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Courant Bracket Twisted Both by a 2-Form B and by a Bi-Vector Θ

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Courant Bracket Twisted Both by a 2-Form B and by a Bi-Vector Θ Eur. Phys. J. C (2021) 81:685 https://doi.org/10.1140/epjc/s10052-021-09447-4 Regular Article - Theoretical Physics Courant bracket twisted both by a 2-form B and by a bi-vector θ Ljubica Davidovi´ca, Ilija Ivaniševi´cb, Branislav Sazdovi´cc Institute of Physics, University of Belgrade, Pregrevica 118, 11080 Belgrade, Serbia Received: 6 May 2021 / Accepted: 12 July 2021 © The Author(s) 2021 Abstract We obtain the Courant bracket twisted simulta- obtained from the action of the appropriate O(D, D) trans- neously by a 2-form B and a bi-vector θ by calculating the formation [8]. The Courant bracket is usually twisted by a Poisson bracket algebra of the symmetry generator in the 2-form B, giving rise to what is known as the twisted Courant basis obtained acting with the relevant twisting matrix. It is bracket [9], and by a bi-vector θ, giving rise to the θ-twisted the extension of the Courant bracket that contains well known Courant bracket [10]. In [3,8,11,12], the former bracket was Schouten–Nijenhuis and Koszul bracket, as well as some new obtained in the generalized currents algebra, and it was shown star brackets. We give interpretation to the star brackets as to be related to the latter by self T-duality [13], when the T- projections on isotropic subspaces. dual of the B field is the bi-vector θ. The B-twisted Courant bracket contains H flux, while the θ-twisted Courant bracket contains non-geometric Q and R 1 Introduction fluxes. The fluxes are known to play a crucial role in the compactification of additional dimensions in string theory The Courant bracket [1,2] represents the generalization of [14]. Non-geometric fluxes can be used to stabilize moduli. In the Lie bracket on spaces of generalized vectors, understood this paper, we are interested in obtaining the Poisson bracket as the direct sum of the elements of the tangent bundle and representation of the twisted Courant brackets that contain the elements of the cotangent bundle. It was obtained in the all fluxes from the generators algebra. Though it is possible algebra of generalized currents firstly in [3]. Generalized cur- to obtain various twists of the C-bracket as well [15], we do rents are arbitrary functionals of the fields, parametrized by not deal with them in this paper. a pair of vector field and covector field on the target space. The realization of all fluxes using the generalized geom- Although the Lie bracket satisfies the Jacobi identity, the etry was already considered, see [16] for a comprehensive Courant bracket does not. review. In [17], one considers the generalized tetrads origi- In bosonic string theory, the Courant bracket is govern- nating from the generalized metric of the string Hamiltonian. ing both local gauge and general coordinate transformations, As the Lie algebra of tetrads originating from the initial met- invariant upon T-duality [4,5]. It is a special case of the more ric defines the geometric flux, it is suggested that all the general C-bracket [6,7]. The C-bracket is obtained as the other fluxes can be extracted from the Courant bracket of T-dual invariant bracket of the symmetry generator algebra, the generalized tetrads. Different examples of O(D, D) and when the symmetry parameters depend both on the initial and O(D) × O(D) transformations of generalized tetrads lead T-dual coordinates. It reduces to the Courant bracket once to the Courant bracket algebras with different fluxes as its when parameters depend solely on the coordinates from the structure constants. initial theory. In [18], one considers the standard Lie algebroid defined It is possible to obtain the twisted Courant bracket, when with the Lie bracket and the identity map as an anchor on the the self T-dual generator algebra is considered in the basis tangent bundle, as well as the Lie algebroid with the Koszul bracket and the bi-vector θ as an anchor on the cotangent Work supported in part by the Serbian Ministry of Education and bundle. The tetrad basis in these Lie algebroids is suitable Science, under Contract no. 171031. for defining the geometric f and non-geometric Q fluxes. a e-mail: [email protected] It was shown that by twisting both of these Lie algebroids b e-mail: [email protected] (corresponding author) by H-flux one can construct the Courant algebroid, which c e-mail: [email protected] gives rise to all of the fluxes in the Courant bracket algebra. 0123456789().: V,-vol 123 685 Page 2 of 15 Eur. Phys. J. C (2021) 81:685 Unlike previous approaches where generalized fluxes were Lastly, we return to the previous basis and obtain the full defined using the Courant bracket algebra, in a current paper expression for the Courant bracket twisted by both B and θ. we obtain them in the Poisson bracket algebra of the sym- It has a similar form as C˚ -twisted Courant bracket, but in this metry generator. case the other brackets contained within it are also twisted. Firstly, we consider the symmetry generator of local gauge The Courant bracket twisted by both B and θ and the one and global coordinate transformations, defined as a standard twisted by C˚ are directly related by a O(D, D) transforma- inner product in the generalized tangent bundle of a dou- tion represented with the block diagonal matrix. ble gauge parameter and a double canonical variable. The O(D, D) group transforms the double canonical variable into some other basis, in terms of which the symmetry gen- 2 The bosonic string essentials erator can be expressed. We demonstrate how the Poisson bracket algebra of this generator can be used to obtain twist The canonical Hamiltonian for closed bosonic string, moving of the Courant bracket by any such transformation. We give a in the D-dimensional space-time with background charac- Bˆ θˆ brief summary of how e and e produce respectively the B- terized by the metric field Gμν and the antisymmetric Kalb– θ twisted and -twisted Courant bracket in the Poisson bracket Ramond field Bμν is given by [19,20] algebra of generators [8]. B˘ κ Secondly, we consider the matrix e used for twisting the 1 −1 μν μ E ν HC = πμ(G ) πν + x Gμν x Courant bracket simultaneously by a 2-form and a bi-vector. 2κ 2 ˘ μ −1 ρν The argument B is defined simply as a sum of the arguments −2x Bμρ (G ) πν, (2.1) Bˆ and θˆ. Unlike Bˆ or θˆ, the square of B˘ is not zero. The full Taylor series gives rise to the hyperbolic functions of the where πμ are canonical momenta conjugate to coordinates parameter depending on the contraction of the 2-form with xμ, and μ μρ the bi-vector α ν = 2κθ Bρν. We represent the symme- try generator in the basis obtained acting with the twisting E = − ( −1 ) ˘ Gμν Gμν 4 BG B μν (2.2) matrix eB on the double canonical variable. This generator is manifestly self T-dual and its algebra closes on the Courant is the effective metric. The Hamiltonian can be rewritten in bracket twisted by both B and θ. the matrix notation Instead of computing the B − θ twisted Courant bracket directly, we introduce the change of basis in which we define 1 some auxiliary generators, in order to simplify the calcula- H = (X T )M H X N , C κ MN (2.3) tions. This change of basis is also realized by the action of 2 an element of the O(D, D) group. The structure constants M appearing in the Poisson bracket algebra have exactly the where X is a double canonical variable given by same form as the generalized fluxes obtained in other papers μ [16–18]. The expressions for fluxes is given in terms of new M κx μ X = , (2.4) auxiliary fields B˚ and θ˚, both being the function of α . πμ The algebra of these new auxiliary generators closes on another bracket, that we call C˚ -twisted Courant bracket. We and HMN is the so called generalized metric, given by obtain its full Poisson bracket representation, and express it in terms of generalized fluxes. We proceed with rewrit- E − ( −1)ρν ing it in the coordinate free notation, where many terms are = Gμν 2Bμρ G , HMN ( −1)μρ ( −1)μν (2.5) recognized as the well known brackets, such as the Koszul 2 G Bρν G or Schouten–Nijenhuis bracket, but some new brackets, that we call star brackets, also appear. These star brackets as a with M, N ∈{0, 1}. In the context of generalized geometry domain take the direct sum of tangent and cotangent bun- [21], the double canonical variable X M represents the gen- dle, and as a result give the graph of the bi-vector θ˚ in the eralized vector. The generalized vectors are 2D structures cotangent bundle, i.e. the sub-bundle for which the vector that combine both vector and 1-form components in a single μ μν and 1-form components are related as ξ = κθ˚ λν.We entity. show that they can be defined in terms of the projections on The standard T-duality [22,23] laws for background fields isotropic subspaces acting on different twists of the Courant have been obtained by Buscher [24] bracket. μν − μν μν κ μν G = (G 1) , B = θ , (2.6) E 2 123 Eur. Phys. J. C (2021) 81:685 Page 3 of 15 685 ( −1)μν ξ where G E is the inverse of the effective metric (2.2), where iξ is the interior product along the vector field , and μν and θ is the non-commutativity parameter, given by ηMN is O(D, D) metric, given by θ μν =−2 ( −1)μρ ( −1)σν.
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