Javascript must be enabled to continue!
Bubble instabilities of mIIA on AdS$_4\times S^6$
View through CrossRef
We consider compactifications of massive IIA supergravity on a
six-sphere. This setup is known to give rise to non-supersymmetric
AdS_44
vacua preserving \mathrm{SO}(7)SO(7)
as well as G_22
residual symmetry. Both solutions have a round
S^6S6
metric and are supported by the Romans’ mass and internal
F_{6}F6
flux. While the \mathrm{SO}(7)SO(7)
invariant vacuum is known to be perturbatively unstable, the
G_22
invariant one has been found to have a fully stable Kaluza-Klein
spectrum. Moreover, it has been shown to be protected against brane-jet
instabilities. Motivated by these results, we study possible bubbling
solutions connected to the G_22
vacuum, representing non-perturbative instabilities of the latter. We
indeed find an instability channel represented by the nucleation of a
bubble of nothing dressed up with a homogeneous D2 brane charge
distribution in the internal space. Our solution generalizes to the case
where S^6S6
is replaced by any six-dimensional nearly-K"ahler manifold.
Title: Bubble instabilities of mIIA on AdS$_4\times S^6$
Description:
We consider compactifications of massive IIA supergravity on a
six-sphere.
This setup is known to give rise to non-supersymmetric
AdS_44
vacua preserving \mathrm{SO}(7)SO(7)
as well as G_22
residual symmetry.
Both solutions have a round
S^6S6
metric and are supported by the Romans’ mass and internal
F_{6}F6
flux.
While the \mathrm{SO}(7)SO(7)
invariant vacuum is known to be perturbatively unstable, the
G_22
invariant one has been found to have a fully stable Kaluza-Klein
spectrum.
Moreover, it has been shown to be protected against brane-jet
instabilities.
Motivated by these results, we study possible bubbling
solutions connected to the G_22
vacuum, representing non-perturbative instabilities of the latter.
We
indeed find an instability channel represented by the nucleation of a
bubble of nothing dressed up with a homogeneous D2 brane charge
distribution in the internal space.
Our solution generalizes to the case
where S^6S6
is replaced by any six-dimensional nearly-K"ahler manifold.
Related Results
Hubungan Perilaku Pola Makan dengan Kejadian Anak Obesitas
Hubungan Perilaku Pola Makan dengan Kejadian Anak Obesitas
<p><em><span style="font-size: 11.0pt; font-family: 'Times New Roman',serif; mso-fareast-font-family: 'Times New Roman'; mso-ansi-language: EN-US; mso-fareast-langua...
Vapor Bubble Interaction With a Superheated Wall
Vapor Bubble Interaction With a Superheated Wall
Sliding bubbles are known to augment heat transfer rates on the surface on which they slide. The pre-cursor problem — the bubble approaching an inclined superheated wall provides t...
Numerical investigation of central breakup of large bubble induced by liquid jet
Numerical investigation of central breakup of large bubble induced by liquid jet
A large spherical bubble rising in quiescent liquid generally leads to the formation of a toroidal bubble (central breakup). In this paper, we investigate the bubble dynamics durin...
A.D.S. Wet Welding
A.D.S. Wet Welding
Abstract
The purpose of this paper is to discuss wet welding using fully anthropomorphic atmospheric diving suits and offer proof that wet welding operations are ...
A cross‐cultural content analysis of restaurant ads in New Zealand
A cross‐cultural content analysis of restaurant ads in New Zealand
Unlike many other cross‐cultural advertising comparisons, this study compares two different cultures within the same country, and the topic of the content analysis is narrowed down...
Oxygen transfer from bubble-plumes
Oxygen transfer from bubble-plumes
Air-bubble plumes produced beneath ocean breaking waves have important roles in gas transfer between atmosphere and ocean because the gas within the bubbles, convected by breaking-...
PD characteristics and deterioration mechanism of oil-impregnated pressboard with bubble defect
PD characteristics and deterioration mechanism of oil-impregnated pressboard with bubble defect
The bubbles are typical defects of oil-paper insulation systems, and
partial discharge (PD) initiated by them can significantly degrade the
insulating performance of oil-paper insu...
Effect of film viscoelasticity on the finite deformation of a spherical bubble
Effect of film viscoelasticity on the finite deformation of a spherical bubble
According to the strain energy density function for finite deformation of viscoelastic material, the relaxation function of the Maxwell mode, and the deformation gradient tensor of...

