DOCSLIB.ORG

Noncommutative Geometry and Cosmology

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Noncommutative Geometry and Cosmology Noncommutative geometry and cosmology Matilde Marcolli Beijing, August 2013 Matilde Marcolli Noncommutative geometry and cosmology This talk is based on: MPT M. Marcolli, E. Pierpaoli, K. Teh, The spectral action and cosmic topology, arXiv:1005.2256, CMP 304 (2011) 125-174 MPT2 M. Marcolli, E. Pierpaoli, K. Teh, The coupling of topology and inflation in Noncommutative Cosmology, arXiv:1012.0780, CMP 309 (2012) N.2, 341-369 CMTB. Ca´ci´c,M.´ Marcolli, K. Teh, Topological coupling of gravity to matter, spectral action and cosmic topology, arXiv:1106.5473, to appear in JNCG and refs on NCG standard model and cosmology: CCM A. Chamseddine, A. Connes, M. Marcolli, Gravity and the standard model with neutrino mixing, Adv. Theor. Math. Phys. 11 (2007), no. 6, 991{1089. MP M. Marcolli, E. Pierpaoli, Early universe models from noncommutative geometry, arXiv:0908.3683, Adv. Theor. Math. Phys. 14 (2010) 1373-1432 KM D. Kolodrubetz, M. Marcolli, Boundary conditions of the RGE flow in noncommutative cosmology, arXiv:1006.4000, Phys. Lett. B 693 (2010) 166-174. Matilde Marcolli Noncommutative geometry and cosmology Two topics of current interest to cosmologists: • Modified Gravity models in cosmology: Einstein-Hilbert action (+cosmological term) replaced or extended with other gravity terms (conformal gravity, higher derivative terms) ) cosmological predictions • The question of Cosmic Topology: Nontrivial (non-simply-connected) spatial sections of spacetime, homogeneous spherical or flat spaces: how can this be detected from cosmological observations? Matilde Marcolli Noncommutative geometry and cosmology The question of Cosmic Topology: Nontrivial (non-simply-connected) spatial sections of spacetime, homogeneous spherical or flat spaces: how can this be detected from cosmological observations? Matilde Marcolli Noncommutative geometry and cosmology Cosmic Microwave Background best source of cosmological data on which to test theoretical models (modified gravity models, cosmic topology hypothesis, particle physics models) COBE satellite (1989) WMAP satellite (2001) Planck satellite (2009): new data available now! Matilde Marcolli Noncommutative geometry and cosmology Cosmic topology and the CMB Einstein equations determine geometry not topology (don't distinguish S3 from S3=Γ with round metric) Cosmological data (BOOMERanG experiment 1998, WMAP data 2003): spatial geometry of the universe is flat or slightly positively curved Homogeneous and isotropic compact case: spherical space forms S3=Γ or Bieberbach manifolds T 3=Γ Is cosmic topology detected by the Cosmic Microwave Background (CMB)? Search for signatures of multiconnected topologies Matilde Marcolli Noncommutative geometry and cosmology CMB sky and spherical harmonics temperature fluctuations 1 ` ∆T X X = a Y T `m `m `=0 m=−` Y`m spherical harmonics Methods to address cosmic topology problem Statistical search for matching circles in the CMB sky: identify a nontrivial fundamental domain Anomalies of the CMB: quadrupole suppression, the small value of the two- point temperature correlation function at angles above 60 degrees, and the anomalous alignment of the quadrupole and octupole Residual gravity acceleration: gravitational effects from other fundamental domains Bayesian analysis of different models of CMB sky for different candidate topologies Results: no conclusive evidence of a non-simply connected topology Matilde Marcolli Noncommutative geometry and cosmology Our approach: NCG provides a modified gravity model through the spectral action The nonperturbative form of the spectral action determines a slow-roll inflation potential The underlying geometry (spherical/flat) affects the shape of the potential (possible models of inflation) Different inflation scenarios depending on geometry and topology of the cosmos More refined topological properties from coupling to matter Matilde Marcolli Noncommutative geometry and cosmology The noncommutative space X × F extra dimensions product of 4-dim spacetime and finite NC space The spectral action functional 1 Tr(f (D =Λ)) + h J ξ;~ D ξ~i A 2 A 0 −1 DA = D + A + " JAJ Dirac operator with inner fluctuations ∗ P A = A = k ak [D; bk ] Action functional for gravity on X (modified gravity) Gravity on X × F = gravity coupled to matter on X Matilde Marcolli Noncommutative geometry and cosmology Spectral triples( A; H; D): • involutive algebra A • representation π : A!L(H) • self adjoint operator D on H • compact resolvent (1 + D2)−1=2 2 K • [a; D] bounded 8a 2 A • even Z=2-grading [γ; a] = 0 and Dγ = −γD • real structure: antilinear isom J : H!H with J2 = ", JD = "0DJ, and Jγ = "00γJ n 0 1 2 3 4 5 6 7 " 1 1 -1 -1 -1 -1 1 1 "0 1 -1 1 1 1 -1 1 1 "00 1 -1 1 -1 • bimodule: [a; b0] = 0 for b0 = Jb∗J−1 • order one condition: [[D; a]; b0] = 0 Matilde Marcolli Noncommutative geometry and cosmology Asymptotic formula for the spectral action (Chamseddine{Connes) Z X k −k Tr(f (D=Λ)) ∼ fk Λ −|Dj + f (0)ζD (0) + o(1) k2DimSp R 1 k−1 for large Λ with fk = 0 f (v)v dv and integration given by residues of −s zeta function ζD (s) = Tr(jDj ); DimSp poles of zeta functions Asymptotic expansion ) Effective Lagrangian (modified gravity + matter) At low energies: only nonperturbative form of the spectral action Tr(f (DA=Λ)) Need explicit information on the Dirac spectrum! Matilde Marcolli Noncommutative geometry and cosmology 1 2 Product geometry( C (X ); L (X ; S); DX ) [ (AF ; HF ; DF ) 1 1 A = C (X ) ⊗ AF = C (X ; AF ) 2 2 H = L (X ; S) ⊗ HF = L (X ; S ⊗ HF ) D = DX ⊗ 1 + γ5 ⊗ DF Inner fluctuations of the Dirac operator 0 −1 D ! DA = D + A + " JAJ A self-adjoint operator X A = aj [D; bj ] ; aj ; bj 2 A ) boson fields from inner fluctuations, fermions from HF Matilde Marcolli Noncommutative geometry and cosmology Get realistic particle physics models [CCM] Need Ansatz for the NC space F ALR = C ⊕ HL ⊕ HR ⊕ M3(C) ) everything else follows by computation Representation: MF sum of all inequiv irred odd N ALR -bimodules (fix N generations) HF = ⊕ MF fermions Algebra AF = C ⊕ H ⊕ M3(C): order one condition F zero dimensional but KO-dim 6 JF = matter/antimatter, γF = L/R chirality Classification of Dirac operators (moduli spaces) Matilde Marcolli Noncommutative geometry and cosmology Parameters of νMSM Get an extension of minimal Standard Model with right handed neutrinos, Majorana mass terms, and lepton mixing - three coupling constants - 6 quark masses, 3 mixing angles, 1 complex phase - 3 charged lepton masses, 3 lepton mixing angles, 1 complex phase - 3 neutrino masses - 11 Majorana mass matrix parameters • Bosons from inner fluctuations of D (gauge: manifold direction, Higgs: NC direction) • Fermions from basis of representation space HF • Correct gauge group and hypercharges of particles • Action functional: spectral action on X × F , asymptotic expansion gives full Lagrangian of νMSM with non-minimal coupling to (modified) gravity. Matilde Marcolli Noncommutative geometry and cosmology The asymptotic expansion of the spectral action from [CCM] 1 f Z p S = (48 f Λ4 − f Λ2 c + 0 d) g d 4x π2 4 2 4 96 f Λ2 − f c Z p + 2 0 R g d 4x 24π2 f Z 11 p + 0 ( R∗R∗ − 3 C C µνρσ) g d 4x 10 π2 6 µνρσ (−2 a f Λ2 + e f ) Z p + 2 0 j'j2 g d 4x π2 f a Z p + 0 jD 'j2 g d 4x 2 π2 µ f a Z p − 0 R j'j2 g d 4x 12 π2 f b Z p + 0 j'j4 g d 4x 2 π2 f Z 5 p + 0 (g 2 G i G µνi + g 2 F α F µνα + g 2 B Bµν ) g d 4x; 2 π2 3 µν 2 µν 3 1 µν Matilde Marcolli Noncommutative geometry and cosmology Parameters: f0, f2, f4 free parameters, f0 = f (0) and, for k > 0, Z 1 k−1 fk = f (v)v dv: 0 a; b; c; d; e functions of Yukawa parameters of SM+r.h.ν y y y y a = Tr(Yν Yν + Ye Ye + 3(Yu Yu + Yd Yd )) y 2 y 2 y 2 y 2 b = Tr((Yν Yν) + (Ye Ye ) + 3(Yu Yu) + 3(Yd Yd ) ) c = Tr(MMy) d = Tr((MMy)2) y y e = Tr(MM Yν Yν): Matilde Marcolli Noncommutative geometry and cosmology Normalization and coefficients Z Z 1 p 4 p 4 S = 2 R g d x + γ0 g d x 2κ0 Z Z µνρσp 4 ∗ ∗p 4 + α0 Cµνρσ C g d x + τ0 R R g d x 1 Z p Z p + jDHj2 g d 4x − µ2 jHj2 g d 4x 2 0 Z Z 2 p 4 4 p 4 − ξ0 R jHj g d x + λ0 jHj g d x 1 Z p + (G i G µνi + F α F µνα + B Bµν ) g d 4x; 4 µν µν µν Energy scale: Unification (1015 { 1017 GeV) g 2f 1 0 = 2π2 4 Preferred energy scale, unification of coupling constants Matilde Marcolli Noncommutative geometry and cosmology Coefficients 2 1 96f2Λ − f0c 1 4 2 f0 2κ2 = 2 γ0 = 2 (48f4Λ − f2Λ c + d) 0 24π π 4 3f 11f α = − 0 τ = 0 0 10π2 0 60π2 2 2 f2Λ e 1 µ0 = 2 − ξ0 = 12 f0 a π2b λ0 = 2 2f0a Matilde Marcolli Noncommutative geometry and cosmology Renormalization group running of parameters Used to obtain physical predictions from the particle physics sector of the model: - [CCM] RGE for particle sector to estimate Higgs mass: 170 GeV... too large! - Recent methods for correcting to realistic Higgs mass ∼125 GeV: • A. Chamseddine, A. Connes, arXiv:1208.1030 (additional scalar field coupled to Higgs) • C. Estrada, M. Marcolli, arXiv:1208.5023 (gravity correction terms, asymptotic safety, anomalous dimensions) - In [MP] [KM]: running coefficients with RGE flow of particle physics content from unification energy down to electroweak.
Load more

Recommended publications
  • The Weil Proof and the Geometry of the Adèles Class Space
    The Weil Proof and the Geometry of the Adèles Class Space Alain Connes,1 Caterina Consani,2 and Matilde Marcolli3 1 Collège de France, 3, rue d’Ulm, Paris, F-75005 France [email protected] 2 Mathematics Department, Johns Hopkins University, Baltimore, MD 21218 USA [email protected] 3 Department of Mathematics, California Institute of Technology 1200 E California Blvd, Pasadena, CA 91101, USA [email protected] Dedicated to Yuri Manin on the occasion of his 70th birthday O simili o dissimili che sieno questi mondi non con minor raggione sarebe bene a l’uno l’essere che a l’altro Giordano Bruno – De l’infinito, universo e mondi Summary. This paper explores analogies between the Weil proof of the Riemann hypothesis for function fields and the geometry of the adèles class space, which is the noncommutative space underlying Connes’ spectral realization of the zeros of the Riemann zeta function. We consider the cyclic homology of the cokernel (in the abelian category of cyclic modules) of the “restriction map” defined by the inclu- sion of the idèles class group of a global field in the noncommutative adèles class space. Weil’s explicit formula can then be formulated as a Lefschetz trace formula for the induced action of the idèles class group on this cohomology. In this formu- lation the Riemann hypothesis becomes equivalent to the positivity of the relevant trace pairing. This result suggests a possible dictionary between the steps in the Weil proof and corresponding notions involving the noncommutative geometry of the adèles class space, with good working notions of correspondences, degree, and codegree etc.
    [Show full text]
  • Noncommutative Geometry Models for Particle Physics and Cosmology, Lecture I
    Noncommutative Geometry models for Particle Physics and Cosmology, Lecture I Matilde Marcolli Villa de Leyva school, July 2011 Matilde Marcolli NCG models for particles and cosmology, I Plan of lectures 1 Noncommutative geometry approach to elementary particle physics; Noncommutative Riemannian geometry; finite noncommutative geometries; moduli spaces; the finite geometry of the Standard Model 2 The product geometry; the spectral action functional and its asymptotic expansion; bosons and fermions; the Standard Model Lagrangian; renormalization group flow, geometric constraints and low energy limits 3 Parameters: relations at unification and running; running of the gravitational terms; the RGE flow with right handed neutrinos; cosmological timeline and the inflation epoch; effective gravitational and cosmological constants and models of inflation 4 The spectral action and the problem of cosmic topology; cosmic topology and the CMB; slow-roll inflation; Poisson summation formula and the nonperturbative spectral action; spherical and flat space forms Matilde Marcolli NCG models for particles and cosmology, I Geometrization of physics Kaluza-Klein theory: electromagnetism described by circle bundle over spacetime manifold, connection = EM potential; Yang{Mills gauge theories: bundle geometry over spacetime, connections = gauge potentials, sections = fermions; String theory: 6 extra dimensions (Calabi-Yau) over spacetime, strings vibrations = types of particles NCG models: extra dimensions are NC spaces, pure gravity on product space becomes gravity
    [Show full text]
  • Lectures on Factorization Homology, ∞-Categories, and Topological
    SPRINGER BRIEFS IN MATHEMATICAL PHYSICS 39 Hiro Lee Tanaka Lectures on Factorization Homology, ∞-Categories, and Topological Field Theories Contributed by Araminta Amabel · Artem Kalmykov · Lukas Müller SpringerBriefs in Mathematical Physics Volume 39 Series Editors Nathanaël Berestycki, University of Vienna, Vienna, Austria Mihalis Dafermos, Mathematics Department, Princeton University, Princeton, NJ, USA Atsuo Kuniba, Institute of Physics, The University of Tokyo, Tokyo, Japan Matilde Marcolli, Department of Mathematics, University of Toronto, Toronto, Canada Bruno Nachtergaele, Department of Mathematics, Davis, CA, USA Hirosi Ooguri, Walter Burke Institute for Theoretical Physics, California Institute of Technology, Pasadena, CA, USA SpringerBriefs are characterized in general by their size (50–125 pages) and fast production time (2–3 months compared to 6 months for a monograph). Briefs are available in print but are intended as a primarily electronic publication to be included in Springer’s e-book package. Typical works might include: • An extended survey of a field • A link between new research papers published in journal articles • A presentation of core concepts that doctoral students must understand in order to make independent contributions • Lecture notes making a specialist topic accessible for non-specialist readers. SpringerBriefs in Mathematical Physics showcase, in a compact format, topics of current relevance in the field of mathematical physics. Published titles will encompass all areas of theoretical and mathematical physics.
    [Show full text]
  • LECTURE Series
    University LECTURE Series Volume 52 Koszul Cohomology and Algebraic Geometry Marian Aprodu Jan Nagel American Mathematical Society http://dx.doi.org/10.1090/ulect/052 Koszul Cohomology and Algebraic Geometry University LECTURE Series Volume 52 Koszul Cohomology and Algebraic Geometry Marian Aprodu Jan Nagel M THE ATI A CA M L ΤΡΗΤΟΣ ΜΗ N ΕΙΣΙΤΩ S A O C C I I R E E T ΑΓΕΩΜΕ Y M A F O 8 U 88 NDED 1 American Mathematical Society Providence, Rhode Island EDITORIAL COMMITTEE Jerry L. Bona NigelD.Higson Eric M. Friedlander (Chair) J. T. Stafford 2000 Mathematics Subject Classification. Primary 14H51, 14C20, 14H60, 14J28, 13D02, 16E05. For additional information and updates on this book, visit www.ams.org/bookpages/ulect-52 Library of Congress Cataloging-in-Publication Data Aprodu, Marian. Koszul cohomology and algebraic geometry / Marian Aprodu, Jan Nagel. p. cm. — (University lecture series ; v. 52) Includes bibliographical references and index. ISBN 978-0-8218-4964-4 (alk. paper) 1. Koszul algebras. 2. Geometry, Algebraic. 3. Homology theory. I. Nagel, Jan. II. Title. QA564.A63 2010 512.46—dc22 2009042378 Copying and reprinting. Individual readers of this publication, and nonprofit libraries acting for them, are permitted to make fair use of the material, such as to copy a chapter for use in teaching or research. Permission is granted to quote brief passages from this publication in reviews, provided the customary acknowledgment of the source is given. Republication, systematic copying, or multiple reproduction of any material in this publication is permitted only under license from the American Mathematical Society.
    [Show full text]
  • Lectures on Arithmetic Noncommutative Geometry Matilde Marcolli
    Lectures on Arithmetic Noncommutative Geometry Matilde Marcolli And indeed there will be time To wonder \Do I dare?" and, \Do I dare?" Time to turn back and descend the stair. ... Do I dare Disturb the Universe? ... For I have known them all already, known them all; Have known the evenings, mornings, afternoons, I have measured out my life with coffee spoons. ... I should have been a pair of ragged claws Scuttling across the floors of silent seas. ... No! I am not Prince Hamlet, nor was meant to be; Am an attendant lord, one that will do To swell a progress, start a scene or two ... At times, indeed, almost ridiculous{ Almost, at times, the Fool. ... We have lingered in the chambers of the sea By sea-girls wreathed with seaweed red and brown Till human voices wake us, and we drown. (T.S. Eliot, \The Love Song of J. Alfred Prufrock") Contents Chapter 1. Ouverture 5 1. The NCG dictionary 7 2. Noncommutative spaces 8 3. Spectral triples 9 Chapter 2. Noncommutative modular curves 17 1. Modular curves 17 2. The noncommutative boundary of modular curves 24 3. Modular interpretation: noncommutative elliptic curves 24 4. Limiting modular symbols 29 5. Hecke eigenforms 40 6. Selberg zeta function 43 7. The modular complex and K-theory of C∗-algebras 44 8. Intermezzo: Chaotic Cosmology 45 Chapter 3. Quantum statistical mechanics and Galois theory 53 1. Quantum Statistical Mechanics 54 2. The Bost{Connes system 58 3. Noncommutative Geometry and Hilbert's 12th problem 63 4. The GL2 system 65 5. Quadratic fields 72 Chapter 4.
    [Show full text]
  • NARRATIVE ENCOUNTERS with MATHEMATICS Contents
    THE WOLF AND THE STREET: NARRATIVE ENCOUNTERS WITH MATHEMATICS MATILDE MARCOLLI Contents 1. Introduction 1 2. Tales for the Wolf 1 2.1. Mathematical themes 2 2.2. Wolf in the Fold 4 2.3. Night Songs 5 3. Street Science 6 3.1. Street Art and Street Signs 6 3.2. The End? 8 1. Introduction I was invited to this conference to present the results of an old experiment, a twenty year old exploration of narrative and mathematics, in the form of a collection of fairytales. I began writing the stories of Racconti per il lupo (Tales for the Wolf) in 1986, when I was a sixteen year old student of the Liceo Classico, more occupied with ancient Greek texts and philosophy than with mathematics. I finished the collection when I was about to graduate in Theoretical Physics, at the University of Milano, in 1993. Those few years spanned enormous transformations, at the personal level, going through the passage from late adolescence to adulthood, and from being a student of classical languages to a professional physicist, as well as on the larger scale of society and the world: those were the years that marked \the end of the short century", with all the upheaval, excitement and anxiety that came with it. In their minuscule cameo scale, the mathematical stories I was putting together, act as a small fragmented mirror of larger events. The stories, written in Italian, and illustrated by a series of collages I prepared in the style of Max Ernst, are now available online at the publisher Lulu.com, along with some of my more recent writings.
    [Show full text]
  • Preserving the Unity of Mathematics CONTENTS
    ICMAT Newsletter #13 Autumn 2016 CSIC - UAM - UC3M - UCM EDITORIAL After the last European Congress of Mathematics, held between July 18th and July 22nd in Berlin, Marta Sanz-Solé, professor at the University of Barcelona, speaks about the European Mathematical Society, of which she was the Chair person between 2010 a 2014. The ECM: Preserving the Unity of Mathematics Less than one year ago, in October, 2015, the European Mathe- matical Society (EMS) celebrated its 25th anniversary. The place chosen to commemorate the event was the Institut Henri Poin- caré, the home of mathematics and theoretical physics in Paris since 1928. In that same year, the London Mathematical Soci- ety, one of the oldest mathematical societies in Europe, cele- brated its 150th anniversary, while many other societies have recently commemorated their 100th anniversary or are about to Rascon Image: Fernando do so. This difference in age may give rise to certain complexes, although there is no reason why this should happen. The EMS has enjoyed great success during its short existence, thanks to the well-defined space it occupies in a world that is advancing rapidly towards globalization, and the exclusively international scenario in which it carries out its functions. The conception and creation of the EMS in 1990 is better under- stood in the political context of Europe that arose after the tragic experience of World War II. In 1958, the communitary structure that currently underpins the Europan Union (EU) was estab- CONTENTS lished, on the basis of which the identity of Europe has been con- solidated, and the project, initially focused on the economy, has evolved along all fronts that affect the lives of those belonging Editorial: Marta Sanz-Solé (University of to the member states; in particular, education, research and in- Barcelona)..............................................................1 novation.
    [Show full text]
  • Yuri Ivanovich Manin
    Yuri Ivanovich Manin Academic career 1960 PhD, Steklov Mathematical Institute, Moscow, Russia 1963 Habilitation, Steklov Mathematical Institute, Moscow, Russia 1960 - 1993 Principal Researcher, Steklov Mathematical In- stitute, Russian Academy of Sciences, Moscow, Russia 1965 - 1992 Professor (Algebra Chair), University of Mos- cow, Russia 1992 - 1993 Professor, Massachusetts Institute of Technolo- gy, Cambridge, MA, USA 1993 - 2005 Scientific Member, Max Planck Institute for Ma- thematics, Bonn 1995 - 2005 Director, Max Planck Institute for Mathematics, Bonn 2002 - 2011 Board of Trustees Professor, Northwestern Uni- versity, Evanston, IL, USA Since 2005 Professor Emeritus, Max Planck Institute for Mathematics, Bonn Since 2011 Professor Emeritus, Northwestern University, Evanston, IL, USA Honours 1963 Moscow Mathematical Society Award 1967 Highest USSR National Prize (Lenin Prize) 1987 Brouwer Gold Medal 1994 Frederic Esser Nemmers Prize 1999 Rolf Schock Prize 1999 Doctor honoris causa, University of Paris VI (Universite´ Pierre et Marie Curie), Sorbonne, France 2002 King Faisal Prize for Mathematics 2002 Georg Cantor Medal of the German Mathematical Society 2002 Abel Bicentennial Doctor Phil. honoris causa, University of Oslo, Norway 2006 Doctor honoris causa, University of Warwick, England, UK 2007 Order Pour le Merite,´ Germany 2008 Great Cross of Merit with Star, Germany 2010 Janos´ Bolyai International Mathematical Prize 2011 Honorary Member, London Mathematical Society Invited Lectures 1966 International Congress of Mathematicians, Moscow, Russia 1970 International Congress of Mathematicians, Nice, France 1978 International Congress of Mathematicians, Helsinki, Finland 1986 International Congress of Mathematicians, Berkeley, CA, USA 1990 International Congress of Mathematicians, Kyoto, Japan 2006 International Congress of Mathematicians, special activity, Madrid, Spain Research profile Currently I work on several projects, new or continuing former ones.
    [Show full text]
  • A Drifter of Dadaist Persuasion
    A DRIFTER OF DADAIST PERSUASION MATILDE MARCOLLI 1. Mathematics through Abstract Art sors immanis et inanis, rota tu volubilis 1.1. Abstractions. Both my parents were very deeply involved in the scene of Italian contemporary art, over the span of several decades. Both of them studied Architecture in the late 1950s and early 1960s at the Politecnico in Milan. My mother, who had been a student Ernesto Nathan Rogers, collaborated with some of the most visible figures in architecture and graphic design of the time: Konrad Wachsmann, Ignazio Gardella, Albe Steiner. My father became a colleague of Umberto Eco and Tom´asMaldonado at the experimental university program in the arts, the DAMS of Bologna. My parents were also painters, and their art was frequently inspired by mathematical themes (Figure 1 and Figure 2). In the 1970s, both before and after my parents divorced, our house was frequented by a circle of artists, designers, and various communist intellectuals. I grew up surrounded by contemporary art, well versed in its history and meaning. I grew up listening to atonal 20th century classical music: by the time I was in my early teens, my favorite composers were Luciano Berio, Luigi Nono, Karlheinz Stockhausen, Iannis Xenakis, Giacinto Scelsi, Pierre Boulez. Later in my teens I discovered early music: Carlo Gesualdo, Luca Marenzio, Orlando di Lasso. I never came to terms with the Romanticism, which remains incomprehensible to me to this day. My taste in the visual arts was largely influenced by the artistic movements that surrounded me in my early years: my father's Abstractism was close to the currents of Op Art and Kinetic Art and to the Ulm school of Design.
    [Show full text]
  • Spectral Action Models of Gravity on Packed Swiss Cheese Cosmology 3
    SPECTRAL ACTION MODELS OF GRAVITY ON PACKED SWISS CHEESE COSMOLOGY ADAM BALL AND MATILDE MARCOLLI Abstract. We present a model of (modified) gravity on spacetimes with fractal structure based on packing of spheres, which are (Euclidean) variants of the Packed Swiss Cheese Cosmology models. As the action functional for gravity we consider the spectral action of noncommutative geometry, and we compute its expansion on a space obtained as an Apol- lonian packing of 3-dimensional spheres inside a 4-dimensional ball. Using information from the zeta function of the Dirac operator of the spectral triple, we compute the leading terms in the asymptotic expansion of the spectral action. They consist of a zeta regularization of a divergent sum which involves the leading terms of the spectral actions of the individual spheres in the packing. This accounts for the contribution of the points 1 and 3 in the dimension spectrum (as in the case of a 3-sphere). There is an additional term coming from the residue at the additional point in the real dimension spectrum that corresponds to the packing constant, as well as a series of fluctuations coming from log-periodic oscillations, created by the points of the dimension spectrum that are off the real line. These terms detect the fractality of the residue set of the sphere packing. We show that the presence of fractality influences the shape of the slow-roll potential for inflation, obtained from the spectral action. We also discuss the effect of truncating the fractal structure at a certain scale related to the energy scale in the spectral action.
    [Show full text]
  • UNCONDITIONAL NONCOMMUTATIVE MOTIVIC GALOIS GROUPS 3 Is Conservative; Consult [2, §1]
    UNCONDITIONAL NONCOMMUTATIVE MOTIVIC GALOIS GROUPS MATILDE MARCOLLI AND GONC¸ALO TABUADA Abstract. In this short note we introduce the unconditional noncommutative motivic Galois groups and relate them with those of Andr´e-Kahn. Dedicated to Herb Clemens, on the occasion of his non-retirement. Motivating questions Motivic Galois groups were introduced by Grothendieck in the sixties as part of his broad theory of (pure) motives. These group schemes are conditional in the sense that their construction makes use of the standard conjectures. Thanks to Kontsevich [6, 7, 8], Grothendieck’s theory of motives admits a noncommutative counterpart, with schemes replaced by dg categories. The standard conjectures admit noncommutative analogues and there exist also conditional noncommutative motivic Galois groups; consult [10, 11, 12] for details. Recently, via an evolved “⊗-categorification” of the Wedderburn-Malcev’s theo- rem, Andr´e-Kahn [2] introduced unconditional motivic Galois groups. These group schemes GalH (attached to a Weil cohomology theory H) are well-defined up to an interior automorphism and do not require the assumption of any of Grothendieck’s standard conjectures. This lead us naturally to the following motivating questions: NC Q1: Do the Galois groups GalH admit noncommutative analogues GalH ? NC Q2: What is the relation between GalH and GalH ? NC Q3: What is the relation between GalH and the conditional Galois groups ? In this short note we provide precise answers to these three questions; see Defi- nition 2.8, Theorem 3.2, and Proposition 4.2, respectively. 1. Preliminaries Let k be a base field and F a field of coefficients. The classical idempotent arXiv:1112.5422v2 [math.KT] 22 Feb 2014 completion construction will be denoted by (−)♮.
    [Show full text]
  • Arxiv:Math/0407480V1
    ARCHIMEDEAN COHOMOLOGY REVISITED CATERINA CONSANI‡ AND MATILDE MARCOLLI† 1. Introduction C. Deninger produced a unified description of the local factors at arithmetic infinity and at the fi- nite places where the local Frobenius acts semi-simply, in the form of a Ray–Singer determinant of a “logarithm of Frobenius” Φ on an infinite dimensional vector space (the archimedean cohomology Har· (X) at the archimedean places, cf. [11]). The first author gave a cohomological interpretation of , the space Har· (X), in terms of a double complex K· · of real differential forms on a smooth projective algebraic variety X (over C or R), with Tate-twists and suitable cutoffs, together with an endomor- phism N, which represents a “logarithm of the local monodromy at arithmetic infinity”. Moreover, in this theory the cohomology of the complex Cone(N)· computes real Deligne cohomology of X (cf. [9]). The construction of [9] is motivated by a dictionary of analogies between the geometry of the tubular neighborhoods of the “fibers at arithmetic infinity” of an arithmetic variety X and the geometric theory of the limiting mixed Hodge structure of a degeneration over a disk. Thus, the formulation and notation used in [9] for the double complex and archimedean cohomology mimics the definition, in the geometric case, of a resolution of the complex of nearby cycles and its cohomology(cf. [28]). In Section 2 and 3 we give an equivalent description of Consani’s double complex, which allows us to investigate further the structure induced on the complex and the archimedean cohomology by the operators N, Φ, and the Lefschetz operator L.
    [Show full text]