Non-Critical String Theory Formulation of Microtubule Dynamics And

Total Page:16

File Type:pdf, Size:1020Kb

Non-Critical String Theory Formulation of Microtubule Dynamics And ACT-09/95 CERN-TH.127/95 CTP-TAMU-24/95 ENSLAPP-A|-/95 hep-ph/9505401 Non-Critical String Theory Formulation of Microtubule Dynamics and Quantum Asp ects of Brain Function a; b;c N.E. Mavromatos and D.V. Nanop oulos a Lab oratoire de Physique Theorique ENSLAPP (URA 14-36 du CNRS, asso ciee a l' E.N.S de Lyon, et au LAPP (IN2P3-CNRS) d'Annecy-le-Vieux), Chemin de Bellevue, BP 110, F-74941 Annecy-le-Vieux Cedex, France. b Texas A & M University, College Station, TX 77843-424 2, USA and Astroparticle Physics Group, Houston Advanced Research Center (HARC), The Mitchell Campus, Wo o dlands, TX 77381, USA. c CERN, Theory Division, Geneva 23 Switzerland Abstract Microtubule (MT) networks, subneural paracrystalline cytosceletal structures, seem to play a fundamental role in the neurons. We cast here the complicated MT dynamics in processed by the SLAC/DESY Libraries on 30 May 1995. 〉 the form of a 1 + 1-dimensional non-critical string theory,thus enabling us to provide a consistent quantum treatment of MTs, including enviromental friction e ects. We suggest, thus, that the MTs are the microsites, in the brain, for the emergence of stable, macroscopic PostScript quantum coherent states, identi able with the preconscious states. Quantum space-time e ects, as describ ed by non-critical string theory, trigger then an organizedcol lapse of the coherent states down to a sp eci c or conscious state. The whole pro cess we estimate to take O (1 sec), in excellent agreement with a plethora of exp erimental/observational ndings. The microscopic arrow of time, endemic in non-critical string theory, and apparent here in the self-collapse pro cess, provides a satisfactory and simple resolution to the age-old problem of how the, central to our feelings of awareness, sensation of the progression of time is generated. ACT-09/95 CERN-TH.127/95 HEP-PH-9505401 CTP-TAMU-24/95 ENSLAPP-A|-/95 May 1995 On leave from P.P.A.R.C. Advanced Fellowship, Dept. of Physics (Theoretical Physics), University of Oxford, 1 Keble Road, Oxford OX1 3NP, U.K. 1 Intro duction The interior of living cells is structurally and dynamically organized by cytoskele- tons, i.e. networks of protein p olymers. Of these structures, MicroTubules (MT) app ear to b e [1] the most fundamental. Their dynamics has b een studied recently by anumb er of authors in connection with the mechanism resp onsible for dissipation- free energy transfer. Recently, Hamero and Penrose [2] have conjectured another fundamental ro ^le for the MT, namely b eing resp onsible for quantum computations in the human brain, and, thus, related to the consciousness of the human mind. The latter is argued to b e asso ciated with certain asp ects of quantum theory [3] that are b elieved to o ccur in the cytoskeleton MT, in particular quantum sup er- p osition and subsequent collapse of the wave function of coherentMTnetworks. While quantum sup erp osition is a well-established and well-understo o d prop erty of quantum physics, the collapse of the wave function has b een always enigmatic. We prop ose here to use an explicit string-derived mechanism - in one interpreta- tion of non-critical string theory - for the collapse of the wave function[4], involving quantum gravity in an essential way and solidifying previous intuitively plausible suggestions[5 , 6]. It is an amazing surprise that quantum gravity e ects, of order of 1=2 19 magnitude G m 10 , with G Newton's gravitational constant and m the p N p N proton mass, can playa r^ole in suchlow energies as the eV scales of the typical energy transfer that o ccurs in cytoskeleta. However, as we show in this article, the ne details of the MT characteristic structure indicate that not only is this con- ceivable, but such scenaria lead to order of magnitude estimates for the time scales entering conscious perception that are close enough to those conjectured/\observed" by neuroscientists, based on completely di erent grounds. To understand how quantum space-time e ects can a ect conscious p erception, we mention that it has long b een susp ected [7] that large scale quantum coherent phenomena can o ccur in the interior of biological cells, as a result of the existence of ordered water molecules. Quantum mechanical vibrations of the latter are re- sp onsible for the app earance of `phonons' similar in nature to those asso ciated with sup erconductivity. In fact there is a close analogy b etween sup erconductivity and energy transfer in biological cells. In the former phenomenon electric currentis transferred without dissipation in the surface of the sup erconductor. In biological cells, as we shall discuss later on, energy is transferred through the cell without loss, despite the existence of frictional forces that represent the interaction of the cell with the surrounding water molecules [8]. Such large scale quantum coherent states can maintain themselves for up to O (1 sec), without signi cantenvironmental entanglement. After that time, the state undergo es self-collapse, probably due to quantum gravity e ects. Due to quantum transitions b etween the di erent states of the quantum system of MT in certain parts of the human brain, a sucient dis- tortion of the surrounding space-time o ccurs, so that a microscopic (Planck size) black hole is formed. Then collapse is induced, with a collapse time that dep ends on the order of magnitude of the number N of coherent microtubulins. It is estimated 12 that, with an N = O [10 ], the collapse time of O (1 sec ), which app ears to b e a typical time scale of conscious events, is achieved. Taking into account that exp eri- 8 ments have shown that there exist N =10 tubulins p er neuron, and that there are 11 10 neurons in the brain, it follows that that this order of magnitude for N refers 7 to a fraction 10 of the human brain, whichisvery close to the fraction b elieved resp onsible for human p erception. The self-collapse of the MT coherent state wave function is an essential step for the op eration of the MT network as a quantum computer. In the past it has b een suggested that MT networks pro cessed information in a way similar to classical cellular automata (CCA) [9]. These are describ ed byinteracting Ising spin chains on the spatial plane obtained by leting op en and attening the MT cylindrical surface. Distortions in the con gurations of individual parts of the spin chain can b e in uenced by the environmental spins, leading to information pro cessing. In view of the suggestion [2] on viewing the conscious parts of the human mind as quantum computers, one might extend the concept of the CCA to a quantum cellular automaton (QCA), undergoing wave function self-collapses due to (quantum gravity) enviromental entanglement. An interesting and basic issue that arises in connection with the ab over^ole of the brain as a quantum computer is the emergence of a direction in the ow of time (arrow). The latter could b e the result of succesive self-collapses of the system's wave function. In a recent series of pap ers [4] wehave suggested a rather detailed mechanism by whichan irreversible time variable has emerged in certain mo dels of string quantum gravity. The mo del utilized string particles propagating in singular space-time backgrounds with event horizons. Consistency of the string approach requires conformal invariance of the asso ciated -mo del, which in turn implies a coupling of the backgrounds for the propagating string mo des to an in nity of global (quasi-top ological) delo calized mo des at higher (massive) string levels. The existence of such couplings is necessitated by sp eci c coherence-preserving target space gauge symmetries that mix the string levels [4]. The sp eci c mo del of ref. [4] is a completely integrable string theory, in the sense of b eing characterised by an in nity of conserved charges. This can b e intuitively understo o d by the fact that the mo del is a (1 + 1)-dimensional Liouville string, and as such it can b e mapp ed to a theory of essentially free fermions on a discretized world sheet (matrix mo del approach [10 ]). A system of free fermions in (1 + 1) dimen- sions is trivially completely integrable, the in nity of the conserved charges b eing provided by appropriate moments of the fermion energies ab ove the Fermi surface. Of course, formally, the precise symmetries of the mo del used in ref. [4] are much more complicated [11], but the idea b ehind the mo del's integrability is essentially the ab ove. It is our b elief that this quantum integrabilityisavery imp ortant feature of theories of space-time asso ciated with the time arrow. In its presence, theories with singular backgrounds app ear consistent as far as maintainance of quantum co- herence is concerned. This is due to the fact that the phase-space density of the eld theory asso ciated with the matter degrees of freedom evolves with time according to the conventional Liouville theorem[4] @ = f; H g (1) t PB as a consequence of phase-space volume-preserving symmetries. In the two-dimensional example of ref. [4], these symmetries are known as W , and are asso ciated with 1 higher spin target-space states[11 ]. They are resp onsible for string-level mixing, and hence they are broken in anylow-energy approximation.
Recommended publications
  • Report of the Supersymmetry Theory Subgroup
    Report of the Supersymmetry Theory Subgroup J. Amundson (Wisconsin), G. Anderson (FNAL), H. Baer (FSU), J. Bagger (Johns Hopkins), R.M. Barnett (LBNL), C.H. Chen (UC Davis), G. Cleaver (OSU), B. Dobrescu (BU), M. Drees (Wisconsin), J.F. Gunion (UC Davis), G.L. Kane (Michigan), B. Kayser (NSF), C. Kolda (IAS), J. Lykken (FNAL), S.P. Martin (Michigan), T. Moroi (LBNL), S. Mrenna (Argonne), M. Nojiri (KEK), D. Pierce (SLAC), X. Tata (Hawaii), S. Thomas (SLAC), J.D. Wells (SLAC), B. Wright (North Carolina), Y. Yamada (Wisconsin) ABSTRACT Spacetime supersymmetry appears to be a fundamental in- gredient of superstring theory. We provide a mini-guide to some of the possible manifesta- tions of weak-scale supersymmetry. For each of six scenarios These motivations say nothing about the scale at which nature we provide might be supersymmetric. Indeed, there are additional motiva- tions for weak-scale supersymmetry. a brief description of the theoretical underpinnings, Incorporation of supersymmetry into the SM leads to a so- the adjustable parameters, lution of the gauge hierarchy problem. Namely, quadratic divergences in loop corrections to the Higgs boson mass a qualitative description of the associated phenomenology at future colliders, will cancel between fermionic and bosonic loops. This mechanism works only if the superpartner particle masses comments on how to simulate each scenario with existing are roughly of order or less than the weak scale. event generators. There exists an experimental hint: the three gauge cou- plings can unify at the Grand Uni®cation scale if there ex- I. INTRODUCTION ist weak-scale supersymmetric particles, with a desert be- The Standard Model (SM) is a theory of spin- 1 matter tween the weak scale and the GUT scale.
    [Show full text]
  • Off-Shell Interactions for Closed-String Tachyons
    Preprint typeset in JHEP style - PAPER VERSION hep-th/0403238 KIAS-P04017 SLAC-PUB-10384 SU-ITP-04-11 TIFR-04-04 Off-Shell Interactions for Closed-String Tachyons Atish Dabholkarb,c,d, Ashik Iqubald and Joris Raeymaekersa aSchool of Physics, Korea Institute for Advanced Study, 207-43, Cheongryangri-Dong, Dongdaemun-Gu, Seoul 130-722, Korea bStanford Linear Accelerator Center, Stanford University, Stanford, CA 94025, USA cInstitute for Theoretical Physics, Department of Physics, Stanford University, Stanford, CA 94305, USA dDepartment of Theoretical Physics, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India E-mail:[email protected], [email protected], [email protected] Abstract: Off-shell interactions for localized closed-string tachyons in C/ZN super- string backgrounds are analyzed and a conjecture for the effective height of the tachyon potential is elaborated. At large N, some of the relevant tachyons are nearly massless and their interactions can be deduced from the S-matrix. The cubic interactions be- tween these tachyons and the massless fields are computed in a closed form using orbifold CFT techniques. The cubic interaction between nearly-massless tachyons with different charges is shown to vanish and thus condensation of one tachyon does not source the others. It is shown that to leading order in N, the quartic contact in- teraction vanishes and the massless exchanges completely account for the four point scattering amplitude. This indicates that it is necessary to go beyond quartic inter- actions or to include other fields to test the conjecture for the height of the tachyon potential. Keywords: closed-string tachyons, orbifolds.
    [Show full text]
  • UV Behavior of Half-Maximal Supergravity Theories
    UV behavior of half-maximal supergravity theories. Piotr Tourkine, Quantum Gravity in Paris 2013, LPT Orsay In collaboration with Pierre Vanhove, based on 1202.3692, 1208.1255 Understand the pertubative structure of supergravity theories. ● Supergravities are theories of gravity with local supersymmetry. ● Those theories naturally arise in the low energy limit of superstring theory. ● String theory is then a UV completion for those and thus provides a good framework to study their UV behavior. → Maximal and half-maximal supergravities. Maximal supergravity ● Maximally extended supergravity: – Low energy limit of type IIA/B theory, – 32 real supercharges, unique (ungauged) – N=8 in d=4 ● Long standing problem to determine if maximal supergravity can be a consistent theory of quantum gravity in d=4. ● Current consensus on the subject : it is not UV finite, the first divergence could occur at the 7-loop order. ● Impressive progresses made during last 5 years in the field of scattering amplitudes computations. [Bern, Carrasco, Dixon, Dunbar, Johansson, Kosower, Perelstein, Rozowsky etc.] Half-maximal supergravity ● Half-maximal supergravity: – Heterotic string, but also type II strings on orbifolds – 16 real supercharges, – N=4 in d=4 ● Richer structure, and still a lot of SUSY so explicit computations are still possible. ● There are UV divergences in d=4, [Fischler 1979] at one loop for external matter states ● UV divergence in gravity amplitudes ? As we will see the divergence is expected to arise at the four loop order. String models that give half-maximal supergravity “(4,0)” susy “(0,4)” susy ● Type IIA/B string = Superstring ⊗ Superstring Torus compactification : preserves full (4,4) supersymmetry.
    [Show full text]
  • Photon-Graviton Amplitudes N
    Photon-graviton amplitudes N. Ahmadiniaz, F. Bastianelli, O. Corradini, José M. Dávila, and C. Schubert Citation: AIP Conference Proceedings 1548, 221 (2013); doi: 10.1063/1.4817048 View online: http://dx.doi.org/10.1063/1.4817048 View Table of Contents: http://scitation.aip.org/content/aip/proceeding/aipcp/1548?ver=pdfcov Published by the AIP Publishing This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 128.148.231.12 On: Mon, 03 Feb 2014 23:34:26 Photon-Graviton Amplitudes † ‡ N. Ahmadiniaz∗, F. Bastianelli , O. Corradini∗∗, José M. Dávila and C. Schubert∗ ∗Instituto de Física y Matemáticas, Universidad Michoacana de San Nicolás de Hidalgo, Edificio C-3, Apdo. Postal 2-82, C.P. 58040, Morelia, Michoacán, México. †Dipartimento di Fisica ed Astronomia, Università di Bologna and INFN, Sezione di Bologna, Via Irnerio 46, I-40126 Bologna, Italy. ∗∗Centro de Estudios en Física y Matemáticas Básicas y Aplicadas, Universidad Autónoma de Chiapas, C.P. 29000, Tuxtla Gutiérrez, México, and Dipartimento di Scienze Fisiche, Informatiche e Matematiche, Universitá di Modena e Reggio Emilia, Via Campi 213/A, I-41125 Modena, Italy. ‡Facultad de Ciencias, Universidad Autónoma del Estado de México, Instituto Literario 100, Toluca 50000, México. Abstract. We report on an ongoing study of the one-loop photon-graviton amplitudes, using both effective action and worldline techniques. The emphasis is on Kawai-Lewellen-Tye-like relations. Keywords: Photon-graviton, KLT, worldline formalism PACS: 04.60.-m, 04.62.+v MOTIVATIONS In 1986 Kawai, Lewellen and Tye [1] found a relation between tree-level amplitudes in open and closed string theory which in the field theory limit also implies relations between amplitudes in gauge theory and in gravity.
    [Show full text]
  • Tachyonic Dark Matter
    Tachyonic dark matter P.C.W. Davies Australian Centre for Astrobiology Macquarie University, New South Wales, Australia 2109 [email protected] Abstract Recent attempts to explain the dark matter and energy content of the universe have involved some radical extensions of standard physics, including quintessence, phantom energy, additional space dimensions and variations in the speed of light. In this paper I consider the possibility that some dark matter might be in the form of tachyons. I show that, subject to some reasonable assumptions, a tachyonic cosmological fluid would produce distinctive effects, such as a surge in quantum vacuum energy and particle creation, and a change in the conventional temperature-time relation for the normal cosmological material. Possible observational consequences are discussed. Keywords: tachyons, cosmological models, dark matter 1 1. Tachyons in an expanding universe In this section I consider the behaviour of a tachyon in an expanding universe, following the treatment in Davies (1975). A tachyon is a particle with imaginary mass iµ (µ real and positive), velocity v > c and momentum and energy given in a local inertial frame by p = µv(v2 – 1)-1/2 (1.1) E = µ(v2 – 1)-1/2 (1.2) where here and henceforth I choose units with c = ħ =1. Consider such a particle moving in a Friedmann-Roberston-Walker (FRW) universe with scale factor a(t), t being the cosmic time. In a short time dt, the particle will have moved a distance vdt to a point where the local comoving frame is retreating at a speed dv = (a′/a)vdt, where a′ = da/dt.
    [Show full text]
  • Pions As Gluons in Higher Dimensions Arxiv:1709.04932V1
    CALT-TH-2017-051 Pions as Gluons in Higher Dimensions Clifford Cheung,a Grant N. Remmen,b,c Chia-Hsien Shen,d and Congkao Wena,d aWalter Burke Institute for Theoretical Physics, California Institute of Technology, Pasadena, CA 91125 bBerkeley Center for Theoretical Physics, Department of Physics, University of California, Berkeley, CA 94720 cTheoretical Physics Group, Lawrence Berkeley National Laboratory, Berkeley, CA 94720 dMani L. Bhaumik Institute for Theoretical Physics, Department of Physics and Astronomy, UCLA, Los Angeles, CA 90095 Abstract We derive the nonlinear sigma model as a peculiar dimensional reduction of Yang-Mills theory. In this framework, pions are reformulated as higher-dimensional gluons arranged in a kinematic configuration that only probes the cubic interactions. Via this procedure we obtain a purely cubic nonlinear sigma action which exhibits a symmetry enforcing color-kinematics duality. Remarkably, the associated kinematic algebra originates directly from the Poincaré algebra in higher dimensions. Applying the same construction to gravity yields a new quartic action for Born-Infeld theory and, applied once more, a cubic action for the special Galileon theory. Since the nonlinear sigma model and special Galileon are subtly encoded in the cubic sectors of Yang-Mills theory and gravity, respectively, their double copy relationship is automatic. arXiv:1709.04932v1 [hep-th] 14 Sep 2017 e-mail: cliff[email protected], [email protected], [email protected], [email protected] Contents 1 Introduction 3 2 Amplitudes Preamble3 2.1 Unifying Relations for Amplitudes . .4 2.2 Transmutation as Special Kinematics . .5 3 From Gluons to Pions6 3.1 Dimensional Reduction to the Nonlinear Sigma Model .
    [Show full text]
  • Bastianelli F., Corradini O., D Vila J.M., Schubert C. Photon-Graviton
    ”ˆ‡ˆŠ ‹…Œ…’›• —‘’ˆ– ˆ ’Œƒ Ÿ„ 2012. ’. 43. ‚›. 5 PHOTONÄGRAVITON AMPLITUDES FROM THE EFFECTIVE ACTION F. Bastianelli 1 , O. Corradini 1,2,J.M.Davilaà 3, C. Schubert 3 1Dipartimento di Fisica, Universita di Bologna and INFN, Sezione di Bologna, Bologna, Italy 2Centro de Estudios en FÃsica y Matematicasà Basicasà y Aplicadas, Universidad Autonomaà de Chiapas, Tuxtla Gutierrez,à Mexicoà 3Instituto de FÃsica y Matematicas,à Universidad Michoacana de San Nicolasà de Hidalgo, Morelia, Michoacan,à Mexicoà We report on the status of an ongoing effort to calculate the complete one-loop low-energy effective actions in the EinsteinÄMaxwell theory with a massive scalar or spinor loop, and to use them for obtaining the explicit form of the corresponding M-graviton/N-photon amplitudes. We present explicit results for the effective actions at the one-graviton four-photon level and for the amplitudes at the one-graviton two-photon level. As expected on general grounds, these amplitudes relate in a simple way to the corresponding four-photon amplitudes. We also derive the gravitational Ward identity for the 1PI one-graviton Ä N-photon amplitude. PACS: 14.70.Kv INTRODUCTION In string theory, the prototypical example of relations between gravity and gauge theory amplitudes are the ®KLT¯ relations discovered by Kawai et al. [1]. Schematically, they are of the form (gravity amplitude) ∼ (gauge amplitude)2 and follow naturally from the factorization of the graviton vertex operator into a product of two gauge boson vertex operators (see, e.g., [2]): closed open ¯ open V = Vleft Vright . (1) These string relations induce also relations in ˇeld theory.
    [Show full text]
  • Three Graviton Scattering and Recoil Effects in Matrix Theory
    Quantum Aspects of Gauge Theories, Supersymmetry and Unification, Paris, 1999 PROCEEDINGS Three graviton scattering and recoil effects in Matrix theory A. Refollia ,N.Terzib and D. Zanonb a Instituut voor Theoretische Fysica, Katholieke Universiteit Leuven Celestijnenlaan 200D B-3001 Leuven, Belgium E-mail: [email protected] b Dipartimento di Fisica dell'Universit`adiMilanoand INFN, Sezione di Milano, Via Celoria 16,20133 Milano, Italy E-mail: [email protected] E-mail: [email protected] Abstract: We discuss recent results on three gravitons in M-atrix theory at finite N.Witha specific choice of the background we obtain the complete result up to two loops. The contributions from three-body forces agree with the ones presented in recent papers. We evaluate the two–body exchanges as well. We show that the result we have obtained from M-atrix theory precisely matches the result from one-particle reducible tree diagrams in eleven-dimensional supergravity . -theory seems to be a consistent quan- that they perfectly reproduce the three gravi- M tum theory which includes eleven dimen- ton scattering in supergravity, both in the di- sional supergravity as a low-energy approxima- rect three-body channel and in the two-body re- tion. Since the introduction of the matrix model coil exchange. The former, which corresponds to of M-theory [1] much progress has been made one-particle irreducible diagrams in supergravity, on the subject. According to the original conjec- has been computed in the first paper of ref. [6] ture, the degrees of freedom of M-theory in the and we confirm that result.
    [Show full text]
  • Introduction to Supersymmetry
    Introduction to Supersymmetry Pre-SUSY Summer School Corpus Christi, Texas May 15-18, 2019 Stephen P. Martin Northern Illinois University [email protected] 1 Topics: Why: Motivation for supersymmetry (SUSY) • What: SUSY Lagrangians, SUSY breaking and the Minimal • Supersymmetric Standard Model, superpartner decays Who: Sorry, not covered. • For some more details and a slightly better attempt at proper referencing: A supersymmetry primer, hep-ph/9709356, version 7, January 2016 • TASI 2011 lectures notes: two-component fermion notation and • supersymmetry, arXiv:1205.4076. If you find corrections, please do let me know! 2 Lecture 1: Motivation and Introduction to Supersymmetry Motivation: The Hierarchy Problem • Supermultiplets • Particle content of the Minimal Supersymmetric Standard Model • (MSSM) Need for “soft” breaking of supersymmetry • The Wess-Zumino Model • 3 People have cited many reasons why extensions of the Standard Model might involve supersymmetry (SUSY). Some of them are: A possible cold dark matter particle • A light Higgs boson, M = 125 GeV • h Unification of gauge couplings • Mathematical elegance, beauty • ⋆ “What does that even mean? No such thing!” – Some modern pundits ⋆ “We beg to differ.” – Einstein, Dirac, . However, for me, the single compelling reason is: The Hierarchy Problem • 4 An analogy: Coulomb self-energy correction to the electron’s mass A point-like electron would have an infinite classical electrostatic energy. Instead, suppose the electron is a solid sphere of uniform charge density and radius R. An undergraduate problem gives: 3e2 ∆ECoulomb = 20πǫ0R 2 Interpreting this as a correction ∆me = ∆ECoulomb/c to the electron mass: 15 0.86 10− meters m = m + (1 MeV/c2) × .
    [Show full text]
  • Chapter 9: the 'Emergence' of Spacetime in String Theory
    Chapter 9: The `emergence' of spacetime in string theory Nick Huggett and Christian W¨uthrich∗ May 21, 2020 Contents 1 Deriving general relativity 2 2 Whence spacetime? 9 3 Whence where? 12 3.1 The worldsheet interpretation . 13 3.2 T-duality and scattering . 14 3.3 Scattering and local topology . 18 4 Whence the metric? 20 4.1 `Background independence' . 21 4.2 Is there a Minkowski background? . 24 4.3 Why split the full metric? . 27 4.4 T-duality . 29 5 Quantum field theoretic considerations 29 5.1 The graviton concept . 30 5.2 Graviton coherent states . 32 5.3 GR from QFT . 34 ∗This is a chapter of the planned monograph Out of Nowhere: The Emergence of Spacetime in Quantum Theories of Gravity, co-authored by Nick Huggett and Christian W¨uthrich and under contract with Oxford University Press. More information at www.beyondspacetime.net. The primary author of this chapter is Nick Huggett ([email protected]). This work was sup- ported financially by the ACLS and the John Templeton Foundation (the views expressed are those of the authors not necessarily those of the sponsors). We want to thank Tushar Menon and James Read for exceptionally careful comments on a draft this chapter. We are also grateful to Niels Linnemann for some helpful feedback. 1 6 Conclusions 35 This chapter builds on the results of the previous two to investigate the extent to which spacetime might be said to `emerge' in perturbative string the- ory. Our starting point is the string theoretic derivation of general relativity explained in depth in the previous chapter, and reviewed in x1 below (so that the philosophical conclusions of this chapter can be understood by those who are less concerned with formal detail, and so skip the previous one).
    [Show full text]
  • Soft Theorems for the Gravity Dilaton and the Nambu-Goldstone Boson Dilaton
    Soft theorems for the Gravity Dilaton and the Nambu-Goldstone Boson Dilaton Raffaele Marotta INFN Naples GGI April 2019 Talk based on: . P. Di Vecchia, R. M., M. Mojaza, JHEP 1901 (2019) 038 + work in progress. P. Di Vecchia, R. M., M. Mojaza, JHEP 1710(2017)017 . P. Di Vecchia, R.M. , M. Mojaza, J. Nohle, Phys. Rev D93 (2016) n.8, 080515. Plan of the talk • Motivations • Soft theorems in spontaneously broken conformal field theories. • Soft theorems from tree level string amplitudes • Multiloop soft theorems in bosonic string theory • Conclusions. Motivations • It is well know that scattering amplitudes in the deep infrared region (or soft limit) satisfy interesting relations. Low’s theorem: Amplitudes with a soft photon are determined from the corresponding amplitude without the soft particle 푝1 푝1 푝 Soft-photon 2 푞 → 0 푛 = ෍ 퐼=1 푝푖 푝푛 Soft-photon polarization 푒푖 charge of the particle smooth in the soft limit Weinberg: Amplitudes involving gravitons and matter particles show and universal behavior when one graviton becomes soft. They were recognized to be a consequence of the gauge invariance Soft-Photon Soft-graviton Adler’s zero (Weiberg, The Quatum Theory of Fields Vol .II.) • Goldstone theorem: When a symmetry G is spontaneously broken to a sub-group H the spectrum of the theory contains as many Goldston bosons 휋푎, parametrizing the 퐺 coset space Τ퐻 . • 푇푖, 푋푎 are the unbroken and broken generators, 푖 푎 respectively. 퐽 휇, 퐽 휇 are the corresponding currents. 푎 • The matrix elements of the broken currents 퐽휇 are: • The matrix element of a broken current between arbitrary states I, j, has two contributions: 푎 푎 퐽 휇 퐽 휇 Goldstone pole No-pole contribution to F is the “decay constant” dominance the matrix element of for 푞2 → 0 the current.
    [Show full text]
  • The Graviton Shlomo Barak
    The Graviton Shlomo Barak To cite this version: Shlomo Barak. The Graviton. 2017. hal-01524355 HAL Id: hal-01524355 https://hal.archives-ouvertes.fr/hal-01524355 Preprint submitted on 18 May 2017 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. The Graviton Shlomo Barak Taga Innovations 16 Beit Hillel St. Tel Aviv 670017 Israel Corresponding author: [email protected] Abstract Gravitational waves have recently been detected. These space waves are predicted by General Relativity. As of today, there is no theoretical proof, or observational evidence, for the existence of quanta of these waves. These quanta are considered by some to be the “force- carrying” mediators between masses - the Gravitons. In this paper we suggest a model of the, as yet hypothetical, Graviton. We also relate to the effort to quantize gravitation, and raise arguments in support of the existence of Gravitons. Key Words: Gravitation, Graviton, Gravitational Wave, General Relativity 1 1 Introduction 1.1 The Graviton The graviton is expected to be a massless spin-2 boson. The nature of the expected graviton is discussed, in a very clear and compact way, in the introduction by Brian Hatfield (Spin of the Graviton and Antigravity) to the book: Feynman Lectures on Gravitation [1].
    [Show full text]