Chern–Simons form

Results: 27



#Item
1A ugus t 2 1 , Remembering Chern  2

A ugus t 2 1 , Remembering Chern 2

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Source URL: www.icm2010.in

Language: English - Date: 2012-02-02 09:07:26
2Chern-Simons Potential in Models of Casimir Effect Yury M.Pis’mak Department of Theoretical Physics, State University Saint-Petersburg

Chern-Simons Potential in Models of Casimir Effect Yury M.Pis’mak Department of Theoretical Physics, State University Saint-Petersburg

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Source URL: hep.phys.spbu.ru

Language: English - Date: 2013-11-21 08:50:42
3Geometric perspectives on topological action functionals Hisham Sati We describe the extended prequantum theory of Chern-Simons-type gauge field theories, which are the most prominent examples of topological field theori

Geometric perspectives on topological action functionals Hisham Sati We describe the extended prequantum theory of Chern-Simons-type gauge field theories, which are the most prominent examples of topological field theori

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Source URL: qcpages.qc.cuny.edu

Language: English - Date: 2014-08-06 07:54:55
4ESI  The Erwin Schrodinger International Institute for Mathematical Physics  Pasteurgasse 4/7

ESI The Erwin Schrodinger International Institute for Mathematical Physics Pasteurgasse 4/7

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Source URL: www.mat.univie.ac.at

Language: English - Date: 2009-12-11 06:14:30
51-Loop Corrections in AdS4 x CP3 Arthur Lipstein Johns Hopkins[removed]Reference: hep-th[removed]by AL and M. Bandres)

1-Loop Corrections in AdS4 x CP3 Arthur Lipstein Johns Hopkins[removed]Reference: hep-th[removed]by AL and M. Bandres)

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Source URL: www.pha.jhu.edu

Language: English - Date: 2010-01-26 20:11:45
6Week 2 (due April[removed]In three space-time dimensions, there exists an alternative gaugeinvariant action for a gauge field Aµ : Z SCS = k d3 x ǫµνρ Aµ ∂ν Aρ . Here ǫµνρ is the completely antisymmetric ten

Week 2 (due April[removed]In three space-time dimensions, there exists an alternative gaugeinvariant action for a gauge field Aµ : Z SCS = k d3 x ǫµνρ Aµ ∂ν Aρ . Here ǫµνρ is the completely antisymmetric ten

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Source URL: www.theory.caltech.edu

Language: English - Date: 2008-04-09 21:16:53
7Week 5 (due May 7) Reading: Srednicky, sections 71, 72. See also Peskin-Schroeder for a better explanation of the Faddeev-Popov gauge-fixing procedure. 1. (a) Derive the equations of motion following from the Yang-Mills

Week 5 (due May 7) Reading: Srednicky, sections 71, 72. See also Peskin-Schroeder for a better explanation of the Faddeev-Popov gauge-fixing procedure. 1. (a) Derive the equations of motion following from the Yang-Mills

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Source URL: www.theory.caltech.edu

Language: English - Date: 2010-05-01 14:58:42
8Week 9 (due March[removed]Consider a theory of a gauge field Aµ and a real scalar σ with the Lagrangian 1 L = − Fµν F µν − M 2 Dµ σDµ σ, 4

Week 9 (due March[removed]Consider a theory of a gauge field Aµ and a real scalar σ with the Lagrangian 1 L = − Fµν F µν − M 2 Dµ σDµ σ, 4

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Source URL: www.theory.caltech.edu

Language: English - Date: 2010-03-07 11:03:40
9Week 9 (due March[removed]Compute the Chern-Simons 5-form and 7-form. 2. Consider a gauge theory on a Riemannian 3-manifold M with gauge group U (N ) and an action Z Z

Week 9 (due March[removed]Compute the Chern-Simons 5-form and 7-form. 2. Consider a gauge theory on a Riemannian 3-manifold M with gauge group U (N ) and an action Z Z

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Source URL: www.theory.caltech.edu

- Date: 2009-03-04 22:30:40
    10Microsoft PowerPoint - AMSTalk_Jan7_2009C

    Microsoft PowerPoint - AMSTalk_Jan7_2009C

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    Source URL: www.physics.rutgers.edu

    Language: English - Date: 2010-11-16 18:33:41