'Su 2' diaporamas de présentation

d=4, N =2, Field Theory and Physical Mathematics

d=4, N =2, Field Theory and Physical Mathematics. Gregory Moore. Rutgers University. ICMP, Aalborg, Denmark, August 8, 2012. This is a review talk. For my recent research results see my talk at Strings-Math, Bonn, 2012:

1.31k views • 118 slides

8. The Group SU(2) and more about SO(3)

8. The Group SU(2) and more about SO(3). SU(2) = Group of 2 ?2 unitary matrices with unit determinant. Simplest non-Abelian Lie group. Locally equivalent to SO(3); share same Lie algebra. Compact & simply connected ? All IRs are single-valued.

1.34k views • 66 slides

Surface Defects and the BPS Spectrum of 4d N=2 Theories

Surface Defects and the BPS Spectrum of 4d N=2 Theories. IHES, May 17, 2011. Gregory Moore, Rutgers University. Davide Gaiotto , G.M. , Andy Neitzke. Wall-crossing in Coupled 2d-4d Systems: 1103.2598 Framed BPS States: 1006.0146

729 views • 62 slides

Supersymmetry I

Supersymmetry I. Hitoshi Murayama Taiwan Spring School March 29, 2002. Why Beyond the Standard Model. Standard Model is sooooo successful. But none of us are satisfied with the SM. Why? Because it leaves so many great questions unanswered ? Drive to go beyond the Standard Model.

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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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Probability

Probability. Probability. Probability is a measure of the possibility of an event happening Measure on a scale between zero and one Probability has a substantial role to play in financial analysis as the outcomes of financial decisions are uncertain e.g. Fluctuation in share prices.

711 views • 49 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

Kazuki Hasebe

Fuzzy Geometry, Supersymmetry, and Many-body Physics. 24-28 Aug. 2010, @ Supersymmetry in Integrable Systems, Yerevan, Armenia. Kazuki Hasebe. (Kagawa N.C.T.). Based on the works (2005 ? 2010) with Yusuke Kimura , Daniel P. Arovas , Xiaoliang Qi , Shoucheng Zhang ,

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LLM geometries in M-theory and probe branes inside them

LLM geometries in M-theory and probe branes inside them. Jun-Bao Wu IHEP, CAS Nov. 24, 2010, KITPC. Based on. B. Chen, E. O Colgain, JW, H. Yavartanoo, JHEP 04 (2010)078, 1001.0906. E. O Colgain, JW, H. Yavartanoo, JHEP 08 (2010)114, 1005.4527. E. O Colgain, JW, H. Yavartanoo,

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Magnetic Monopoles

Magnetic Monopoles. Hermann Kolanoski, AMANDA Literature Discussion 8.+15.Feb.2005. How large is a monopole? Is a monopole a particle? How do monopoles interact? What are topological charges? What is a homotopy class?. Content: Dirac monopoles Topological charges

589 views • 29 slides

A MODEL BUILDING BY COSET SPACE DIMENSIONAL REDUCTION USING 10 DIMENSIONAL COSET SPACES

A MODEL BUILDING BY COSET SPACE DIMENSIONAL REDUCTION USING 10 DIMENSIONAL COSET SPACES. collaborators. Takaaki Nomura(Saitama univ). Masahumi Koike, Toshihumi Jitto, Joe Sato (Saitama univ). Takashi Shimomura (University of valencia). 2007 12/18 GUT07 (Ritsumeikan uviv). Outline.

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A MODEL BUILDING BY COSET SPACE DIMENSIONAL REDUCTION USING 10 DIMENSIONAL COSET SPACES

A MODEL BUILDING BY COSET SPACE DIMENSIONAL REDUCTION USING 10 DIMENSIONAL COSET SPACES. collaborators. Takaaki Nomura(Saitama univ). Masahumi Koike, Toshihumi Jitto, Joe Sato (Saitama univ). Takashi Shimomura (University of valencia). 2007 12/13 KEK. Outline. Introduction CSDR scheme

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Discrete and Unified Ideas on Fermion Mixing

Discrete and Unified Ideas on Fermion Mixing. symmetries for the understanding of neutrino data. Michele Frigerio University of California, Riverside. AHEP Seminar @ IFIC Valencia, March 14, 2005. The Flavor Problem. Standard Model contains 13 free parameters in the Yukawa sector .

338 views • 24 slides

Application of the Cluster Embedding Method to Transport Through Anderson Impurities

Application of the Cluster Embedding Method to Transport Through Anderson Impurities. A method to study highly correlated nanostructures. George Martins Carlos Busser Physics Department Oakland University. Colaboracion Interamericana de Materiais. Materials World Network.

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AGT ??? (1) Gaiotto ??? (String Advanced Lectures No.18)

AGT ??? (1) Gaiotto ??? (String Advanced Lectures No.18). ????????????? (KEK) ????????? (IPNS) ????? 2010 ? 6 ? 2 ???? 12:30-14:30. Contents. 1. Seiberg-Witten curve 2. SU(2) generalized quivers 3. SU(3) generalized quivers 4. SU(N) generalized quivers 5. Towards AGT relation.

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Contributions to ? parameter from heavy gauge bosons in Littlest Higgs model with T-parity

Contributions to ? parameter from heavy gauge bosons in Littlest Higgs model with T-parity. The Graduate University for Advanced Studies. Masaki Asano. hep-ph/0602157. Collaborated with. Shigeki Matsumoto, Nobuchika Okada, Yasuhiro Okada. In the Standard Model. http://map.gsfc.nasa.gov/.

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Resonant signature of the Littlest Higgs model with T-parity at Linear Colliders

Resonant signature of the Littlest Higgs model with T-parity at Linear Colliders. Shigeki Matsumoto (KEK, Theory). Collider signatures of the Little Higgs model with T-parity, with focusing on the production of the T - quark at ILC.

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AGT ??? (2) AGT ??? (String Advanced Lectures No.19)

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553 views • 11 slides

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