2004
DOI: 10.1103/physrevd.70.044017
|View full text |Cite
|
Sign up to set email alerts
|

Particle production in matrix cosmology

Abstract: We consider cosmological particle production in 1ϩ1 dimensional string theory. The process is described most efficiently in terms of anomalies, but we also discuss the explicit mode expansions. In matrix cosmology the usual vacuum ambiguity of quantum fields in time-dependent backgrounds is resolved by the underlying matrix model. This leads to a finite energy density for the ''in'' state which cancels the effect of anomalous particle production.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
74
1

Year Published

2004
2004
2024
2024

Publication Types

Select...
5
2

Relationship

1
6

Authors

Journals

citations
Cited by 42 publications
(77 citation statements)
references
References 47 publications
2
74
1
Order By: Relevance
“…Supposedly such a complication would appear for the droplet cosmologies as well, but there is no obvious candidate for what it might be. Therefore, it seems unlikely that a spacetime analysis of tachyon scattering can be carried out as has been done in the case of the standard, static Fermi sea as well as the moving hyperbola solution (3.7) [9,10]. In addition, the leg pole transform is only known on the null boundaries of spacetime, and not in its bulk.…”
Section: Jhep09(2004)065mentioning
confidence: 99%
See 1 more Smart Citation
“…Supposedly such a complication would appear for the droplet cosmologies as well, but there is no obvious candidate for what it might be. Therefore, it seems unlikely that a spacetime analysis of tachyon scattering can be carried out as has been done in the case of the standard, static Fermi sea as well as the moving hyperbola solution (3.7) [9,10]. In addition, the leg pole transform is only known on the null boundaries of spacetime, and not in its bulk.…”
Section: Jhep09(2004)065mentioning
confidence: 99%
“…We also have ∂ x σ = √ g/f . Now we can use the equation of motion (2.7) to find the forms of f and g. Using (4.4), notice that 10) so the equation of motion (2.7) implies…”
Section: Jhep09(2004)065mentioning
confidence: 99%
“…From the general formulae in [10] (equation (36)) it follows that the fluctuations are massless particles in a metric which is conformally equivalent to In this metric, t = 0 is a coordinate singularity. The transformations (13) and (17) render the metric Minkowskian…”
Section: The Opening Hyperbola Solutionmentioning
confidence: 99%
“…The static Fermi sea is, of course, not the only solution of the equations of motion. A class of nontrivial solutions can be obtained by acting with various W ∞ transformations on this static profile [10]. In phase space, one class of transformations is given by…”
Section: Moving Fermi Sea Solutionsmentioning
confidence: 99%
See 1 more Smart Citation