Unification Hints The Standard Model: Partial Unification.

Slides:



Advertisements
Similar presentations
Physics at the TeV Scale Particles and forces The known particle spectrum The need for TeV energies The origin of mass The path to Grand Unification Supersymmetry.
Advertisements

Kiwoon Choi PQ-invariant multi-singlet NMSSM
Extra Dimensions of Space-Time String theory suffers conformal anomaly that makes theory inconsistent --> get rid of it Conformal anomaly ~ (D-26) for.
Non-perturbative effects in string theory compactifications Sergey Alexandrov Laboratoire Charles Coulomb Université Montpellier 2 in collaboration with.
Outlook: Higgs, SUSY, flavor Ken-ichi Hikasa (Tohoku U.) Fourth Workshop, Origin of Mass and SUSY March 8, 2006, Epochal Tsukuba.
STRING THEORY: CHALLENGES AND PROSPECTS John H. Schwarz October 2008.
Higgs Boson Mass In Gauge-Mediated Supersymmetry Breaking Abdelhamid Albaid In collaboration with Prof. K. S. Babu Spring 2012 Physics Seminar Wichita.
Anomaly cancellations on heterotic 5-branes ( 前編 ) 矢田 雅哉.
Physics Beyond the Standard Model
Discovering Gluinos at Hadron Colliders SLAC Theory Group Jay Wacker December 5, 2008 In collaboration with: M. Lisanti, J. Alwall, M. Le.
Road to the MSSM thru M theory ? Stuart Raby University of Michigan Ann Arbor May 5, 2007.
Richard Howl The Minimal Exceptional Supersymmetric Standard Model University of Southampton UK BSM 2007.
Title of talk1 A Fertile Patch in the Heterotic Landscape Stuart Raby Rutgers University March 24, 2009.
Minimal Supersymmetric Standard Model (MSSM) SM: 28 bosonic d.o.f. & 90 (96) fermionic d.o.f. SUSY: # of fermions = # of bosonsN=1 SUSY: There are no particles.
Fermion Masses and Unification Steve King University of Southampton.
4 th Generation Leptons in Minimal Walking Technicolor Theory Matti Heikinheimo University of Jyväskylä.
Introduction to universal extra dimensions (UEDs) Mitsuru Kakizaki (ICRR, University of Tokyo) May 10, KEK Refs: Original idea: Appelquist, Cheng,
Extra Dimensional Models
Title of talk1 On the Heterotic Road to the MSSM Stuart Raby Eotvos-Cornell 2007 Budapest, Hungary June 29, 2007.
.. Particle Physics at a Crossroads Meenakshi Narain Brown University.
Extra Dimensions with Many Inverse Femptobarns at the Tevatron Universal Extra Dimensions Warped Extra Dimensions – Beyond RS1 - SM in the bulk –Brane.
 Collaboration with Prof. Sin Kyu Kang and Prof. We-Fu Chang arXiv: [hep-ph] submitted to JHEP.
Kaluza-Klein gluon production at the LHC
Fermion Masses and Unification Steve King University of Southampton.
Minimal SO(10)×A4 SUSY GUT ABDELHAMID ALBAID In Collaboration with K. S. BABU Oklahoma State University.
1 Brane world cosmology Lecture from the course “Introduction to Cosmoparticle Physics”
Center for theoretical Physics at BUE
1 EXTRA DIMENSIONS AT FUTURE HADRON COLLIDERS G.F. Giudice CERN.
International Conference on Linear Colliders Paris, April 19-23, 2004 Theoretical Introduction John Ellis.
Low scale gravity mediation in warped extra dimensions and collider phenomenology on sector hidden sector LCWS 06, March 10, Bangalore Nobuchika.
Sreerup Raychaudhuri TIFR Extra Dimensions and Collider Physics Workshop on Synergy between High Energy and High Luminosity Frontiers Tata Institute of.
Wednesday, Apr. 23, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #24 Wednesday, Apr. 23, 2003 Dr. Jae Yu Issues with SM picture Introduction.
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 –
String/M Theory – what is it? Branes and brane world Holography The Landscape Nick Evans Strong Force Origins Superstrings Ten & eleven dimensions.
1 Supersymmetry Yasuhiro Okada (KEK) January 14, 2005, at KEK.
1 THEORETICAL PREDICTIONS FOR COLLIDER SEARCHES “Big” and “little” hierarchy problems Supersymmetry Little Higgs Extra dimensions G.F. Giudice CERN.
Low scale supergravity mediation in brane world scenario and hidden sector phenomenology Phys.Rev.D74:055005,2006 ( arXiv: hep-ph/ ) ACFA07 in Beijing:
Mirage Mediation of SUSY Breaking K. S. Jeong KIAS 25 May, 2007 Based on hep-ph/ , hep-ph/
Perspectives in string theory? L.Bonora SISSA,Trieste, Italy Belgrade, September 2012.
INVASIONS IN PARTICLE PHYSICS Compton Lectures Autumn 2001 Lecture 8 Dec
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.
STANDARD MODEL. Precision Electroweak data?? Higgs coupling blows up!! Higgs potential collapses Higgs coupling less than in Standard Model viXra Blogger’s.
SUSY and Superstrings Masahiro Yamaguchi Tohoku University Asian School Particles, Strings and Cosmology (NasuLec) September 25-28, Japan.
Particle Physics: Status and Perspectives Part 9: Energy Frontier and Open Questions Manfred Jeitler SS 2015.
1 Prospect after discoveries of Higgs/SUSY Yasuhiro Okada (KEK) “Discoveries of Higgs and Supersymmetry to Pioneer Particle Physics in the 21 st Century”
Nobuchika Okada The University of Alabama Miami 2015, Fort Lauderdale, Dec , GeV Higgs Boson mass from 5D gauge-Higgs unification In collaboration.
The Search For Supersymmetry Liam Malone and Matthew French.
Masato Yamanaka (Saitama University) collaborators Shigeki Matsumoto Joe Sato Masato Senami Phys.Rev.D76:043528,2007Phys.Lett.B647: and Universal.
03/31/2006S. M. Lietti - UED Search at SPRACE 1 Universal Extra Dimensions Search at SPRACE S. M. Lietti DOSAR Workshop at U.T. Arlington.
Constructing 5D Orbifold GUTs from Heterotic Strings w/ R.J. Zhang and T. Kobayashi Phys. Lett. B593, 262 (2004) & Nucl. Phys. B704, 3 (2005) w/ A. Wingerter.
DIS2003 A.Tilquin Searches for Physics Beyond the Standard Model at LEP What is the Standard Model Why to go beyond and how Supersymmetry Higgs sector.
Report on model separation Masaki Asano (Tohoku U.) The 12th general meeting of the ILC physics working group.
Searching for in High Mass Dilepton Spectrum at CDF, Fermilab ADD model Drell-Yan production of a graviton of varying string scale M S = M Pl(4+n) [4]
New Strong LHC Rogerio Rosenfeld Instituto de Física Teórica UNESP  
Three family GUT-like models from heterotic string
STRING THEORY AND M-THEORY: A Modern Introduction
Nick Evans University of Southampton
Magnetic supersymmetry breaking
Grand Unified Theories and Higgs Physics
The Standard Model Lecture III
The symmetry of interactions
The MESSM The Minimal Exceptional Supersymmetric Standard Model
Search For New Physics Chary U of S.
Physics at a Linear Collider
Introduction to universal extra dimensions (UEDs)
6D Supergravity and the Cosmological Constant
Introduction to Particle Physics
Kaluza-Klein states and the geography of extra dimensions
Prospect after discoveries of Higgs/SUSY
Presentation transcript:

Unification Hints The Standard Model: Partial Unification

Matter Sector “chiral” Family Symmetry? Neutral Up Down Family Symmetry?

Standard Model parameters Cabibbo, Kobayashi, Maskawa

} } ? ? ? e e Grand Unification

-u c ucuc ud ucuc ud u d ecec } } dcdc dcdc dc e e Grand Unification LH states SU(2) doublets {

-u c ucuc ud ucuc ud u d ecec } } dcdc dcdc dc e e Grand Unification -t c tctc tb tctc tb tb cc bcbc bcbc bcbc   -u c ucuc ud ucuc ud u d ecec ucuc ud ucuc ud u d ecec dcdc dcdc dcdc e e -c cc cs c cs cs cc scsc scsc scsc   Generations (?)

-u c ucuc ud ucuc ud u d ecec dcdc dcdc dc e e Grand Unification } : New lepto-quark gauge interactions } u u dcdc e+e+

Neutrino Mass <H><H> <H><H> Grand Unification +5

-u c ucuc ud ucuc ud u d ecec } } dcdc dcdc dc e e Gauge Couplings +

Precision Measuremets Log 10 [Energy Scale (GeV)]  1 -1  2 -1  3 -1 Either: No Grand Unification or: more particles... Either: No Grand Unification or: more particles...

Supersymmetry threshold Log 10 [Energy Scale (GeV)]  1 -1  2 -1  3 -1 TeV scale supersymmetry

String theory World sheet } String tension OpenClosed

String Structure : 1 st string revolution Ghost free condition : D=10 Fermionic (+SUSY) E8 SO(32) Type I Type IIA Type IIB String excitations : J m2 Compactification D=10 D=4 +(D=6) compactified – radius R Kaluza Klein & winding modes Gauge structure : restricted by anomaly cancellation Green Schwarz +chiral structure for q, l ; multiplet structure determined by topology of manifold : Calabi Yau - 3 generation examples known Supersymmetry (c.f. D=26 Bosonic) †

String Structure : 2nd string revolution E8 SO(32) Type I Type IIA Type IIB D=11 supergravity M String dualities D-branes Submanifold on which open strings start or end

String phenomenology How can we distinguish them?

Supersymmetry threshold Log 10 [Energy Scale (GeV)]  1 -1  2 -1  3 -1 TeV scale supersymmetry

I GGR, D.Ghilencea SUSY gauge coupling unification

I Unification Hints ×  3,2,1 E TeV M Pl anck Gravitational coupling 1/r 2+n 1/r p Gauge coupling ? Unification at a TeV?

Warped Unification RS1 TeV Brane All scales up to Planck scale present - logarithmic running of gauge couplings! Randall, Schwarz Sundrum, Delgardo,... Choi, Kim, Kim × D=5

I Updated fit : E MPMP  3,2,1 G N (Q) Q 2 Unification with gravity? SUSY coupling unification

} } Gauge unification - Heterotic String

String Threshold Effects (WCHS) N=2 KK modesWinding modes Dixon, Kaplunovsky, Louis

Threshold sensitivity To preserve insensitivity to heavy thresholds (no power law sensitivity) need Ghilencea,GGR

Weakly coupled heterotic strings with Wilson line breaking Discrete group Physical states : e.g.

Reduction in X,Y boson contribution - equivalent to reduction in unification scale. } (14)

N=3, n=1N=7, n=1N=7, n=2N=7, n= (4.12)3.68 (4.43)3.71 (3.78))4.81 (6.75) (-0.27)-0.25 (-0.28)-0.25 (-0.25)-0.30 (-0.36) 2.81 (3.10)2.84 (3.29)2.86 (2.90)3.50 (4.61) 0.49 (0.54)0.50 (0.57)0.50 (0.51)0.60 (0.73) Quantitative effect of Wilson lines : No Higgs KK modes Higgs KK modes 2D1D or 2D (matter KK modes degenerate) GGR

String profile from gauge unification WCHS + Wilson line