2008
DOI: 10.1088/1126-6708/2008/10/085
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Exploring pure spinor string theory onAdS4× ℂℙ3

Abstract: In this paper we formulate the pure spinor superstring theory on AdS 4 × CP 3 . By recasting the pure spinor action as a topological A-model on the fermionic supercoset Osp(6|4)/SO(6) × Sp(4) plus a BRST exact term, we prove the exactness of the σmodel. We then give a gauged linear σ-model which reduces to the superstring in the limit of large volume and we study its branch geometry in different phases. Moreover, we discuss possible D-brane boundary conditions and the principal chiral model for the fermionic s… Show more

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Cited by 69 publications
(37 citation statements)
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“…We have also obtained the explicit form of the spin connection of the AdS 4 × CP 3 superspace (to the second order in υ) which was left out in [7]. In contrast to the Green-Schwarz formulation, the knowledge of the form of the spin connection is required, for instance, for the pure spinor description of superstrings in curved superbackgrounds [17] and, in particular, is needed for extending to the full AdS 4 × CP 3 superspace the supercoset pure-spinor sigma-model of [18,19,20]. With some more efforts, which will be made elsewhere, one can also compute the form of the superfield strengths F 2 and F 4 of the RR fluxes in type IIA AdS 2 × S 2 × T 6 superbackgrounds and corresponding quantities describing this superbackground in the type IIB case.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…We have also obtained the explicit form of the spin connection of the AdS 4 × CP 3 superspace (to the second order in υ) which was left out in [7]. In contrast to the Green-Schwarz formulation, the knowledge of the form of the spin connection is required, for instance, for the pure spinor description of superstrings in curved superbackgrounds [17] and, in particular, is needed for extending to the full AdS 4 × CP 3 superspace the supercoset pure-spinor sigma-model of [18,19,20]. With some more efforts, which will be made elsewhere, one can also compute the form of the superfield strengths F 2 and F 4 of the RR fluxes in type IIA AdS 2 × S 2 × T 6 superbackgrounds and corresponding quantities describing this superbackground in the type IIB case.…”
Section: Resultsmentioning
confidence: 99%
“…where κ α (ξ) is a 32-component spinor parameter, 19) and g ij is an induced worldsheet metric. The string equations of motion (2.15) and (2.16) transform into each other under the kappa-symmetry variations.…”
Section: Lax Connection and Kappa-symmetrymentioning
confidence: 99%
“…At strong coupling the situation is less clear: in [75] and [78] the coefficient h 0 was argued to be 0 whereas in [109] some evidence was given in favor of a different value − log 2 2π (see also [74]). Hopefully this issue could be analyzed from world-sheet sigma model first principles calculation like in [79,80]. Equation (2.1) admits two solutions, and we define two branches of the function x(u), which are called "mirror" and "physical":…”
Section: Jhep06(2010)088mentioning
confidence: 99%
“…The recent developments on the duality between N = 6 superconformal Chern-Simons theory in three dimensions and superstrings moving on AdS 4 ×P 3 [1,2,3,4,6,7,8,9,10] have prompted the study of superstrings on Osp(N |4) backgrounds [11,12,13,14]. The main issue is of course the integrability of the system and this has been already studied in a series of papers [15,16,17,18,19,20,21,22,23,24,25,26].…”
Section: Introductionmentioning
confidence: 99%
“…On the other side, one would like also to consider the string theory in a framework where all symmetries are manifest and which takes the RR fields of the background properly into account. In [14], the limit for large RR fields is analyzed and it has been shown the relation with a topological model on the Grassmannian Osp( |4)/SO(6) × Sp (4). The exactness of the background is also discussed in [14].…”
Section: Introductionmentioning
confidence: 99%