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Current algebra functors and extensions  [PDF]
Anton Alekseev,Pavol Severa,Cornelia Vizman
Mathematics , 2012, DOI: 10.1142/S0129055X13500128
Abstract: We show how the fundamental cocycles on current Lie algebras and the Lie algebra of symmetries for the sigma model are obtained via the current algebra functors. We present current group extensions integrating some of these current Lie algebra extensions.
Extensions of diffeomorphism and current algebras  [PDF]
T. A. Larsson
Physics , 2000,
Abstract: Dzhumadil'daev has classified all tensor module extensions of $diff(N)$, the diffeomorphism algebra in $N$ dimensions, and its subalgebras of divergence free, Hamiltonian, and contact vector fields. I review his results using explicit tensor notation. All of his generic cocycles are limits of trivial cocycles, and many arise from the Mickelsson-Faddeev algebra for $gl(N)$. Then his results are extended to some non-tensor modules, including the higher-dimensional Virasoro algebras found by Eswara Rao/Moody and myself. Extensions of current algebras with $d$-dimensional representations are obtained by restriction from $diff(N+d)$. This gives a connection between higher-dimensional Virasoro and Kac-Moody cocycles, and between Mickelsson-Faddeev cocycles for diffeomorphism and current algebras.
Central extensions of current algebras  [PDF]
Pasha Zusmanovich
Mathematics , 2008, DOI: 10.1090/S0002-9947-10-05304-3
Abstract: This is an old paper put here for archeological purposes. We compute the second cohomology of current Lie algebras of the form $L\otimes A$, where $L$ belongs to some class of Lie algebras which includes classical simple and Zassenhaus algebras, and of some modular semisimple Lie algebras. The results are largely superseded by subsequent papers, though, perhaps, some tricks and observations used here remain of minor interest.
Extensions for Generalized Current Algebras  [PDF]
Brian D. Boe,Christopher M. Drupieski,Tiago R. Macedo,Daniel K. Nakano
Mathematics , 2015,
Abstract: Given a complex semisimple Lie algebra ${\mathfrak g}$ and a commutative ${\mathbb C}$-algebra $A$, let ${\mathfrak g}[A] = {\mathfrak g} \otimes A$ be the corresponding generalized current algebra. In this paper we explore questions involving the computation and finite-dimensionality of extension groups for finite-dimensional ${\mathfrak g}[A]$-modules. Formulas for computing $\operatorname{Ext}^{1}$ and $\operatorname{Ext}^{2}$ between simple ${\mathfrak g}[A]$-modules are presented. As an application of these methods and of the use of the first cyclic homology, we completely describe $\operatorname{Ext}^{2}_{{\mathfrak g}[t]}(L_{1},L_{2})$ for ${\mathfrak g}=\mathfrak{sl}_{2}$ when $L_{1}$ and $L_{2}$ are simple ${\mathfrak g}[t]$-modules that are each given by the tensor product of two evaluation modules.
Simple Current Extensions and Mapping Class Group Representations  [PDF]
Peter Bantay
Physics , 1996, DOI: 10.1142/S0217751X9800007X
Abstract: The conjecture of Fuchs, Schellekens and Schweigert on the relation of mapping class group representations and fixed point resolution in simple current extensions is investigated, and a cohomological interpretation of the untwisted stabilizer is given.
The Untwisted Stabilizer in Simple Current Extensions  [PDF]
Peter Bantay
Physics , 1996, DOI: 10.1016/S0370-2693(97)00110-X
Abstract: A method is presented to compute the order of the untwisted stabilizer of a simple current orbit, as well as some results about the properties of the resolved fields in a simple current extension.
Optimization of the current pulse for spin-torque switches  [PDF]
Tom Dunn,Alex Kamenev
Physics , 2011, DOI: 10.1063/1.3576929
Abstract: We address optimization of the spin current intensity profile needed to achieve spin torque switching of a nanomagnet. For systems with Ohmic dissipation we prove that the optimal current drives the magnetization along the trajectory, which is exact time-reversed replica of the relaxation trajectory towards the equilibrium. In practice it means that the optimal current is very nearly {\em twice} the minimal critical current needed to switch the magnet. Pulse duration of such an optimal current is a slow logarithmic function of temperature and the required probability of switching.
Simple current extensions and permutation orbifolds in string theory  [PDF]
M. Maio
Physics , 2011, DOI: 10.1016/j.nuclphysbps.2011.05.004
Abstract: We review extensions by integer spin simple currents in two-dimensional conformal field theories and their applications in string theory. In particular, we study the problem of resolving the fixed points of a simple current and apply the formalism to the permutation orbifold. In terms of string compactifications, we construct permutations of N=2 minimal models and use them as building blocks in heterotic Gepner models.
Simple current extensions beyond semi-simplicity  [PDF]
Thomas Creutzig,Shashank Kanade,Andrew R. Linshaw
Mathematics , 2015,
Abstract: Let V be a simple VOA and consider a representation category of V that is a vertex tensor category in the sense of Huang-Lepowsky. In particular, this category is a braided tensor category. Let J be an object in this category that is a simple current of order two of either integer or half-integer conformal dimension. We prove that $V\oplus J$ is either a VOA or a super VOA. If the representation category of V is in addition ribbon, then the categorical dimension of J decides this parity question. Combining with Carnahan's work, we extend this result to simple currents of arbitrary order. Our next result is a simple sufficient criterion for lifting indecomposable objects that only depends on conformal dimensions. Several examples of simple current extensions that are $C_2$-cofinite and non-rational are then given and induced modules listed.
Lifts of automorphisms of vertex operator algebras in simple current extensions  [PDF]
Hiroki Shimakura
Mathematics , 2006,
Abstract: In this article, we study isomorphisms between simple current extensions of a simple VOA. For example, we classify the isomorphism classes of simple current extensions of some VOAs. Moreover, we consider the same simple current extension and describe the normalizer of the abelian automorphism group associated with this extension. In particular, we regard the moonshine module as simple current extensions of five subVOAs V_L^+ for 2-elementary totally even lattices L, and describe corresponding five normalizers of elementary abelian 2-group in the automorphism group of the moonshine module in terms of V_L^+. By using this description, we show that three of them form a Monster amalgam.

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