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Degenerate domain walls in supersymmetric theories. [PDF]
Chen S, Ievlev E, Shifman M.
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Geometric-topological deep transfer learning for precise vessel segmentation in 3D medical volumes. [PDF]
Wu J, Wen Z, Zhou H, Sun N, Zhang Y.
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The 3d Mixed BF Lagrangian 1-Form: A Variational Formulation of Hitchin's Integrable System. [PDF]
Caudrelier V +3 more
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Inverse design mechanical metamaterials with dual load-bearing and heat-transfer capabilities. [PDF]
Liu Y.
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Effective field theories of topological crystalline insulators and topological crystals
We present a general approach to obtain effective field theories for topological crystalline insulators whose low-energy theories are described by massive Dirac fermions. We show that these phases are characterized by the responses to spatially dependent
Sheng-Jie Huang +2 more
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Topological anti-topological fusion in four-dimensional superconformal field theories [PDF]
We present some new exact results for general four-dimensional superconformal field theories. We derive differential equations governing the coupling constant dependence of chiral primary correlators.
Kyriakos Papadodimas
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Topological quantum field theory
Publications Mathématiques de l'IHÉS, 1988The starting point to topological quantum field theory was given by \textit{E. Witten} [J. Differ. Geom. 17, 661-692 (1982; Zbl 0499.53056)] where he explained the geometric meaning of super-symmetry, pointing out that for super-symmetric quantum mechanics the Hamiltonian is just the Hodge- Laplacian.
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G-Topological quantum field theory
Boletín de la Sociedad Matemática Mexicana, 2016zbMATH Open Web Interface contents unavailable due to conflicting licenses.
González, Ana, Segovia, Carlos
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1996
A topological field theory generally consists of i) a collection of fields defined on a Riemannian manifold (M, g) ii) a nilpotent operator Q (Q 2 = 0) which is odd with respect to the Grassmann grading iii) physical states defined to be Q.cohomology classes iv) an energy-momentum tensor which is Q—exact i.e.
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A topological field theory generally consists of i) a collection of fields defined on a Riemannian manifold (M, g) ii) a nilpotent operator Q (Q 2 = 0) which is odd with respect to the Grassmann grading iii) physical states defined to be Q.cohomology classes iv) an energy-momentum tensor which is Q—exact i.e.
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