2019
DOI: 10.1007/jhep08(2019)057
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SO(8) supergravity and the magic of machine learning

Abstract: Using de Wit-Nicolai D = 4 N = 8 SO(8) supergravity as an example, we show how modern Machine Learning software libraries such as Google's TensorFlow can be employed to greatly simplify the analysis of high-dimensional scalar sectors of some M-Theory compactifications. We provide detailed information on the location, symmetries, and particle spectra and charges of 192 critical points on the scalar manifold of SO(8) supergravity, including one newly discovered N = 1 vacuum with SO(3) residual symmetry, one new … Show more

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Cited by 48 publications
(110 citation statements)
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“…By implementing a generalised S-S ansatz in E 7(7) -EFT, we uplifted the AdS 4 vacuum to a new family of AdS 4 × S 1 × S 5 S-folds of type IIB supergravity with hyperbolic monodromies M(k) = −S T k (with k ≥ 3 ) along S 1 . The residual SU(2) × U(1) symmetry and N = 2 supersymmetry of the AdS 4 vacuum are realised on the S-folds: the internal S 5 is deformed into a product of S 2 and (squashed) S 3 with SU(2) × U(1) σ × U(1) φ isometries and a warping factor, whereas the 4 The two terms in B2 and C2 which are proportional to σ1 ∧ σ3 can be eliminated by means of a gauge transformation of the form B2 → B2 − d 2 √ 2 ∆ 4 e −η sin(2θ) cos θ cos ψ σ2 , C2 → C2 + d 2 √ 2 ∆ 4 e η sin(2θ) cos θ sin ψ σ2 , (3.45) where we have shifted the coordinate φ → ψ + π 4 . However, since these terms are generated by the generalised S-S ansatz discussed in Section 3.1, we will retain them here.…”
Section: Discussionmentioning
confidence: 99%
“…By implementing a generalised S-S ansatz in E 7(7) -EFT, we uplifted the AdS 4 vacuum to a new family of AdS 4 × S 1 × S 5 S-folds of type IIB supergravity with hyperbolic monodromies M(k) = −S T k (with k ≥ 3 ) along S 1 . The residual SU(2) × U(1) symmetry and N = 2 supersymmetry of the AdS 4 vacuum are realised on the S-folds: the internal S 5 is deformed into a product of S 2 and (squashed) S 3 with SU(2) × U(1) σ × U(1) φ isometries and a warping factor, whereas the 4 The two terms in B2 and C2 which are proportional to σ1 ∧ σ3 can be eliminated by means of a gauge transformation of the form B2 → B2 − d 2 √ 2 ∆ 4 e −η sin(2θ) cos θ cos ψ σ2 , C2 → C2 + d 2 √ 2 ∆ 4 e η sin(2θ) cos θ sin ψ σ2 , (3.45) where we have shifted the coordinate φ → ψ + π 4 . However, since these terms are generated by the generalised S-S ansatz discussed in Section 3.1, we will retain them here.…”
Section: Discussionmentioning
confidence: 99%
“…The numerical data for the N = 1 critical point, S1384096, in [1] point towards additional symmetry, which we identify as a discrete Z 2 subgroup of the SO(8) gauge group. The resulting SO(3) × Z 2 -invariant truncation of the N = 8 supergravity can be constructed analytically.…”
Section: Introductionmentioning
confidence: 90%
“…Recently, a new numerical approach based on Machine Learning (ML) software libraries, such as Google's TensorFlow [30], was employed in [1] to simplify the analysis of the potential resulting in the total of 192 critical points together with a precise information about those points that includes the mass spectra of small fluctuations and unbroken (super)symmetries. It is expected that this list of critical points should be nearly complete.…”
Section: Introductionmentioning
confidence: 99%
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