SUSY Breaking in Local String Models J.P. Conlon, A. Maharana, FQ arXiv:0810.5660 [hep-th] ] R. Blumenhagen, J.P. Conlon, S. Krippendorf, S.Moster, FQ.

Slides:



Advertisements
Similar presentations
אוניברסיטת בן - גוריון Ram Brustein Stabilizing moduli in the outer region: IIB and Heterotic flux compactifications Cosmological stability: A parachute.
Advertisements

Renata Kallosh Davis, May 16, 2004 Stanford Stanford Deformation, non-commutativity and cosmological constant problem.
 Symmetries and vanishing couplings in string-derived low-energy effective field theory              Tatsuo Kobayashi 1.Introduction.
Phenomenological aspects of magnetized brane models Tatsuo Kobayashi
Brane-World Inflation
Inflation and String Cosmology Andrei Linde Andrei Linde.
Non-perturbative effects in string theory compactifications Sergey Alexandrov Laboratoire Charles Coulomb Université Montpellier 2 in collaboration with.
A Realization of Effective SUSY Zhen-hua Zhao ITP,CAS Liu & Zhao arXiv:
Problems with the MSSM : mu & proton decay Stuart Raby KMI Nagoya University October 24, 2011.
Effective Theory of Cosmological SUSY Breaking Principles of CSB: 1.C.C. Discrete Input Controlling No. Physical States in de Sitter Space-Time 2. SUSY.
Flux Compactifications: An Overview Sandip Trivedi Tata Institute of Fundamental Research, Mumbai, India Korea June 2008.
אוניברסיטת בן - גוריון Ram Brustein  Moduli space of effective theories of strings  Outer region of moduli space: problems!  “central” region:  stabilization.
BRANE SOLUTIONS AND RG FLOW UNIVERSIDADE FEDERAL DE CAMPINA GRANDE September 2006 FRANCISCO A. BRITO.
Moduli stabilization and flavor structure in 5D SUGRA with multi moduli Yutaka Sakamura (RIKEN) in collaboration with Hiroyuki Abe (Yukawa Inst.) June.
New Cosmological Implications for LARGE Volume Scenarios Michele Cicoli DAMTP, University of Cambridge StringPheno09, Warsaw, 16 June 2009 Based on: MC,
6 August, 2007 at SI2007. Phys.Rev.D75:025019,2007, ArXiv: [hep-th]. Based on articles : In collaboration with Hiroyuki Abe (YITP), Tatsuo Kobayashi.
The LARGE Volume Scenario: Realisation and Cosmological Implications M. Cicoli, J. Conlon, FQ, [hep-th] + to appear J. Conlon, R. Kallosh, A.
Random Matrix Theory Workshop NBIA May 2007 Large N double scaling limits in Gauge Theories and Matrix Models Gaetano Bertoldi Swansea University.
Title of talk1 String Model Building Stuart Raby String Pheno 09 Warsaw University June 19, 2009 Savoy Hotel M ü nchen I Amalienstra ß e 25 I M ü.
Moduli Stabilization: A Revolution in String Phenomenology / Cosmology ? F. Quevedo SUSY 2005.
Road to the MSSM thru M theory ? Stuart Raby University of Michigan Ann Arbor May 5, 2007.
Physical Constraints on Gauss-Bonnet Dark Energy Cosmologies Ishwaree Neupane University of Canterbury, NZ University of Canterbury, NZ DARK 2007, Sydney.
Title of talk1 A Fertile Patch in the Heterotic Landscape Stuart Raby Rutgers University March 24, 2009.
SHIFT SYMMETRY and INFLATION in SUPERGRAVITY Ph. Brax and J. Martin hep/th to appear in PRD.
Large Volume String Compactifications hep-th/ , , , , hep-ph/ and to appear F. Quevedo, Cambridge. UKBSM Liverpool 2007.
Inflation, String Theory, Andrei Linde Andrei Linde and Origins of Symmetry.
John ELLIS, King’s College London Planck-Compatible Inflationary Models.
אוניברסיטת בן - גוריון Ram Brustein  Outer region of moduli space: problems!  Central region: parametrization with N=1 SUGRA  Scales & shape of central.
Gravity and Extra Dimensions José Santiago Theory Group (Fermilab) APS April meeting, Session Y4 (Gravity and Cosmology) Jacksonville (FL) April 14-17,
Andreas Ringwald (DESY) PASCOS 2012, Merida, Mexico, 3-8 June 2012 Searching for axions and ALPs from string theory.
String theoretic QCD axions in the light of PLANCK and BICEP2 Kiwoon CosKASI Conference, April 16, 2014 KC, K.S. Jeong and M.S. Seo, arXiv:
Extra Dimensional Models with Magnetic Fluxes Tatsuo Kobayashi 1. Introduction 2. Magnetized extra dimensions 3. N-point couplings and flavor symmetries.
Cosmology in LARGE volume string models Tetsutaro Higaki arXiv: published in JHEP 1211 (2012) 125 with Fuminobu Takahashi at Tohoku U. See also.
1 EXTRA DIMENSIONS AT FUTURE HADRON COLLIDERS G.F. Giudice CERN.
Cosmological Moduli Problem and Double Thermal Inflation Cosmological Moduli Problem and Double Thermal Inflation in Large Volume Scenario in Large Volume.
Cosmology and String Theory F. Quevedo Cambridge CORFU 2005.
Stabilizing moduli with flux in brane gas cosmology Jin Young Kim (Kunsan National Univ.) CosPA 2009, Melbourne Based on arXiv: [hep-th]; PRD 78,
Axion and anomalous U(1) gauge symmetry Axion and anomalous U(1) gauge symmetry in string theory in string theory Kiwoon Choi (KAIST) ASK 2011 Apr.11 –
Fibre Inflation High-Fibre models from regular potentials String Pheno Workshop: CERN 2008 C.P. Burgess with M. Cicoli and F.Quevedo.
Unification Hints The Standard Model: Partial Unification.
Mirage Mediation of SUSY Breaking K. S. Jeong KIAS 25 May, 2007 Based on hep-ph/ , hep-ph/
Anomalous U(1)΄s, Chern-Simons couplings and the Standard Model Pascal Anastasopoulos (INFN, Roma “Tor Vergata”) Pascal Anastasopoulos (INFN, Roma “Tor.
Title of talk1 Unification & B-L in String Theory Stuart Raby B-L Workshop, LBL September 21, 2007.
Introduction to Strings Yoshihisa Kitazawa KEK Nasu lecture 9/25/06.
Title of talk1 A Fertile Patch in the Heterotic Landscape Stuart Raby String Phenomenology CERN August 11, 2008.
The LARGE Volume String Scenarios F. Quevedo, Cambridge/ICTP. Havana, Cuba J. Conlon, V. Balasubramanian, P. Berglund, FQ +….since 2005 M. Dolan,
Moduli stabilization, SUSY breaking and the Higgs sector Tatsuo Kobayashi 1. Introduction 2. KKLT scenario 3 . Generalized KKLT scenario 4. TeV scale mirage.
Is the four-dimensional effective theory effective? YITP Hideo Kodama HK and Kunihito Uzawa, JHEP0507:061(2005) HK and Kunihito Uzawa, hep-th/
At the IFT workshop 28/Sep., Challenges for String Theory at the LHC era 2.Constraints on GUT 7-brane Topology in F- theory 3.Challenges for String.
Moduli stabilization, SUSY breaking and the Higgs sector Tatsuo Kobayashi 1. Introduction 2. KKLT scenario 3 . Generalized KKLT scenario 4. TeV scale mirage.
Mar. 29, 2008 LHC 研究会 Axionic Mirage Mediation Tohoku Univ. Shuntaro Nakamura Collaborated with K. Okumura and M. Yamaguchi This talk is based on arXiv:
Mirage Mediation of Supersymmetry Breaking: Phenomenology and Cosmology Masahiro Yamaguchi (Tohoku University) Sep. 25, Beijing.
Happy Golden Age Peter!!!. Phenomenological Aspects of D-branes at Singularities F. Quevedo, Cambridge/ICTP. Planck 2011/PeterFest, Lisbon S. Krippendorf,
Recent Developments in LARGE Volume String Scenario F. Quevedo, Cambridge/ICTP. Planck 2010, CERN, May-June R. Blumenhagen, J. Conlon, S. Krippendorf,
P-Term Cosmology A.C. Davis (with C. Burrage) ,
Perturbative vs Non- Perturbative Effects for Moduli Stabilisation and Cosmology J. Conlon, FQ [hep-ph] M. Cicoli, J. Conlon, FQ, [hep-th]
Three family GUT-like models from heterotic string
STRING THEORY AND M-THEORY: A Modern Introduction
Moduli phenomenology and cosmology Tatsuo Kobayashi
Kaluza-Klein non-compactification to dS
Magnetic supersymmetry breaking
Kähler Moduli Inflation
Late-time Cosmology with String Gases
dark matter Properties stable non-relativistic non-baryonic
Inflationary multiverse and string theory
The Cosmological Constant Problem & Self-tuning Mechanism
Holographic Heavy- Light mesons from non- Abelian DBI
grand gauge-Higgs unification
Constraints on Quantum Gravity
Presentation transcript:

SUSY Breaking in Local String Models J.P. Conlon, A. Maharana, FQ arXiv: [hep-th] ] R. Blumenhagen, J.P. Conlon, S. Krippendorf, S.Moster, FQ arXiv:0906.xxxx [hep-th] See also S. de Alwis talk here F. Quevedo, Cambridge/CERN. String Phenomenology, Warsaw, June 2009.

Phenomenology String Theory String Phenomenology

String Model Building:  Global Models (e.g. Heterotic)  Local Brane Models (e.g. IIB)

Bottom-up Approach Gauge group Chiral spectrum Yukawa couplings Gauge couplings Proton stability Flavour symmetries Moduli Stabilisation Cosmological constant SUSY Breaking Scales (unification, axions,…) Inflation, Reheating Cosmological moduli problem Global (bulk) Issues Local (brane) Issues Aldazabal,Ibanez, FQ, Uranga 2000

GLOBAL ISSUES

LARGE Volume Scenario

MODULI STABILISATION 4-cycle size: τ (Kahler moduli) 3-cycle size: U (Complex structure moduli) + String Dilaton: S

Exponentially Large Volumes Perturbative (alpha’) corrections to K Example : BBCQ, CQS (2005) Exponentially large volume, broken SUSY, AdS Fluxes

De Sitter?: anti D3 or D,F uplifing (Or W~ W 0 + φ 1 φ 2 e -aT2 ) LARGE volume de Sitter! S. Krippendorf, FQ 2009 Model dependent e.g.:

General Conditions for LARGE Volume h 12 > h 11 > 1 At least one blow-up mode (point-like singularity) Blow-up mode fixed by non- perturbative effects, volume by alpha’ corrections Cicoli, Conlon, FQ

e.g. Swiss Cheese Calabi-Yau’s e.g. Blumenhagen, et al., Grimm et al., Kreuzer et al. 08

Relevant Scales String scale Ms=M P /V 1/2 Kaluza-Klein scale M KK =M P /V 2/3 Gravitino mass m 3/2 =W 0 M P /V

Moduli Masses Dilaton + Complex structure M~m 3/2 =W 0 M P /V ‘Small’ Kahler moduli M~(lnV)m 3/2 Volume modulus M~W 0 M P /V 3/2 << m 3/2

Original Scenarios M String = M GUT ~ GeV (V~ ) W 0 ~ <<1 (or W 0 ~1 plus warping) Fits with coupling unification Natural scale of most (all?) string inflation models. Axi-volume quintessence scale (w=-0.999….) Cosmological moduli problem! M String = M int. ~ GeV (V~10 14 ) W 0 ~1 (no hierarchy problem) m 3/2 ~1 TeV QCD axion scale Neutrino masses LLHH Cosmological moduli problem, unification? M String = 1 TeV (V~10 30 ) W 0 ~1 Most exciting, but 5th Force (volume modulus m~ eV)??

LOCAL ISSUES

LARGE Volume Implies Standard Model is localised ! ( SM D7 cannot wrap the exponentially large cycle since g 2 =1/V 2/3 )  Fractional D3/D7 Brane at a singularity (collapsed cycle)  Magnetised D7 - Brane wrapping a ‘small’ four-cycle  Local F-Theory Blumenhagen talk Heckman, Tatar, … talks

Universe D3 Brane or or D7 Brane

e.g. Standard Model at (Fractional) D3/D7 Branes at Singularities Collapsing single 4-cycle: del Pezzo surfaces dP n, n=0,1, …,8 (P 2 blown-up at n arbitrary points c 1 >0, b 2 =n+1, 2n-8 parameters, n>3) More general singularities, e.g. Y pq, L abc

e.g. Realistic dP 1 Models Standard Model LR Symmetric Model Hierarchy in 3 generation masses! Also: Pati-Salam, etc.

GLOBAL/LOCAL MIXING

Local/Global Mixing Standard Model in small cycle SM cycle NOT fixed by non-perturbative effects: SM chiral implies: W np = MSSM: =0, so W np =0, (singularity)? Or = Blumenhagen et al.2007

Effective Field Theory I Geometric Regime

Effective Field Theory II Around the Singularity (Blow-up Regime)

SUSY BREAKING

SM Cycle does not break SUSY! ‘Fayet-Iliopoulos’  0 ‘Sequestered moduli/gravity mediated SUSY Breaking’ No-scale (vanishing soft terms)Suppressed !

Gravity/Moduli Mediated Soft-terms Soft terms <<< M 3/2 !!!

Local Yukawas and SUSY Breaking () All soft terms of order (loop factor)/V 3/2 or 1/V 2 (e.g. anomaly mediation and/or Dilaton F-term) Independent of SUSY breaking fields

New Scenarios Scalars 1/V 3/2, others 1/V 2 All a/V 3/2 All 1/V 2 Loop corrections ~ b/V 5/3 M string ~ GeV Gauge mediation? (F X /x>m<<M 3/2 ?) but with heavy gravitino!

General Properties Uplifting to de Sitter important Gravitino very heavy M 3/2 >10 8 GeV !! Generically no CMP!!!! (M volume >M soft ) Minimal volume V~ TeV soft terms and M string ~10 15 GeV Unification scale M X ~ M string V 1/6 ~10 16 GeV ! Right scale for inflation! No CMP !!! Conlon’s talk De Alwis 2006

Conclusions Continuous progress in this `Decade of Applied String Theory’ Bottom-up (Local Model Building) fits with Large Volume Realistic models at singularities: powerful quiver/dimer constructions New SUSY breaking scenarios with TeV soft terms and GUT scale unification Alleviate tension between low energy SUSY and cosmology Generically no CMP!!! Open challenges (compact CY, detailed susy breaking, EFT in F-theory models,…)