2022
DOI: 10.48550/arxiv.2204.06391
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Chaotic instability in the BFSS matrix model

Abstract: Chaotic scattering is a manifestation of transient chaos realized by the scattering with non-integrable potential. When the initial position is taken in the potential, a particle initially exhibits chaotic motion, but escapes outside after a certain period of time. The time to stay inside the potential can be seen as lifetime and this escape process may be regarded as a kind of instability. The process of this type exists in the Banks-Fischler-Shenker-Susskind (BFSS) matrix model in which the potential has fla… Show more

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Cited by 1 publication
(3 citation statements)
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“…The Yang-Mills energy momentum tensor T µν in ( 13), (15) [75,76,77,79] and therefore opens a room of possibilities for a vector field driven cosmology and inflation [3]. The space homogeneous gauge fields are described by a classical mechanical system, so called Yang-Mills classical mechanics (YMCM) [75,76,77,79,78,80,81,82,84,85,86,87,88,89,90,91,92,93,95,96,97,98,99], it represents the bosonic part of the matrix models [85,86,81,87,88,89,90,91] and were considered in the context of the cosmological models in [109,110,111,112,113,114,115,116,117,118,…”
Section: Equation Of State Describing Gauge Field Theory Vacuum Fluct...mentioning
confidence: 99%
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“…The Yang-Mills energy momentum tensor T µν in ( 13), (15) [75,76,77,79] and therefore opens a room of possibilities for a vector field driven cosmology and inflation [3]. The space homogeneous gauge fields are described by a classical mechanical system, so called Yang-Mills classical mechanics (YMCM) [75,76,77,79,78,80,81,82,84,85,86,87,88,89,90,91,92,93,95,96,97,98,99], it represents the bosonic part of the matrix models [85,86,81,87,88,89,90,91] and were considered in the context of the cosmological models in [109,110,111,112,113,114,115,116,117,118,…”
Section: Equation Of State Describing Gauge Field Theory Vacuum Fluct...mentioning
confidence: 99%
“…These scales lead to a much shorter universe live-time, but, importantly, to finite non-diverging time intervals 7 . In the case of Type II solution to be considered in the next section, when 0 ≤ γ 2 < γ 2 c and ã(0) ≥ µ 2 , the deceleration parameter q is negative and the scale factor grows exponentially with the inflation of a finite duration (97 ) that undergoes a continuous transition to a linear in time growth (99).…”
Section: Type I Solutionmentioning
confidence: 99%
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