Weak Gravity Conjecture Constraints on the SM and Beyond

Total Page:16

File Type:pdf, Size:1020Kb

Weak Gravity Conjecture Constraints on the SM and Beyond Weak Gravity Conjecture constraints on the SM and Beyond Víctor Martín Lozano Universität Bonn Bethe Center for Theoretica Physics "#anez$ M-L, Valenzue a &'()*+),-./0 234! '('' 5/)'(6 0** "#anez$ M-L, Valenzue a &'()(+),1''0 Víctor Martín Lozano % Uni Bonn SUSY /)'8 Introduction Naturalness problems: Cosmological constant EW hierarchy problem Víctor Martín Lozano % Uni Bonn SUSY /)'8 Introduction Naturalness problems: Cosmological constant EW hierarchy problem LHC Víctor Martín Lozano % Uni Bonn SUSY /)'8 Introduction Naturalness problems: Cosmological constant † EW hierarchy problem LHC † Yet, so far... Víctor Martín Lozano % Uni Bonn SUSY /)'8 Introduction Naturalness problems: Cosmological constant EW hierarchy problem LHC Numerical Coincidence: Víctor Martín Lozano % Uni Bonn SUSY /)'8 Introduction !bsence of New #hysics forces us to think di%erently about the guiding principles of HE# Maybe the U( structure is telling us ho" the IR should beha*e +uantum ,ra*ity Constraints Víctor Martín Lozano % Uni Bonn SUSY /)'8 Quantum Gravity Constraints Not e*erything is possible within -tring Theory/+uantum Gra*ity Víctor Martín Lozano % Uni Bonn SUSY /)'8 Quantum Gravity Constraints Not e*erything is possible within -tring Theory/+uantum Gra*ity Not e*ery e%ecti*e theory can be embedded in Q,: -"ampland!0 1(afa 2345 Víctor Martín Lozano % Uni Bonn SUSY /)'8 Quantum Gravity Constraints #icture by Irene (alenzuela Víctor Martín Lozano % Uni Bonn SUSY /)'8 Quantum Gravity Conjectures Guiding principles to build an e%ecti*e theory consistent with +, Common features of the string landscape, model building failures, blac$ hole arguments. -Absence of global symmetries 1:an$s8;ison 2<<5 1Horo"it6, Strominger, Seiberg. 5 -Completeness hypothesis 1#olchins$i 23=5 -Wea$ ,ra*ity Conjecture 1!r$ani8Hamed et al 2345 8-"ampland constraints about the moduli space 1>oguri8(afa 2345 .hese conjectures could ha*e a signi9cant impact on low energy physics00 Víctor Martín Lozano % Uni Bonn SUSY /)'8 Weak Gravity Conjecture 1!r$ani8Hamed et al 2345 In theories of +G with a p-form gauge field, there must be an electrically charged object with charge Q and tension T such that: In order to allo" for e?tremal blac$ holes to decay (remnants) ,ra*ity must be al"ays "ea$er than any other interaction Víctor Martín Lozano % Uni Bonn SUSY /)'8 Weak Gravity Conjecture 1!r$ani8Hamed et al 2345 In theories of +G with a p-form gauge field, there must be an electrically charged object with charge Q and tension T such that: In order to allo" for e?tremal blac$ holes to decay (remnants) ,ra*ity must be al"ays "ea$er than any other interaction -harpened version of the WGC: 1>oguri 8 (afa 2B45 Non-S'-Y AdS *acua cannot be consistent with Q, 8It also applies to lo"er dimensional *acua 8.he !dS vacua must be stable Víctor Martín Lozano % Uni Bonn SUSY /)'8 Weak Gravity Conjecture 1!r$ani8Hamed et al 2345 In theories of +G with a p-form gauge field, there must be an electrically charged object with charge Q and tension T such that: In order to allo" for e?tremal blac$ holes to decay (remnants) ,ra*ity must be al"ays "ea$er than any other interaction -harpened version of the WGC: 1>oguri 8 (afa 2B45 Non-S'-Y AdS *acua cannot be consistent with Q, -M compacti9cations should be also consistent with Q, Víctor Martín Lozano % Uni Bonn SUSY /)'8 Compactifications of the SM to 3D 1!r$ani8Hamed et al 23D5 Standard &odel + ,ravity on : 1!rnold8Eornal8Wise 2B35 Casimir Energy >ne-loop corrections: , ;epending on the light mass spectra and the c.c we could get !dS *acua00 Looking at the whole spectrum one can 9nd inconsistencies that can be sol*ed assuming -'-Y for instance 1,on6alo, Herráez, IbFGez 2B<5 Víctor Martín Lozano % Uni Bonn SUSY /)'8 Compactifications of the SM to 3D Standard &odel + ,ravity on : Víctor Martín Lozano % Uni Bonn SUSY /)'8 Compactifications of the SM to 3D Standard &odel + ,ravity on : Víctor Martín Lozano % Uni Bonn SUSY /)'8 Compactifications of the SM to 3D Standard &odel + ,ravity on : Normal Inverted Hierarchy Hierarchy @NHA @IH) Víctor Martín Lozano % Uni Bonn SUSY /)'8 Compactifications of the SM to 3D Standard &odel + ,ravity on : Majorana Neutrinos Víctor Martín Lozano % Uni Bonn SUSY /)'8 Compactifications of the SM to 3D Standard &odel + ,ravity on : ;irac Neutrinos Víctor Martín Lozano % Uni Bonn SUSY /)'8 Constraints on neutrino masses Majorana Neutrinos !dS vacuum for any *alue of )'LE; >'.0 ;irac Neutrinos NH IH No *acuum < 6.7 meV < 2.1 me( *acuum 4 7 meV < < 7.7 me( 2.1 me( H < 2.56 me( *acuum > 7.7 me( > 2.56 me( < 7.7 meV (NH) H 2.56 meV (IH) Víctor Martín Lozano % Uni Bonn SUSY /)'8 Lo"er bound on the Cosmological Constant &ajorana (DiracA Eirst argument to ha*e , not based on Cosmology Víctor Martín Lozano % Uni Bonn SUSY /)'8 'pper bound on the EW scale Majorana Neutrinos ;irac Neutrinos #arameters leading to a higher EW scale: Inconsistency with quantum gravity .here is also a lo"er bound: 1,on6alo, IbFGez 2B<5 Víctor Martín Lozano % Uni Bonn SUSY /)'8 :-& Physics : Weyl Fermion Majorana Neutrinos ;irac Neutrinos Víctor Martín Lozano % Uni Bonn SUSY /)'8 :-& Physics : Dirac Fermion Majorana Neutrinos ;irac Neutrinos Víctor Martín Lozano % Uni Bonn SUSY /)'8 :-& Physics : Axion .he presence of the a?ion ma$es the Majorana Neutrinos !dS vacuum deeper ;irac Neutrinos Víctor Martín Lozano % Uni Bonn SUSY /)'8 Conclusions Not e*ery effecti*e theory can be embedded into +, @+, conjectures) Consistency with Q, implies constraints low energy physics !dS Instability Conjecture + stability of 3D SM vacua: 8 Lo"er bound on the cosmological constant and upper bound on neutrino masses 8 Upper bound on the EW scale in terms of the c.c Víctor Martín Lozano % Uni Bonn SUSY /)'8 .
Recommended publications
  • String-Inspired Running Vacuum—The ``Vacuumon''—And the Swampland Criteria
    universe Article String-Inspired Running Vacuum—The “Vacuumon”—And the Swampland Criteria Nick E. Mavromatos 1 , Joan Solà Peracaula 2,* and Spyros Basilakos 3,4 1 Theoretical Particle Physics and Cosmology Group, Physics Department, King’s College London, Strand, London WC2R 2LS, UK; [email protected] 2 Departament de Física Quàntica i Astrofísica, and Institute of Cosmos Sciences (ICCUB), Universitat de Barcelona, Av. Diagonal 647, E-08028 Barcelona, Catalonia, Spain 3 Academy of Athens, Research Center for Astronomy and Applied Mathematics, Soranou Efessiou 4, 11527 Athens, Greece; [email protected] 4 National Observatory of Athens, Lofos Nymfon, 11852 Athens, Greece * Correspondence: [email protected] Received: 15 October 2020; Accepted: 17 November 2020; Published: 20 November 2020 Abstract: We elaborate further on the compatibility of the “vacuumon potential” that characterises the inflationary phase of the running vacuum model (RVM) with the swampland criteria. The work is motivated by the fact that, as demonstrated recently by the authors, the RVM framework can be derived as an effective gravitational field theory stemming from underlying microscopic (critical) string theory models with gravitational anomalies, involving condensation of primordial gravitational waves. Although believed to be a classical scalar field description, not representing a fully fledged quantum field, we show here that the vacuumon potential satisfies certain swampland criteria for the relevant regime of parameters and field range. We link the criteria to the Gibbons–Hawking entropy that has been argued to characterise the RVM during the de Sitter phase. These results imply that the vacuumon may, after all, admit under certain conditions, a rôle as a quantum field during the inflationary (almost de Sitter) phase of the running vacuum.
    [Show full text]
  • Swampland Conjectures
    Swampland Conjectures Pablo Soler - Heidelberg ITP Strings and Fields ’19 - YITP Kyoto String phenomenology & the swampland ` <latexit sha1_base64="EAxFprSVFYJYfuKS7d/uV4r6OYc=">AAAB7XicbVDLSgNBEOyNrxhfUY9eBoPgKeyKoMegF48RzAOSJcxOepMxszPLzKwQQv7BiwdFvPo/3vwbJ8keNLGgoajqprsrSgU31ve/vcLa+sbmVnG7tLO7t39QPjxqGpVphg2mhNLtiBoUXGLDciuwnWqkSSSwFY1uZ37rCbXhSj7YcYphQgeSx5xR66RmF4Xopb1yxa/6c5BVEuSkAjnqvfJXt69YlqC0TFBjOoGf2nBCteVM4LTUzQymlI3oADuOSpqgCSfza6fkzCl9EivtSloyV39PTGhizDiJXGdC7dAsezPxP6+T2fg6nHCZZhYlWyyKM0GsIrPXSZ9rZFaMHaFMc3crYUOqKbMuoJILIVh+eZU0L6qBXw3uLyu1mzyOIpzAKZxDAFdQgzuoQwMYPMIzvMKbp7wX7937WLQWvHzmGP7A+/wBlJiPHg==</latexit> p String/M-theory <latexit sha1_base64="8DaxENaOM20fupORTAiGRfmtnI4=">AAAB7XicbVDLSgNBEOyNrxhfUY9eBoPgKeyqoMeAF48RzAOSJcxOepMxszPLzKwQQv7BiwdFvPo/3vwbJ8keNLGgoajqprsrSgU31ve/vcLa+sbmVnG7tLO7t39QPjxqGpVphg2mhNLtiBoUXGLDciuwnWqkSSSwFY1uZ37rCbXhSj7YcYphQgeSx5xR66RmF4XomV654lf9OcgqCXJSgRz1Xvmr21csS1BaJqgxncBPbTih2nImcFrqZgZTykZ0gB1HJU3QhJP5tVNy5pQ+iZV2JS2Zq78nJjQxZpxErjOhdmiWvZn4n9fJbHwTTrhMM4uSLRbFmSBWkdnrpM81MivGjlCmubuVsCHVlFkXUMmFECy/vEqaF9XArwb3V5XaZR5HEU7gFM4hgGuowR3UoQEMHuEZXuHNU96L9+59LFoLXj5zDH/gff4AlKGPEg==</latexit> `s L<latexit sha1_base64="uD+wtoefsR0DkLrUP2Tpiynljx8=">AAAB6HicbVBNS8NAEJ3Ur1q/qh69LBbBU0lE0GNBBA8eWrAf0Iay2U7atZtN2N0IJfQXePGgiFd/kjf/jds2B219MPB4b4aZeUEiuDau++0U1tY3NreK26Wd3b39g/LhUUvHqWLYZLGIVSegGgWX2DTcCOwkCmkUCGwH45uZ335CpXksH8wkQT+iQ8lDzqixUuO+X664VXcOskq8nFQgR71f/uoNYpZGKA0TVOuu5ybGz6gynAmclnqpxoSyMR1i11JJI9R+Nj90Ss6sMiBhrGxJQ+bq74mMRlpPosB2RtSM9LI3E//zuqkJr/2MyyQ1KNliUZgKYmIy+5oMuEJmxMQSyhS3txI2oooyY7Mp2RC85ZdXSeui6rlVr3FZqd3mcRThBE7hHDy4ghrcQR2awADhGV7hzXl0Xpx352PRWnDymWP4A+fzB6RwjNM=</latexit>
    [Show full text]
  • Evidence for a Sublattice Weak Gravity Conjecture
    Evidence for a Sublattice Weak Gravity Conjecture The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters Citation Heidenreich, Ben, Matthew Reece, and Tom Rudelius. 2017. Evidence for a Sublattice Weak Gravity Conjecture. Journal of High Energy Physics 2017, 25. Citable link http://nrs.harvard.edu/urn-3:HUL.InstRepos:41392811 Terms of Use This article was downloaded from Harvard University’s DASH repository, and is made available under the terms and conditions applicable to Open Access Policy Articles, as set forth at http:// nrs.harvard.edu/urn-3:HUL.InstRepos:dash.current.terms-of- use#OAP Prepared for submission to JHEP Evidence for a Sublattice Weak Gravity Conjecture Ben Heidenreich,a;b Matthew Reece,a and Tom Rudeliusa aDepartment of Physics, Harvard University, Cambridge, MA 02138, USA bPerimeter Institute for Theoretical Physics, Waterloo, Ontario, Canada N2L 2Y5 E-mail: [email protected], [email protected], [email protected] Abstract: The Weak Gravity Conjecture postulates the existence of superextremal charged particles, i.e. those with mass smaller than or equal to their charge in Planck units. We present further evidence for our recent observation that in known examples a much stronger statement is true: an infinite tower of superextremal particles of different charges exists. We show that effective Kaluza-Klein field theories and perturbative string vacua respect the Sublattice Weak Gravity Conjecture, namely that a finite index sublattice of the full charge lattice exists with a superextremal particle at each site. In perturbative string theory we show that this follows from modular invariance.
    [Show full text]
  • (No) Eternal Inflation and Precision Higgs Physics
    (No) Eternal Inflation and Precision Higgs Physics Nima Arkani-Hameda, Sergei Dubovskyb;c, Leonardo Senatoreb, Giovanni Villadorob aSchool of Natural Sciences, Institute for Advanced Study, Olden Lane, Princeton, NJ 08540, USA b Jefferson Physical Laboratory, Harvard University, Cambridge, MA 02138, USA c Institute for Nuclear Research of the Russian Academy of Sciences, 60th October Anniversary Prospect, 7a, 117312 Moscow, Russia Abstract Even if nothing but a light Higgs is observed at the LHC, suggesting that the Standard Model is unmodified up to scales far above the weak scale, Higgs physics can yield surprises of fundamental significance for cosmology. As has long been known, the Standard Model vacuum may be metastable for low enough Higgs mass, but a specific value of the decay rate holds special significance: for a very narrow window of parameters, our Universe has not yet decayed but the current inflationary period can not be future eternal. Determining whether we are in this window requires exquisite but achievable experimental precision, with a measurement of the Higgs mass to 0.1 GeV at the LHC, the top mass to 60 MeV at a linear collider, as well as an improved determination of αs by an order of magnitude on the lattice. If the parameters are observed to lie in this special range, particle physics will establish arXiv:0801.2399v2 [hep-ph] 2 Apr 2008 that the future of our Universe is a global big crunch, without harboring pockets of eternal inflation, strongly suggesting that eternal inflation is censored by the fundamental theory. This conclusion could be drawn even more sharply if metastability with the appropriate decay rate is found in the MSSM, where the physics governing the instability can be directly probed at the TeV scale.
    [Show full text]
  • UNIVERSITÀ DEGLI STUDI DI PADOVA Dipartimento Di Fisica E Astronomia “Galileo Galilei”
    UNIVERSITÀ DEGLI STUDI DI PADOVA Dipartimento di Fisica e Astronomia “Galileo Galilei” Corso di Laurea Magistrale in Fisica Tesi di Laurea Non perturbative instabilities of Anti-de Sitter solutions to M-theory Relatore Laureanda Dr. Davide Cassani Ginevra Buratti Anno Accademico 2017/2018 Contents 1 Introduction 1 2 Motivation 7 2.1 The landscape and the swampland . .8 2.2 The Weak Gravity Conjecture . .8 2.3 Sharpening the conjecture . 11 3 False vacuum decay 15 3.1 Instantons and bounces in quantum mechanics . 16 3.2 The field theory approach . 24 3.3 Including gravity . 29 3.4 Witten’s bubble of nothing . 33 4 M-theory bubbles of nothing 37 4.1 Eleven dimensional supergravity . 38 4.2 Anti-de Sitter geometry . 41 4.3 Young’s no-go argument . 47 4.4 Re-orienting the flux . 53 4.5 M2-brane instantons . 59 5 A tri-Sasakian bubble geometry? 65 6 Conclusions 77 A Brane solutions in supergravity 79 B Anti-de Sitter from near-horizon limits 83 iii iv CONTENTS Chapter 1 Introduction There are several reasons why studying the stability properties of non supersymmetric Anti- de Sitter (AdS) spaces deserves special interest. First, AdS geometries naturally emerge in the context of string theory compactifications, here including M-theory. General stability arguments can be drawn in the presence of supersymmetry, but the question is non trivial and still open for the non supersymmetric case. However, it has been recently conjectured by Ooguri and Vafa [1] that all non supersymmetric AdS vacua supported by fluxes are actually unstable.
    [Show full text]
  • Swampland, Trans-Planckian Censorship and Fine-Tuning
    Swampland, Trans-Planckian Censorship and Fine-Tuning Problem for Inflation: Tunnelling Wavefunction to the Rescue Suddhasattwa Brahma1∗, Robert Brandenberger1† and Dong-han Yeom2,3‡ 1 Department of Physics, McGill University, Montr´eal, QC H3A 2T8, Canada 2 Department of Physics Education, Pusan National University, Busan 46241, Republic of Korea 3 Research Center for Dielectric and Advanced Matter Physics, Pusan National University, Busan 46241, Republic of Korea Abstract The trans-Planckian censorship conjecture implies that single-field models of inflation require an extreme fine-tuning of the initial conditions due to the very low-scale of inflation. In this work, we show how a quantum cosmological proposal – namely the tunneling wavefunction – naturally provides the necessary initial conditions without requiring such fine-tunings. More generally, we show how the tunneling wavefunction can provide suitable initial conditions for hilltop inflation models, the latter being typically preferred by the swampland constraints. 1 TCC Bounds on Inflation The trans-Planckian censorship conjecture (TCC), proposed recently [1], aims to resolve an old problem for inflationary cosmology. The idea that observable classical inhomogeneities are sourced by vacuum quantum fluctuations [2, 3] lies at the heart of the remarkable arXiv:2002.02941v2 [hep-th] 20 Feb 2020 success of inflationary predictions. On the other hand, if inflation lasted for a long time, then one can sufficiently blue-shift such macroscopic perturbations such that they end up as quantum fluctuations on trans-Planckian scales [4]. This would necessarily require the validity of inflation, as an effective field theory (EFT) on curved spacetimes, beyond the Planck scale. This is what the TCC aims to prevent by banishing any trans-Planckian mode from ever crossing the Hubble horizon and, thereby, setting an upper limit on the duration of inflation.
    [Show full text]
  • Matthew Reece Harvard University
    Exploring the Weak Gravity Conjecture Matthew Reece Harvard University Based on 1506.03447, 1509.06374, 1605.05311, 1606.08437 with Ben Heidenreich and Tom Rudelius. & 161n.nnnnn with Grant Remmen, Thomas Roxlo, and Tom Rudelius Ooguri, Vafa 2005 Concretely: How good can approximate symmetries be? Can an approx. global symmetry be “too good to be true” and put a theory in the swampland? Approximate Symmetries For large-field, natural inflation we might like to have a good approximate shift symmetry φ φ + f, f > M ! Pl In effective field theory, nothing is wrong with this. In quantum gravity, it is dangerous. Quantum gravity theories have no continuous global symmetries. Basic reason: throw charged stuff into a black hole. No hair, so it continues to evaporate down to the smallest sizes we trust GR for. True of arbitrarily large charge ⇒ violate entropy bounds. (see Banks, Seiberg 1011.5120 and references therein) The Power of Shift Symmetries Scalar fields with good approximate shift symmetries can play a role in: • driving expansion of the universe (now or in the past) • solving the strong CP problem • making up the dark matter • breaking supersymmetry • solving cosmological gravitino problems These are serious, real-world phenomenological questions! Example: QCD Axion Weinberg/Wilczek/…. taught us to promote theta to field: a ↵s µ⌫ Gµ⌫ G˜ instantons: shift-symmetric potential fa 8⇡ di Cortona et al. 1511.02867 Important point: large field range, small spurion 2 2 2 2 2 1 m f (md/mu) 1 m f (md/mu)((md/mu) (md/mu) + 1) 2 ⇡ ⇡ λ = ⇡ ⇡ − ma = 2 2 4 4 f (1 + (md/mu)) −f (1 + md/mu) Example: QCD Axion 9 • Stellar cooling constraints: fa >~ 10 GeV • This means the quartic coupling <~ 10-41.
    [Show full text]
  • A Brief Introduction to the Weak Gravity Conjecture Eran Palti Department of Physics, Ben-Gurion University of the Negev, Beer-Sheva 84105, Israel
    Letters in High Energy Physics LHEP-176, 2020 A Brief Introduction to the Weak Gravity Conjecture Eran Palti Department of Physics, Ben-Gurion University of the Negev, Beer-Sheva 84105, Israel Abstract The Weak Gravity Conjecture proposes that a theory with a gauge field that is coupled to gravity must have charged matter on which gravity acts as the weakest force. It also proposes that there is an intrinsic cutoff on such an effective theory, which corresponds to a tower of charged states, that is set by the strength of the gauge coupling (in Planck units). This article is a brief introduction to the Weak Gravity Conjecture, covering aspects of the motivations for it as well as various extensions and refinements. Keywords: Swampland, Quantum Gravity, String Theory gauge fields for simplicity), with gauge coupling g, there must DOI: 10.31526/LHEP.2020.176 exist at least one particle with quantized charge q and mass m which satisfies the bound p 1. INTRODUCTION m ≤ 2gqMp . (4) There are four known forces in the universe: the strong and The bound (4) is termed the Electric WGC. This is to dif- weak forces, electromagnetism, and gravity. The known fun- ferentiate it from a related bound termed the Magnetic WGC. damental matter particles are all charged under at least two The simplest way to introduce this second bound is through the of these forces. For example, the right-handed electron carries electromagnetic dual of (4) [1]. Under electromagnetic duality electromagnetic charge and gravitational charge. These charges the gauge coupling g is exchanged for its inverse g−1, while the can be deduced from the Coulomb forces that two electrons feel electrically charged particle is exchanged for a monopole with when placed a distance r apart.
    [Show full text]
  • Swampland Constraints on 5D N = 1 Supergravity Arxiv:2004.14401V2
    Prepared for submission to JHEP Swampland Constraints on 5d N = 1 Supergravity Sheldon Katz, a Hee-Cheol Kim, b;c Houri-Christina Tarazi, d Cumrun Vafa d aDepartment of Mathematics, MC-382, University of Illinois at Urbana-Champaign, Ur- bana, IL 61801, USA bDepartment of Physics, POSTECH, Pohang 790-784, Korea cAsia Pacific Center for Theoretical Physics, Postech, Pohang 37673, Korea dDepartment of Physics, Harvard University, Cambridge, MA 02138, USA Abstract: We propose Swampland constraints on consistent 5-dimensional N = 1 supergravity theories. We focus on a special class of BPS magnetic monopole strings which arise in gravitational theories. The central charges and the levels of current algebras of 2d CFTs on these strings can be calculated by anomaly inflow mechanism and used to provide constraints on the low-energy particle spectrum and the effective action of the 5d supergravity based on unitarity of the worldsheet CFT. In M-theory, where these theories are realized by compactification on Calabi-Yau 3-folds, the spe- cial monopole strings arise from wrapped M5-branes on special (\semi-ample") 4- cycles in the threefold. We identify various necessary geometric conditions for such cycles to lead to requisite BPS strings and translate these into constraints on the low-energy theories of gravity. These and other geometric conditions, some of which can be related to unitarity constraints on the monopole worldsheet, are additional arXiv:2004.14401v2 [hep-th] 13 Jul 2020 candidates for Swampland constraints on 5-dimensional N = 1 supergravity
    [Show full text]
  • Antipodal Correlation on the Meron Wormhole and a Bang-Crunch Universe
    PHYSICAL REVIEW D 97, 126006 (2018) Antipodal correlation on the meron wormhole and a bang-crunch universe Panagiotis Betzios* Crete Center for Theoretical Physics, Institute for Theoretical and Computational Physics, Department of Physics, University of Crete, 71003 Heraklion, Greece † Nava Gaddam Institute for Theoretical Physics and Center for Extreme Matter and Emergent Phenomena, Utrecht University, 3508 TD Utrecht, Netherlands ‡ Olga Papadoulaki Mathematical Sciences and STAG Research Centre, University of Southampton, Highfield, Southampton SO17 1BJ, United Kingdom (Received 13 January 2018; published 11 June 2018) We present a covariant Euclidean wormhole solution to Einstein Yang-Mills system and study scalar perturbations analytically. The fluctuation operator has a positive definite spectrum. We compute the Euclidean Green’s function, which displays maximal antipodal correlation on the smallest three sphere at the center of the throat. Upon analytic continuation, it corresponds to the Feynman propagator on a compact bang-crunch universe. We present the connection matrix that relates past and future modes. We thoroughly discuss the physical implications of the antipodal map in both the Euclidean and Lorentzian geometries and give arguments on how to assign a physical probability to such solutions. DOI: 10.1103/PhysRevD.97.126006 I. INTRODUCTION whose few proposed resolutions suffer from closed time- like curves and other intricacies [10]. Euclidean wormholes [1–3] are extrema of the Euclidean Inspired by these questions, we
    [Show full text]
  • The String Landscape, the Swampland and The
    The String Landscape The Swampland And Our Universe Cumrun Vafa Harvard University Feb. 28, 2020 KITP, Santa Barbara https://www.cumrunvafa.orG Quantum Field Theories—without gravity included— are well understood. They beautifully describe the interaction of all the elementary particles we know. To include gravity, `Couple the QFT to Gravity’ we need to consider fluctuating metric for spacetime instead of fixed Minkowski space. However, when one tries to add gravity into the mix (in the form of gravitons) the formalism breaks down. The computation of physical processes leads to incurable infinities! This naively suggests: Quantum Field Theories cannot be coupled to gravity! This cannot be true! After all we live in a universe with both gravity and with quantum fields! Resolution? String Theory: A consistent framework which unifies quantum theory and Einstein's theory of gravity—a highly non-trivial accomplishment! Leads to consistent coupling of QFT’s to gravity. Joining and splitting of strings leads to interaction between strings Resolves the inconsistency between quantum theory and gravity Extra Dimensions One of the novel features of string theory is the prediction that there are extra dimensions, beyond 3 spatial dimensions and 1 time. These must be tiny to avoid experimental detection to date. Extra dimensions of string theory can have a large number of distinct possibilities The physical properties observed in 3+1 dimensions depends on the choice of the compact tiny space: Number of forces, particles and their masses, etc. Since there are a vast number of allowed tiny spaces which are allowed we get a huge number of consistent possible effective 3+1 dimensional theories; The String Landscape Each choice of compactification space leads to a distinct observable physics in 4 dimensions.
    [Show full text]
  • Pdf/10.1002/Andp.19053221004]
    This electronic thesis or dissertation has been downloaded from the King’s Research Portal at https://kclpure.kcl.ac.uk/portal/ Numerical general relativity and beyond formation of relativistic axion stars, boosting and colliding oscillotons, and gravitational collapse in khronometric theory Widdicombe, James Awarding institution: King's College London The copyright of this thesis rests with the author and no quotation from it or information derived from it may be published without proper acknowledgement. END USER LICENCE AGREEMENT Unless another licence is stated on the immediately following page this work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International licence. https://creativecommons.org/licenses/by-nc-nd/4.0/ You are free to copy, distribute and transmit the work Under the following conditions: Attribution: You must attribute the work in the manner specified by the author (but not in any way that suggests that they endorse you or your use of the work). Non Commercial: You may not use this work for commercial purposes. No Derivative Works - You may not alter, transform, or build upon this work. Any of these conditions can be waived if you receive permission from the author. Your fair dealings and other rights are in no way affected by the above. Take down policy If you believe that this document breaches copyright please contact [email protected] providing details, and we will remove access to the work immediately and investigate your claim. Download date: 24. Apr. 2021 Numerical General Relativity and Beyond Formation of Relativistic Axion Stars, Boosting and Colliding Oscillotons, and Gravitational Collapse in Khronometric Theory James Young Widdicombe Supervisor: Dr Eugene Lim Department of Physics King's College London A thesis presented for the degree of Doctor of Philosophy September 2019 Declaration I declare that this thesis has been composed solely by myself and that it has not been submitted, in whole or in part, in any previous application for a degree.
    [Show full text]