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首页> 外文期刊>Nuclear physics, B >Cosmological perturbations from multi-field inflation in generalized Einstein theories [Review]
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Cosmological perturbations from multi-field inflation in generalized Einstein theories [Review]

机译:广义爱因斯坦理论中多场通货膨胀引起的宇宙学扰动[综述]

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摘要

We study cosmological perturbations generated from quantum fluctuations in multi-field inflationary scenarios in generalized Einstein theories, taking both adiabatic and isocurvature modes into account. In the slow-roll approximation, explicit closed-form long-wave solutions for field and metric perturbations are obtained by the analysis in the Einstein frame. Since the evolution of fluctuations depends on specific gravity theories, we make detailed investigations based on analytic and numerical approaches in four generalized Einstein theories: the Jordan-Brans-Dicke (JBD) theory, the Einstein gravity with a non-minimally coupled scalar field, the higher-dimensional Kaluza-Klein theory, and the R + R-2 theory with a non-minimally coupled scalar field. We find that solutions obtained in the slow-roll approximation show good agreement with full numerical results except around the end of inflation. Due to the presence of isocurvature perturbations., the gravitational potential Phi and the curvature perturbation zeta do not remain constant on super-horizon scales. In particular, we find that negative non-minimal coupling can lead to strong enhancement of in both the Einstein and higher derivative gravity, in which case it is difficult to unambiguously decompose scalar perturbations into adiabatic and isocurvature modes during the whole stage of inflation. (C) 2001 Elsevier Science B.V. All rights reserved. [References: 106]
机译:我们在广义爱因斯坦理论中研究了在多场膨胀情景中由量子涨落产生的宇宙扰动,同时考虑了绝热和等曲率模式。在慢滚近似中,通过在爱因斯坦框架中进行分析,获得了针对场和度量扰动的显式闭合形式长波解。由于波动的演化取决于特定的引力理论,因此我们基于解析和数值方法对四种广义的爱因斯坦理论进行了详细的研究:约旦-布兰斯-迪克(JBD)理论,具有非最小耦合标量场的爱因斯坦引力,高维的Kaluza-Klein理论以及具有非最小耦合标量场的R + R-2理论。我们发现在慢滚动逼近中获得的解与通货膨胀结果结束之前的完整数值结果显示出良好的一致性。由于存在等曲率扰动,因此在超水平尺度上,重力势Phi和曲率扰动zeta不会保持恒定。特别是,我们发现负的非最小耦合会导致爱因斯坦强度的极大增强和较高的导数重力,在这种情况下,很难在整个充气阶段将标量摄动明确分解为绝热和等曲率模式。 (C)2001 Elsevier Science B.V.保留所有权利。 [参考:106]

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