scholarly journals Courant bracket as T-dual invariant extension of Lie bracket

2021 ◽  
Vol 2021 (3) ◽  
Author(s):  
Lj. Davidović ◽  
I. Ivanišević ◽  
B. Sazdović

Abstract We consider the symmetries of a closed bosonic string, starting with the general coordinate transformations. Their generator takes vector components ξμ as its parameter and its Poisson bracket algebra gives rise to the Lie bracket of its parameters. We are going to extend this generator in order for it to be invariant upon self T-duality, i.e. T-duality realized in the same phase space. The new generator is a function of a 2D double symmetry parameter Λ, that is a direct sum of vector components ξμ, and 1-form components λμ. The Poisson bracket algebra of a new generator produces the Courant bracket in a same way that the algebra of the general coordinate transformations produces Lie bracket. In that sense, the Courant bracket is T-dual invariant extension of the Lie bracket. When the Kalb-Ramond field is introduced to the model, the generator governing both general coordinate and local gauge symmetries is constructed. It is no longer self T-dual and its algebra gives rise to the B-twisted Courant bracket, while in its self T-dual description, the relevant bracket becomes the θ-twisted Courant bracket. Next, we consider the T-duality and the symmetry parameters that depend on both the initial coordinates xμ and T-dual coordinates yμ. The generator of these transformations is defined as an inner product in a double space and its algebra gives rise to the C-bracket.

2021 ◽  
Vol 81 (8) ◽  
Author(s):  
Ljubica Davidović ◽  
Ilija Ivanišević ◽  
Branislav Sazdović

AbstractWe obtain the Courant bracket twisted simultaneously by a 2-form B and a bi-vector $$\theta $$ θ by calculating the Poisson bracket algebra of the symmetry generator in the basis obtained acting with the relevant twisting matrix. It is the extension of the Courant bracket that contains well known Schouten–Nijenhuis and Koszul bracket, as well as some new star brackets. We give interpretation to the star brackets as projections on isotropic subspaces.


1990 ◽  
Vol 05 (24) ◽  
pp. 4753-4767 ◽  
Author(s):  
GUSTAV W. DELIUS

The N = 2 super-Kac-Moody algebra is defined as the algebra corresponding to an N = 2 superloop group. Using the method of coadjoint orbits, which is explained, an action is derived which has the N = 2 super-Kac-Moody algebra as its Poisson bracket algebra and is invariant under the N = 2 superloop group. It is invariant under N = 2 superconformal transformations. This action is thus the generalization of the WZW model to (2,0) superspace. We study the relation to the known WZW model in (1,0) superspace after imposing a constraint on the (2,0) superfield.


1992 ◽  
Vol 07 (24) ◽  
pp. 6159-6174 ◽  
Author(s):  
G. BIMONTE ◽  
P. SALOMONSON ◽  
A. SIMONI ◽  
A. STERN

We examine the Wess-Zumino-Novikov-Witten (WZNW) model on a circle and compute the Poisson bracket algebra for left- and right-moving chiral group elements. Our computations apply for arbitrary groups and arbitrary boundary conditions, the latter being characterized by the monodromy matrix. Unlike in previous treatments, the Poisson brackets do not require specifying a particular parametrization of the group valued fields in terms of angles spanning the group. We do however find it necessary to make a gauge choice, as the chiral group elements are not gauge invariant observables. (On the other hand, the quadratic form of the Poisson brackets may be defined independently of a gauge fixing.) Gauge invariant observables can be formed from the monodromy matrix and these observbles are seen to commute in the quantum theory.


2007 ◽  
Vol 04 (04) ◽  
pp. 517-522 ◽  
Author(s):  
A. V. BRATCHIKOV

In a Hamiltonian system with first class constraints, observables can be defined as elements of a quotient Poisson bracket algebra. In the gauge fixing method, observables form a quotient Dirac bracket algebra. We show that these two algebras are isomorphic. A new realization of the observable algebras through the original Poisson bracket is found. Generators, brackets and pointwise products of the algebras under consideration are calculated.


1996 ◽  
Vol 11 (27) ◽  
pp. 4815-4835 ◽  
Author(s):  
F. DELDUC ◽  
M. MAGRO

We study the Poisson bracket algebra of the (N = 2)-supersymmetric chiral WZNW model in superspace. It involves two classical r matrices, one of which comes from the geometrical constraints implied by N = 2 supersymmetry. The phase space itself consists of superfields satisfying constraints involving this r matrix. An attempt is made to relax these constraints. The symmetries of the model are investigated.


1998 ◽  
Vol 09 (05) ◽  
pp. 599-621 ◽  
Author(s):  
BYUNG-JAY KAHNG

As a generalization of the linear Poisson bracket on the dual space of a Lie algebra, we introduce certain nonlinear Poisson brackets which are "cocycle perturbations" of the linear Poisson bracket. We show that these special Poisson brackets are equivalent to Poisson brackets of central extension type, which resemble the central extensions of an ordinary Lie bracket via Lie algebra cocycles. We are able to formulate (strict) deformation quantizations of these Poisson brackets by means of twisted group C*-algebras. We also indicate that these deformation quantizations can be used to construct some specific non-compact quantum groups.


1989 ◽  
Vol 04 (04) ◽  
pp. 339-349 ◽  
Author(s):  
S. JAMES GATES ◽  
PARTHASARATHI MAJUMDAR

The superparticle model with Siegel's modification is generalized to include a one-dimensional local world line supersymmetry. The constraints of the model are shown to yield a Poisson bracket algebra that closes. The quantization of the system in the light cone gauge produces a spectrum of states identical to that obtained for the spinning superparticle model without Siegel's modification.


1997 ◽  
Vol 09 (01) ◽  
pp. 1-27 ◽  
Author(s):  
Janusz Grabowski

A Z-graded Lie bracket { , }P on the exterior algebra Ω(M) of differential forms, which is an extension of the Poisson bracket of functions on a Poisson manifold (M,P), is found. This bracket is simultaneously graded skew-symmetric and satisfies the graded Jacobi identity. It is a kind of an 'integral' of the Koszul–Schouten bracket [ , ]P of differential forms in the sense that the exterior derivative is a bracket homomorphism: [dμ, dν]P=d{μ, ν}P. A naturally defined generalized Hamiltonian map is proved to be a homomorphism between { , }P and the Frölicher–Nijenhuis bracket of vector valued forms. Also relations of this graded Poisson bracket to the Schouten–Nijenhuis bracket and an extension of { , }P to a graded bracket on certain multivector fields, being an 'integral' of the Schouten–Nijenhuis bracket, are studied. All these constructions are generalized to tensor fields associated with an arbitrary Lie algebroid.


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