'Gauge fields' presentation slideshows

What is a fundamental particle??

What is a fundamental particle??. No standard definition. Formal definition : A particle which can not be described in terms of more fundamental particles. Present day fundamental particles may not be fundamental particles of tomorrow. LEPTONS (+ ANTI) QUARKS (+ANTI)

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Summary

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Craig Roberts Physics Division

Continuum strong QCD . Craig Roberts Physics Division. Chiral Q C D. m t = 40,000 m u Why?. Current-quark masses External paramaters in Q C D Generated by the Higgs boson, within the Standard Model Raises more questions than it answers. Chiral Symmetry.

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Aspen Winter 2003 Conference on Particle Physics: At the Frontiers Jan 19-25 2003

Aspen Winter 2003 Conference on Particle Physics: At the Frontiers Jan 19-25 2003. BLACK HOLES & GRAVITONS AT HECs. Maria Spiropulu Enrico Fermi Institute UofC. What ?. A singular classical object (black hole)

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Multiple M5-branes and ABJM Theory

Multiple M5-branes and ABJM Theory. Seiji Terashima (YITP, Kyoto) based on the works ( JHEP 0912 (2009) 059 and arXiv:1012:3961, to appear in JHEP ) with Futoshi Yagi (IHES). 2011 February 18 at NTU. 1. Introduction. Recent exciting progress in string theory:. Low energy actions of

769 views • 58 slides

Roberto Casalbuoni Department of Physics, Sezione INFN,

Higgsless Models. Roberto Casalbuoni Department of Physics, Sezione INFN, G. Galilei Institute for Theoretical Physics (GGI) Florence - Italy. casalbuoni@fi.infn.it. Leuven, February 17, 2010. Outline of the talk.

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Roberto Casalbuoni Dipartimento di Fisica, Sezione INFN, Istituto G. Galilei per la Fisica Teorica

Higgsless Models. Roberto Casalbuoni Dipartimento di Fisica, Sezione INFN, Istituto G. Galilei per la Fisica Teorica Firenze. casalbuoni@fi.infn.it. Padova, 22 Gennaio, 2009. Outline of the talk.

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Summary

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Vladimir Cvetkovi?

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8. Forces, Connections and Gauge Fields

8. Forces, Connections and Gauge Fields. 8.0. Preliminary 8.1. Electromagnetism 8.2. Non-Abelian Gauge Theories 8.3. Non-Abelian Theories and Electromagnetism 8.4. Relevance of Non-Abelian Theories to Physics 8.5. The Theory of Kaluza and Klein. 8.0 Preliminary.

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TU Wien, April 2014

`. M. Isachenkov , I.K., V. Schomerus , arXiv : 1403.6857. Chiral Primaries in Strange Metals Ingo Kirsch DESY Hamburg, Germany. Based on work with V . Schomerus , M . Isachenkov. TU Wien, April 2014. Chiral Primaries in Strange Metals .

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Spontaneous breakdown (SB) of symmetry

Spontaneous breakdown (SB) of symmetry. real scalar j. v.e.v. Z 2 symmetry. SB. mass of x :. field redefinition. +fermion y. chiral symmetry. mass term. :forbidden. mass of y :. fermion mass generation by SB. complex scalar field f. global U(1) symmetry. v.e.v. SB.

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Hidden local symmetry and infinite tower of vector mesons for baryons

Hidden local symmetry and infinite tower of vector mesons for baryons. Yang, Ghil-Seok ( ? ?? ) . Department of Physics & CHEP ( C enter for H igh E nergy P hysics) Kyungpook Nat'l University.

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Gravity Waves and Linear Inflation from Axion Monodromy

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Advanced ERC Grant: QUAGATUA

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SDiff invariant Bagger-Lambert-Gustavsson

model and its N=8 superspace formulations. SDiff invariant Bagger-Lambert-Gustavsson . Based on I.B. & P. K. Townsend, JHEP 0902, 013 (2009) [ arXiv:0808.1583v2 ] and I. B., Phys.Lett. B 669 , 193 (2008) [ arXiv:0808.3568 ]. Igor A. Bandos

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3d CFT and Multi M2-brane Theory on

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Yoshio Nishina 1890-1951

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Unity of All Elementary-Particle Forces Originally Published by:

Unity of All Elementary-Particle Forces Originally Published by: Howard Georgi and S. L. Glashow on 10 January 1974 Presented by: Stephen Bello. What are the Three Elementary Particle Forces?. Images courtesy of http://hyperphysics.phy-astr.gsu.edu/hbase/forces/funfor.html.

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