'Gauge symmetry' presentation slideshows

Representations and particles of osp (1|2n) generalized conformal supersymmetry

Representations and particles of osp (1|2n) generalized conformal supersymmetry. Igor Salom Institute of physics, University of Belgrade. Motivation/Outline. Hundreds of papers on osp generalization of conformal supersymmetry in last 30 years, yet group-theoretical approach is missing

929 views • 73 slides

Making the most and the best of Unparticle

Making the most and the best of Unparticle. to gain as much advantage and enjoyment as you can from sth. to a ccept a difficult situation and do as well as you can. A survey of scale invariance and conformal group. Banks-Zaks fields as an example of non-trivial IR fixed point.

665 views • 52 slides

Asymmetric Orbifold toward Heterotic Anomalous U(1) GUT

Asymmetric Orbifold toward Heterotic Anomalous U(1) GUT. Toshifumi Yamashita (Nagoya University). 09 Nov. 2009 @KEK mini workshop. working with Nagoya U. : Maekawa, Moriyama, Teraguchi Takei, Ito, Kuwakino NCTU (Taiwan) : Keijiro Takahashi.

586 views • 45 slides

Review of gauge-Higgs unification models

Review of gauge-Higgs unification models. TIS2005, Taiwan, 6/10/2005. Naoyuki Haba ( ???? ). (Tokushima Univ.). Plan of talk. 1. models of gauge-Higgs unification. 2. electro-weak symmetry breaking ???. 3. electro-weak symmetry breaking ???. 4. Higgs phenomenology.

569 views • 45 slides

SUSY and Superstrings

SUSY and Superstrings. Masahiro Yamaguchi Tohoku University Asian School Particles, Strings and Cosmology (NasuLec) September 25-28, 2006@Nasu, Japan. Phenomenology of SUSY and Superstrings. Masahiro Yamaguchi Tohoku University Asian School Particles, Strings and Cosmology (NasuLec)

562 views • 44 slides

New Views of the Universe

580 views • 42 slides

New Frontiers in Particle Physics

New Frontiers in Particle Physics. Jeff Forshaw University of Manchester. What we know. There are a few elementary particles that interact with each other. The interactions come in four types: Gravity Electromagnetism Weak Strong. Standard Model. e. W. e. d. u.

494 views • 34 slides

Heavy quarkonia in AdS /QCD

Heavy quarkonia in AdS /QCD. Y. Kim (KIAS) YK, J.-P. Lee, S. H. Lee, Phys. Rev. D75:114008, 2007. YK, B.-H. Lee, C. Park, and S.-J. Sin, hep - th /08081143 . Plan. Why heavy quarkonia ? Bottom-up AdS /QCD Heavy quarkonium in bottom-up Holographic heavy quark potential Summary.

440 views • 32 slides

Introduction to Gauge Higgs unification with a graded Lie algebra

Introduction to Gauge Higgs unification with a graded Lie algebra. 2011. 10. 7 @ Academia Sinica , Taiwan Jubin Park (NTHU). Collaboration with Prof. We-Fu Chang. Based on D. B. Fairlie PLB 82,1.

431 views • 30 slides

String theoretic QCD axions in the light of PLANCK and BICEP2

String theoretic QCD axions in the light of PLANCK and BICEP2 (QCD axion after BICEP2) Kiwoon Choi @ KIAS, May 1, 2014 KC, K.S. Jeong and M.S. Seo , arXiv:1404.3880 The IBS Center for Theoretical Physics of the Universe . Outline

371 views • 29 slides

The minimal B-L model naturally realized at TeV scale

The minimal B-L model naturally realized at TeV scale. Yuta Orikasa (SOKENDAI) Satoshi Iso (KEK,SOKENDAI) Nobuchika Okada(University of Alabama) Phys.Lett.B676(2009)81 Phys.Rev.D80(2009)115007.

410 views • 25 slides

Inflation from radion gauge-Higgs potential at Planck scale

Inflation from radion gauge-Higgs potential at Planck scale. Yugo Abe ( Shinshu University ) GRaB100@NTU, July 10, 2015 In collaboration with T. Inami (NTU), Y. Kawamura ( Shinshu U), Y. Koyama (NCTS). YA , T. Inami , Y. Kawamura, & Y. Koyama , [ arXiv: 1504.06905]. 0. Our focus.

290 views • 24 slides

Meta-stable Supersymmetry Breaking in Spontaneously Broken N=2 SQCD

403 views • 23 slides

Electroweak Summary

Electroweak Summary. Chris Hays, Oxford University for the EWK/BSM session conveners: Michael Kramer Dave South Filip Zarnecki XVI th Workshop on Deep Inelastic Scattering London, England April 10, 2008. Electroweak and Beyond-the-Standard-Model Session. 42 talks

614 views • 22 slides

D-term Dynamical Supersymmetry Breaking

D-term Dynamical Supersymmetry Breaking. with N. Maru (Keio U.) arXiv:1109.2276 one in preparation. K. Fujiwara and, H.I. and M. Sakaguchi arXiv : hep-th /0409060, P. T. P. 113 arXiv : hep-th /0503113, N. P. B 723 H. I., K. Maruyoshi and S. Minato

378 views • 22 slides

Electroweak Summary

Electroweak Summary. Chris Hays, Oxford University for the EWK/BSM session conveners: Michael Kramer Dave South Filip Zarnecki XVI th Workshop on Deep Inelastic Scattering London, England April 10, 2008. Electroweak and Beyond-the-Standard-Model Session. 42 talks

316 views • 22 slides

New Gauge Symmetries from String Theory

New Gauge Symmetries from String Theory. Pei-Ming Ho Physics Department National Taiwan University Sep. 23, 2011@CQSE. Gauge vs Global. For covariant quantities Old definitions in some textbooks: U = independent of spacetime ? global U = function of spacetime ? gauge (local).

341 views • 21 slides

New Gauge Symmetries from String Theory

New Gauge Symmetries from String Theory. Pei-Ming Ho Physics Department National Taiwan University Sep. 23, 2011@CQSE. Gauge vs Global. For covariant quantities Old definitions in some textbooks: U = independent of spacetime ? global U = function of spacetime ? gauge (local).

341 views • 21 slides

A Realization of Effective SUSY

A Realization of Effective SUSY. Zhen- hua Zhao ITP,CAS Liu & Zhao arXiv:1312.7389. Contents. Motivation The Model Phenomenological Consequence Summary. Higgs with 125 GeV mass. SM is completed and self-consistent. Gauge Hierarchy Problem.

269 views • 19 slides

Methods of Experimental Particle Physics

Methods of Experimental Particle Physics. Alexei Safonov Lecture #1. Syllabus etc. Structure of the class: 2 lectures per week (50 mins each) 2 labs per week (1hr long each)

262 views • 12 slides