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Low energy effective string cosmology
High Energy Physics - Theory · Submitted 30 Jun 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In the case of $H$ field radiation (wavelengths within the Hubble length) we obtain the usual four dimensional radiation dominated FRW model as the unique late time attractor.
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The abstract, sentence by sentence
We give the general analytic solutions derived from the low energy string effective action for four dimensional Friedmann-Robertson-Walker models with dilaton and antisymmetric tensor field, considering both long and short wavelength modes of the $H$-field. The presence of a homogeneous $H$-field significantly modifies the evolution of the scale factor and dilaton. In particular it places a lower bound on the allowed value of the dilaton. The scale factor also has a lower bound but our solutions remain singular as they all contain regions where the spacetime curvature diverges signalling a breakdown in the validity of the effective action. We extend our results to the simplest Bianchi I metric in higher dimensions with only two scale factors. We again give the general analytic solutions for long and short wavelength modes for the $H$ field restricted to the three dimensional space, which produces an anisotropic expansion. In the case of $H$ field radiation (wavelengths within the Hubble length) we obtain the usual four dimensional radiation dominated FRW model as the unique late time attractor.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We give the general analytic solutions derived from the low energy string effective action for four dimensional Friedmann-Robertson-Walker models with dilaton and antisymmetric tensor field, considering both long and short wavelength modes of the $H$-field. | contribution 0.98 | 0.95 | 0.15 | asserted 1.00 |
| s1 | The presence of a homogeneous $H$-field significantly modifies the evolution of the scale factor and dilaton. | result 0.96 | 0.85 | 0.24 | asserted 1.00 |
| s2 | In particular it places a lower bound on the allowed value of the dilaton. | result 0.98 | 0.88 | 0.20 | asserted 1.00 |
| s3 | The scale factor also has a lower bound but our solutions remain singular as they all contain regions where the spacetime curvature diverges signalling a breakdown in the validity of the effective action. | limitation 0.82 | 0.93 | 0.23 | asserted 1.00 |
| s4 | We extend our results to the simplest Bianchi I metric in higher dimensions with only two scale factors. | contribution 0.99 | 0.94 | 0.05 | asserted 0.98 |
| s5 | We again give the general analytic solutions for long and short wavelength modes for the $H$ field restricted to the three dimensional space, which produces an anisotropic expansion. | contribution 0.98 | 0.96 | 0.08 | asserted 1.00 |
| s6 | In the case of $H$ field radiation (wavelengths within the Hubble length) we obtain the usual four dimensional radiation dominated FRW model as the unique late time attractor. | result 0.99 | 0.92 | 0.24 | asserted 1.00 |
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The paper
Original abstract
We give the general analytic solutions derived from the low energy string effective action for four dimensional Friedmann-Robertson-Walker models with dilaton and antisymmetric tensor field, considering both long and short wavelength modes of the $H$-field. The presence of a homogeneous $H$-field significantly modifies the evolution of the scale factor and dilaton. In particular it places a lower bound on the allowed value of the dilaton. The scale factor also has a lower bound but our solutions remain singular as they all contain regions where the spacetime curvature diverges signalling a breakdown in the validity of the effective action. We extend our results to the simplest Bianchi I metric in higher dimensions with only two scale factors. We again give the general analytic solutions for long and short wavelength modes for the $H$ field restricted to the three dimensional space, which produces an anisotropic expansion. In the case of $H$ field radiation (wavelengths within the Hubble length) we obtain the usual four dimensional radiation dominated FRW model as the unique late time attractor.
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References
How the literature uses it
8 arXiv papers cite this in 13 sentences
Papers citing it · 3 sentences without a confident label
Builds on it 1 paper
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An extension of the work in [ref] , involving the antisymmetric tensor was made in [ref] and is based on a similar non-perturbative conformal invariance, which is different from the traditional approach [ref] .
Non-perturbative time-dependent String Backgrounds and Axion-induced Optical Activity · Introduction · 0.96
Cites it as support 2 papers
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This may be a good approximation at early times if compared with the $Λ$ the curvature and/or kinetic energy are large, $Λ≪R, (∇ϕ)^2, H^2$ [ref] .
Anisotropic homogeneous string cosmology with two-loop corrections · Two-loop (order $α'$) $β$-functions and $α'$-corrected string effective action · 0.99
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This may be a good approximation if the curvature and/or kinetic energy are large compared to the $Λ$, i.e. $Λ≪R, ∇ϕ, H^2$ [ref] .
New five-dimensional Bianchi type magnetically charged hairy topological black hole solutions in string theory · Low energy string effective action and one-loop Lg-functions · 0.97
Cites it as background 6 papers
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The antisymmetric tensor usually implies an anisotropic metric [ref] , but it is also possible to consider an isotropic metric, either with an axion depending on time only [ref] , or with a plane wave axion, after a space-averaging of the energy momentum tensor corresponding to $H_ρμν$ [ref] .
Antisymmetric-Tensor and Electromagnetic effects in an alpha'-non-perturbative Four-Dimensional String Cosmology · Introduction · 0.82
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Namely the LQG is the background independent quantisation of the Hilbert-Einstein action [equation] On the other side, ST of the closed strings leads to the gravitational action in the form [ref] [equation] where $H^2=H_μναH^μνα$ and $H_μνα=3! ∂_ [ μ B_να]$.
Universe from vacuum in loop-string cosmology · Introduction · 0.84
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(with $H_ABC=_[AB_BC]$), which describes a 3-brane embedded in a 5-dimensional bulk with dilaton and Kalb-Ramond 2-form [ref] .
Bouncing cosmology from Kalb-Ramond Braneworld · The 5-D solution · 0.81
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