) Φv;g;t(Ψ) Φv0;g0;t0 (Ψ) dΨ e F L1 Z D 0 E = v; e−i(t−t )H`;m v0 θ(t − t0)g(`)g0(`) d`; F L0 where the function θ : R ! R is defined by ( θ(x) = 0 if x < 0; θ(x) = 1 if x ≥ 0: 1.2. Free string field theory for the closed Bosonic string: Mathematical results. In Section 2 we will prove the following result, which may be viewed as a mathematical version of α −α H (1.2). Choose α > 0 and let F = e L0;m F: α Theorem 1. There exists a Banach space B ⊃ H1(R) ⊗ L2([L0;L1]) ⊗ F and a Gaussian prob- 0 0 1 ability measure µ on B such that if v; v 2 F are eigenvectors of H`;m, g; g 2 C ([L0;L1]), and 0 t; t 2 R, the function Φv;g;t : H1(R) ⊗ L2([L0;L1]) ⊗ F ! C, given by Z L1 D E Φv;g;t(f ⊗ h ⊗ w) = f(t) d` h(`)g(`) w; v F L0 extends to an element Φv;g;t 2 Lp(B; dµ) for all p ≥ 1. Furthermore, L1 Z Z D 0 E 0 −|t−t j H`;m 0 (1.3) dµ Φv;g;t Φv0;g0;t0 = d` g(`) g (`) v; e v : F B L0 Remark 1.4. Note that (1.3) differs from (1.2) by the absence of the function θ(t − t0) and by the familiar \Wick rotation" i(t − t0) ! (t − t0). In physical language we have replaced the first order Minkowski action by a second order Euclidean action. This would seem to be necessary to get a reasonable field theory limit; furthermore the first order theory of Kaku and Kikkawa [7] does not produce any vacuum-to-vacuum diagrams in either the free or interacting theories. Our main technique for producing the measure µ is the abstract Wiener space construction of L. Gross [6] (see Appendix B). The path integral description of quantum field theory relates the measure µ to quantities asso- 1 ciated with two dimensional quantum field theory on the Riemann surface S × R as follows. Let 1 0 1 d S` denote the circle of length `, and let dν`;C be the Gaussian measure on S (S` × R; R) ⊗ R with 2 −1 0 1 0 0 1 1 d covariance C = (−∆ + m ) . Then if g; g 2 C ([L0;L1]), t; t 2 R, and f; f 2 C (S ; R) ⊗ R , 1 1 d we may define for 2 C (S` × R; R) ⊗ R Z L1 Z D 1 E Φf;g;t( ) = d` g(`) (s; t); p f(s=`) ds 1 d L0 S` ` R 1 1 d Then the map Φf;g;t : C (S` × R; R) ⊗ R × [L0;L1] ! C extends to a function Φf;g;t 2 Lp(dν`;C × dm[L0;L1]) for all p ≥ 1; NONPERTURBATIVE STRING FIELD THEORY 3 where m[L0;L1] is Lebesgue measure on [L0;L1]: And we have (1.5) q −|t−t0j − 1 (d2=dx2)+m2 Z L1 Z Z L1 `2 1 0 D e 0E d` Φf;g;t Φf 0;g0;t0 dν`;C = d` g(`) g (`) f; f : 0 1 d q L (S1; )⊗ d L0 S (S × ; )⊗ 2 L0 1 2 2 2 2 R R ` R R R − `2 (d =dx ) + m in line with (1.3). 1.3. Interacting String field theory: Formal path integrals. Interacting string field theory is obtained from a cubic function on the space B. We first describe a version of the formal construction 1 d of [7]. We imagine a string { that is, a function φ : S` ! R { breaking up into two loops 1 d φ1 : S`1 ! R 1 d φ2 : S`2 ! R where `1 + `2 = `. In mathematical terms, we have a projection `1;`2 1 d 1 d 1 d (1.6) π` : L2(S ; R) ⊗ R ! (L2(S ; R) ⊗ R ) ⊕ (L2(S ; R) ⊗ R ); giving rise to a map{ `1;`2 (1.7) π` : F ! F ⊗ F and, if we imagine for a moment that the string field Ψ is a function with values in Fock space, we formally obtain a cubic interaction term Z 1 Z L1Z L1 D `1;`2 E (1.8) I(Ψ) = dt d`1 d`2 Ψ(`1; t) ⊗ Ψ(`2; t); π` Ψ(`1 + `2; t) : F −∞ L0 L0 A version of the partition function of the interacting string field theory of [7] is given formally by D E Z R L1 R 1 d L d` −∞ dt Ψ(t;`); i dt −H`;m Ψ(t;`) +λ Re I(Ψ) (1.9) Z(λ) = dΨ e 0 F : The expression (1.9) gives rise to a formal power series, each term of which corresponds to a k directed trivalent ribbon graph Γ whose edges are labeled by two variables te 2 R, `e 2 [L0;L1]. Formally, then, X jAut(Γ)j Z 1 Z 1 Y Z L1 Z L1 Y Z(λ) ∼ λjvert (Γ)j ::: dt ::: d` f (ft g; f` g); jvert (Γ)j! e e Γ e e Γ −∞ −∞ e2e(Γ) L0 L0 e2e(Γ) where jvert (G)j is the number of vertices in Γ and jAut(Γ)j is the order of the group of automor- phisms of Γ : Kaku and Kikkawa's [7] arguments lead one to expect that 2 −d=2 fΓ(fteg; f`eg) ∼ det(−∆Γ;fteg;f`eg + m ) ; where ∆Γ;fteg;f`eg is the Laplacian on a Riemann surface formed by replacing each edge e of the ribbon graph Γ by a tube of length te and width `e, and gluing the corresponding tubes to form a {Note that since Fock space is constructed from the symmetric product of square-integrable loops, which are not continuous, the problem of \gluing" two loops of lengths `1 and `2 to form a loop of length `1 + `2; which is a cause of concern in the physics literature, does not arise.
Load more

Recommended publications
  • Wiener Measures on Certain Banach Spaces Over Non-Archimedean Local fields Compositio Mathematica, Tome 93, No 1 (1994), P
    COMPOSITIO MATHEMATICA TAKAKAZU SATOH Wiener measures on certain Banach spaces over non-archimedean local fields Compositio Mathematica, tome 93, no 1 (1994), p. 81-108 <http://www.numdam.org/item?id=CM_1994__93_1_81_0> © Foundation Compositio Mathematica, 1994, tous droits réservés. L’accès aux archives de la revue « Compositio Mathematica » (http: //http://www.compositio.nl/) implique l’accord avec les conditions gé- nérales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une in- fraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ 81 © 1994 Kluwer Academic Publishers. Printed in the Netherlands. Wiener measures on certain Banach spaces over non-Archimedean local fields TAKAKAZU SATOH Department of Mathematics, Faculty of Science, Saitama University, 255 Shimo-ookubo, Urawu, Saitama, 338, Japan Received 8 June 1993; accepted in final form 29 July 1993 Dedicated to Proffessor Hideo Shimizu on his 60th birthday 1. Introduction The integral representation is a fundamental tool to study analytic proper- ties of the zeta function. For example, the Euler p-factor of the Riemann zeta function is where dx is a Haar measure of Q, and p/( p - 1) is a normalizing constant so that measure of the unit group is 1. What is necessary to generalize such integrals to a completion of a ring finitely generated over Zp? For example, let T be an indeterminate. The two dimensional local field Qp«T» is an infinite dimensional Qp-vector space.
    [Show full text]
  • Mixtures of Gaussian Cylinder Set Measures and Abstract Wiener Spaces As Models for Detection Annales De L’I
    ANNALES DE L’I. H. P., SECTION B A. F. GUALTIEROTTI Mixtures of gaussian cylinder set measures and abstract Wiener spaces as models for detection Annales de l’I. H. P., section B, tome 13, no 4 (1977), p. 333-356 <http://www.numdam.org/item?id=AIHPB_1977__13_4_333_0> © Gauthier-Villars, 1977, tous droits réservés. L’accès aux archives de la revue « Annales de l’I. H. P., section B » (http://www.elsevier.com/locate/anihpb) implique l’accord avec les condi- tions générales d’utilisation (http://www.numdam.org/conditions). Toute uti- lisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. Inst. Henri Pincaré, Section B : Vol. XIII, nO 4, 1977, p. 333-356. Calcul des Probabilités et Statistique. Mixtures of Gaussian cylinder set measures and abstract Wiener spaces as models for detection A. F. GUALTIEROTTI Dept. Mathematiques, ~cole Polytechnique Fédérale, 1007 Lausanne, Suisse 0. INTRODUCTION AND ABSTRACT Let H be a real and separable Hilbert space. Consider on H a measurable family of weak covariance operators { Re, 0 > 0 } and, on !?+ : = ]0, oo [, a probability distribution F. With each Re is associated a weak Gaussian distribution Jlo. The weak distribution p is then defined by Jl can be studied, as we show below, within the theory of abstract Wiener spaces. The motivation for considering such measures comes from statistical communication theory. There, signals of finite energy are often modelled as random variables, normally distributed, with values in a L2-space.
    [Show full text]
  • Change of Variables in Infinite-Dimensional Space
    Change of variables in infinite-dimensional space Denis Bell Denis Bell Change of variables in infinite-dimensional space Change of variables formula in R Let φ be a continuously differentiable function on [a; b] and f an integrable function. Then Z φ(b) Z b f (y)dy = f (φ(x))φ0(x)dx: φ(a) a Denis Bell Change of variables in infinite-dimensional space Higher dimensional version Let φ : B 7! φ(B) be a diffeomorphism between open subsets of Rn. Then the change of variables theorem reads Z Z f (y)dy = (f ◦ φ)(x)Jφ(x)dx: φ(B) B where @φj Jφ = det @xi is the Jacobian of the transformation φ. Denis Bell Change of variables in infinite-dimensional space Set f ≡ 1 in the change of variables formula. Then Z Z dy = Jφ(x)dx φ(B) B i.e. Z λ(φ(B)) = Jφ(x)dx: B where λ denotes the Lebesgue measure (volume). Denis Bell Change of variables in infinite-dimensional space Version for Gaussian measure in Rn − 1 jjxjj2 Take f (x) = e 2 in the change of variables formula and write φ(x) = x + K(x). Then we obtain Z Z − 1 jjyjj2 <K(x);x>− 1 jK(x)j2 − 1 jjxjj2 e 2 dy = e 2 Jφ(x)e 2 dx: φ(B) B − 1 jxj2 So, denoting by γ the Gaussian measure dγ = e 2 dx, we have Z <K(x);x>− 1 jjKx)jj2 γ(φ(B)) = e 2 Jφ(x)dγ: B Denis Bell Change of variables in infinite-dimensional space Infinite-dimesnsions There is no analogue of the Lebesgue measure in an infinite-dimensional vector space.
    [Show full text]
  • Dynamics of Infinite-Dimensional Groups and Ramsey-Type Phenomena
    \rtp-impa" i i 2005/5/12 page 1 i i Dynamics of infinite-dimensional groups and Ramsey-type phenomena Vladimir Pestov May 12, 2005 i i i i \rtp-impa" i i 2005/5/12 page 2 i i i i i i \rtp-impa" i i 2005/5/12 page i i i Contents Preface iii 0 Introduction 1 1 The Ramsey{Dvoretzky{Milman phenomenon 17 1.1 Finite oscillation stability . 17 1.2 First example: the sphere S1 . 27 1.2.1 Finite oscillation stability of S1 . 27 1.2.2 Concentration of measure on spheres . 32 1.3 Second example: finite Ramsey theorem . 41 1.4 Counter-example: ordered pairs . 47 2 The fixed point on compacta property 49 2.1 Extremely amenable groups . 49 2.2 Three main examples . 55 2.2.1 Example: the unitary group . 55 2.2.2 Example: the group Aut (Q; ) . 60 ≤ 2.2.3 Counter-example: the infinite symmetric group 62 2.3 Equivariant compactification . 63 2.4 Essential sets and the concentration property . 66 2.5 Veech theorem . 71 2.6 Big sets . 76 2.7 Invariant means . 81 3 L´evy groups 95 3.1 Unitary group with the strong topology . 95 i i i i i \rtp-impa" i i 2005/5/12 page ii i i ii CONTENTS 3.2 Group of measurable maps . 98 3.2.1 Construction and example . 98 3.2.2 Martingales . 101 3.2.3 Unitary groups of operator algebras . 110 3.3 Groups of transformations of measure spaces . 115 3.3.1 Maurey's theorem .
    [Show full text]
  • The Singular Moving Points Are What Is Left of the Moving Points
    BOOK REVIEWS 695 points. Those which are not singular, are regular. The regular moving points are the union of disjoint annuli; the singular moving points are what is left of the moving points. The description of the flow then is given in terms of the regular moving points, where it can be completely described in terms of simple "patches"-certain standard annular flows; the fixed points-where it is, of course, fixed; and the singular moving points-where life gets complicated. To develop the theory for singular moving points, the author first considers a very special case: the case of flows in a multiply-connected region of the plane where every orbit is aperiodic and has all its endpoints in the boundary. These he calls Kaplan-Mar kus flows, after the two who first began develop­ ment of the theory of such flows. Complete success in describing such flows has eluded the author and his coworkers except, to some extent, where the set of singular fixed points has only finitely many components. The later is, however, basic, and so for many cases, another patch in the quilt yields to description. After this, the author explores various ways to combine such flows with regular flows and develop further theory. Flows without stagnation points can be described rather completely. For flows with a finite number of stagnation points, or whose set of stagnation points has countable closure, a considerable amount is known, though the information is not as complete as for the no stagnation point case. In all cases where a description is possible, it is the set of regular moving points that supplies the main body of information.
    [Show full text]
  • On Superpositional Filtrations
    Munich Personal RePEc Archive On superpositional filtrations Strati, Francesco 20 August 2012 Online at https://mpra.ub.uni-muenchen.de/40879/ MPRA Paper No. 40879, posted 29 Aug 2012 04:19 UTC On superpositional filtrations Francesco Strati Department of Statistics, University of Messina Messina, Italy E-mail: [email protected] Abstract In this present work I shall define the basic notions of superpositional filtrations. Given a superposition integral I shall find a general measure theory by means of cylinder sets and then I shall define the properties of the sfiltration for a general process X. n §1. We denote by Sn ≡ S(R ) the Schwartz space endowed with a natural topology (Sτ ) which stems from the seminorm α β ||ϕ||α,β ≡ sup |x D ϕ(x)| < ∞. x∈Rn ′ ′ Rn We call this kind of space S-space, and it is a Fr´echet space [FrB]. We denote by Sn ≡S ( ) the space of tempered distributions. It is the topological dual of the topological vector space (Sn, Sτ ) [FrT]. A locally integrable function can be a tempered distribution if, for some constants a and C |f(x)|dx ≤ aGC , G → ∞ Z|x|≤G and thus |f(x)ϕ(x)|dx < ∞, ∀ϕ ∈S′. Rn Z Therefore we can say that Rn f(x)ϕ(x)dx is a tempered distribution [FrT]. ′ ′ We know that the superpositionR integral [FrB] runs through S -spaces, rather given a ∈ Sm Rn ′ ′ Rm ′ and a summable v ∈S( , S ), the superposition integral of v on Sm( ) is the element of Sn defined by lim (αk ◦ vˆ)= av = a ◦ vˆ k→+∞ Rm Z 2010 Mathematics Subject Classification: Primary 28C05, 28C15 ; Secondary 28A05.
    [Show full text]
  • Arxiv:1905.02109V1 [Math.FA] 6 May 2019 Hl N14,F On( John F
    SCIENCE CHINA Mathematics CrossMark . ARTICLES . doi: Infinite dimensional Cauchy-Kowalevski and Holmgren type theorems Jiayang YU1 & Xu ZHANG 2,∗ 1 School of Mathematics, Sichuan University, Chengdu 610064, P. R. China; 2 School of Mathematics, Sichuan University, Chengdu 610064, P. R. China Email: [email protected], zhang [email protected] Abstract The aim of this paper is to show Cauchy-Kowalevski and Holmgren type theorems with infinite number of variables. We adopt von Koch and Hilbert’s definition of analyticity of functions as monomial expansions. Our Cauchy-Kowalevski type theorem is derived by modifying the classical method of majorants. Based on this result, by employing some tools from abstract Wiener spaces, we establish our Holmgren type theorem. Keywords Cauchy-Kowalevski theorem, Holmgren theorem, monomial expansions, abstract Wiener space, divergence theorem, method of majorants MSC(2010) Primary 35A10, 26E15, 46G20; Secondary 46G20, 46G05, 58B99. Citation: Jiayang Yu, Xu Zhang. Infinite dimensional Cauchy-Kowalevski and Holmgren type theorems. Sci China Math, 2019, 60, doi: 1 Introduction The classical Cauchy-Kowalevski theorem asserts the local existence and uniqueness of analytic solutions to quite general partial differential equations with analytic coefficients and initial data in the finite dimensional Euclidean space n (for any given n ). In 1842, A. L. Cauchy first proved this theorem arXiv:1905.02109v1 [math.FA] 6 May 2019 R N ∈ for the second order case; while in 1875, S. Kowalevski proved the general result. Both of them used the method of majorants. Because of its fundamental importance, there exists continued interest to generalize and/or improve this theorem (See [2,10,24,26–29,31–33,35] and the references cited therin).
    [Show full text]
  • STRASSEN's LAW of the ITERATED LOGARITHM by James D
    ANNALES DE L’INSTITUT FOURIER JAMES D. KUELBS Strassen’s law of the iterated logarithm Annales de l’institut Fourier, tome 24, no 2 (1974), p. 169-177 <http://www.numdam.org/item?id=AIF_1974__24_2_169_0> © Annales de l’institut Fourier, 1974, tous droits réservés. L’accès aux archives de la revue « Annales de l’institut Fourier » (http://annalif.ujf-grenoble.fr/) implique l’accord avec les conditions gé- nérales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une in- fraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. Inst. Fourier, Grenoble 24, 2 (1974), 169-177. STRASSEN'S LAW OF THE ITERATED LOGARITHM by James D. KUELBS (*). 1. Introduction. Throughout E is a real locally convex Hausdorff topolo- gical vector space. If the topology on E is metrizable and complete, then E is called a Frechet space and it is well known that the topology on E is generated by an increasing sequence of semi-norms |[ .||^ (/ == 1, 2, . .) such that Ii E —_ ^\^ "••" ^2^(1+11.11,) gives an invariant metric on E which generates the topology on E. A semi-norm [|.|| is called a Hilbert semi-norm if INI2 == (^? ^) where (., .) is an inner product which may possibly vanish at some x ^ 0. We say a Frechet space E is of Hilbert space type if we can choose an increasing sequence of Hilbert semi-norms which generate the topology of E.
    [Show full text]
  • DUALITY PHENOMENA and VOLUME INEQUALITIES in CONVEX GEOMETRY a Dissertation Submitted to Kent State University in Partial Fulfil
    DUALITY PHENOMENA AND VOLUME INEQUALITIES IN CONVEX GEOMETRY A dissertation submitted to Kent State University in partial fulfillment of the requirements for the degree of Doctor of Philosophy by Jaegil Kim August, 2013 Dissertation written by Jaegil Kim B.S., Pohang University of Science and Technology, 2005 M.S., Pohang University of Science and Technology, 2008 Ph.D., Kent State University, 2013 Approved by Chair, Doctoral Dissertation Committee Dr. Artem Zvavitch Members, Doctoral Dissertation Committee Dr. Richard M. Aron Members, Doctoral Dissertation Committee Dr. Fedor Nazarov Members, Doctoral Dissertation Committee Dr. Dmitry Ryabogin Members, Outside Discipline Dr. Fedor F. Dragan Members, Graduate Faculty Representative Dr. David W. Allender Accepted by Chair, Department of Mathematical Sciences Dr. Andrew Tonge Associate Dean Raymond Craig Dean, College of Arts and Sciences ii TABLE OF CONTENTS ACKNOWLEDGEMENTS . v Introduction and Preliminaries 1 0.1 Basic concepts in Convex Geometry . 2 0.2 Summary and Notation . 5 0.3 Bibliographic Note . 7 I Mahler conjecture 8 1 Introduction to the volume product . 9 1.1 The volume product and its invariant properties . 9 1.2 Mahler conjecture and related results . 13 2 More on Hanner polytopes . 16 2.1 Connection with perfect graphs . 16 2.2 Direct sums of polytopes . 20 3 Local minimality in the symmetric case . 31 3.1 Construction of Polytopes . 31 3.2 Computation of volumes of polytopes . 41 3.3 A gap between K and a polytope . 60 4 Local minimality in the nonsymmetric case . 79 4.1 Continuity of the Santal´omap . 80 iii 4.2 Construction of polytopes for the simplex case .
    [Show full text]
  • Small-Time Large Deviations for Sample Paths of Infinite-Dimensional Symmetric Dirichlet Processes
    Small-Time Large Deviations for Sample Paths of Infinite-Dimensional Symmetric Dirichlet Processes vorgelegt von Mag. rer. nat. Stephan Sturm aus Wien Von der Fakult¨atII { Mathematik und Naturwissenschaften der Technischen Universit¨atBerlin zur Erlangung des akademischen Grades Doktor der Naturwissenschaften { Dr. rer. nat. { genehmigte Dissertation Promotionsausschuss Vorsitzender: Prof. Dr. Stefan Felsner Gutachter: Prof. Dr. Alexander Schied Prof. Dr. Jean-Dominique Deuschel Tag der wissenschaftlichen Aussprache: 15. Januar 2010 Berlin 2009 D 83 ii Introduction The objective of the present thesis is to study the small-time asymptotic behavior of diffusion processes on general state spaces. In particular we want to determine the convergence speed of the weak law of large numbers, so we study the asymptotics on an exponential scale, as developed starting with the pioneering work of Cram´er[C] (but already Khinchin [Kh] used in the early 1920s the notion of 'large deviations' for the asymptotics of very improbable events). Moreover, we are interested in the behavior of the whole path of the diffusion. So we consider a diffusion process (Xt) on the state space " " X , and define the family of diffusions (Xt ), " > 0, Xt = X"t. For this family of sample paths we want to prove large deviation principle " " − inf I(!) ≤ lim inf " log Pµ[X· 2 A] ≤ lim sup " log Pµ[X· 2 A] ≤ − inf I(!) !2A◦ "!0 "!0 !2A for any measurable set A in the space of sample paths Ω := ([0; 1]; X ), with some rate function I which will be determined. First results in this direction were achieved by Varadhan [Va67b], who proved the small-time asymp- totics on an exponential scale for elliptic, finite-dimensional diffusion processes.
    [Show full text]
  • The Converse of Minlos' Theorem Dedicated to Professor Tsuyoshi Ando on the Occasion of His Sixtieth Birthday
    Publ. RIMS, Kyoto Univ. 30(1994), 851-863 The Converse of Minlos' Theorem Dedicated to Professor Tsuyoshi Ando on the occasion of his sixtieth birthday By Yoshiaki OKAZAKI* and Yasuji TAKAHASHI** Abstract Let ^ be the class of barrelled locally convex Hausdorff space E such that E'^ satisfies the property B in the sense of Pietsch. It is shown that if Ee^and if each continuous cylinder set measure on E' is <7(£', E) -Radon, then E is nuclear. There exists an example of non-nuclear Frechet space E such that each continuous Gaussian cylinder set measure on £'is 0(E', E)-Radon. Let q be 2 < q < oo. Suppose that E e ^ and £ is a projective limit of Banach space {Ea} such that the dual E'a is of cotype q for every ct,. Suppose also that each continuous Gaussian cylinder set measure on E' is a(E',E) -Radon. Then E is nuclear. §1. Introduction Let £ be a nuclear locally convex Hausdorff space, then each continuous cylinder set measure on E' is <r(£',E)-Radon (Minlos' theorem, see Badrikian [2], Gelfand and Vilenkin [4], Minlos [11], Umemura [20] and Yamasaki [21]). We consider the converse problem. Let £ be a locally convex Hausdorff space. If each continuous cylinder set measure on £"' is o(E',E)-Radon, then is E nuclear? The partial answers are known as follows. (1) If E is a a-Hilbert space or a Frechet space, then the answer is affirmative (see Badrikian [2], Gelfand and Vilenkin [4], Minlos, [11], Mushtari [12], Umemura [20] and Yamasaki [21]).
    [Show full text]
  • Inequivalent Vacuum States in Algebraic Quantum Theory
    Inequivalent Vacuum States in Algebraic Quantum Theory G. Sardanashvily Department of Theoretical Physics, Moscow State University, Moscow, Russia Abstract The Gelfand–Naimark–Sigal representation construction is considered in a general case of topological involutive algebras of quantum systems, including quantum fields, and in- equivalent state spaces of these systems are characterized. We aim to show that, from the physical viewpoint, they can be treated as classical fields by analogy with a Higgs vacuum field. Contents 1 Introduction 2 2 GNS construction. Bounded operators 4 3 Inequivalent vacua 8 4 Example. Infinite qubit systems 12 5 Example. Locally compact groups 13 6 GNS construction. Unbounded operators 17 7 Example. Commutative nuclear groups 20 arXiv:1508.03286v1 [math-ph] 13 Aug 2015 8 Infinite canonical commutation relations 22 9 Free quantum fields 27 10 Euclidean QFT 31 11 Higgs vacuum 34 12 Automorphisms of quantum systems 35 13 Spontaneous symmetry breaking 39 1 14 Appendixes 41 14.1 Topologicalvectorspaces . .... 41 14.2 Hilbert, countably Hilbert and nuclear spaces . ...... 43 14.3 Measuresonlocallycompactspaces . .... 45 14.4Haarmeasures .................................... 49 14.5 Measures on infinite-dimensional vector spaces . ........ 51 1 Introduction No long ago, one thought of vacuum in quantum field theory (QFT) as possessing no physical characteristics, and thus being invariant under any symmetry transformation. It is exemplified by a particleless Fock vacuum (Section 8). Contemporary gauge models of fundamental interactions however have arrived at a concept of the Higgs vacuum (HV). By contrast to the Fock one, HV is equipped with nonzero characteristics, and consequently is non-invariant under transformations. For instance, HV in Standard Model of particle physics is represented by a constant back- ground classical Higgs field, in fact, inserted by hand into a field Lagrangian, whereas its true physical nature still remains unclear.
    [Show full text]