2020
DOI: 10.48550/arxiv.2002.11741
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A new energy bound for Einstein-Scalar theory in AlAdS$_4$ and holographic bound for deformed CFT$_3$

Krai Cheamsawat

Abstract: In this work, we derive an upper bound on energetic quantities, namely vacuum energy and free energy, for static solutions of Einstein-Scalar theory in four dimensional asymptotically locally Anti-de Sitter(AlAdS) spacetime with a nontrivial scalar potential where the scalar field mass parameter(m 2 ) is equal to 0 or -2. This system is the holographic dual of strongly coupled conformal field theory(CFT) in three dimensions being deformed by a relevant or marginal scalar operator of conformal dimension ∆ = 1, … Show more

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“…Hence in both cases the sign of a (t) is not immediately clear. However, note that the large-behavior of a (t) can be obtained in the flat-space scaling limit discussed above, and is given in (3.36); assuming a r 0 k (t) is 10 Explicitly, consider the deformed torus ds 2 = e 2f [(dx 1 ) 2 + (dx 2 ) 2 ], where x 1 and x 2 both have periodicity ∆x, and we take f = cos(2πx 1 /∆x) + O( 2 ). The perturbative heat kernel for the Dirac fermion on a deformed torus is computed in [14], and in this case comes out to be…”
Section: Negativity Of ∆Kmentioning
confidence: 99%
“…Hence in both cases the sign of a (t) is not immediately clear. However, note that the large-behavior of a (t) can be obtained in the flat-space scaling limit discussed above, and is given in (3.36); assuming a r 0 k (t) is 10 Explicitly, consider the deformed torus ds 2 = e 2f [(dx 1 ) 2 + (dx 2 ) 2 ], where x 1 and x 2 both have periodicity ∆x, and we take f = cos(2πx 1 /∆x) + O( 2 ). The perturbative heat kernel for the Dirac fermion on a deformed torus is computed in [14], and in this case comes out to be…”
Section: Negativity Of ∆Kmentioning
confidence: 99%