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arXiv 1609.06191hep-thastro-ph.COgr-qc
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曲率存在于哪里?体框架与膜框架的区别

Where does curvaton reside? Differences between bulk and brane frames

François Larrouturou, Shinji Mukohyama, Ryo Namba, Yota Watanabe

摘要:

某些类的暴胀模型自然引入了两个不同的度量/框架,它们在可观测量方面的等价性经常受到质疑。D-膜暴胀提出了嵌入弦论的暴胀子的候选者,并拥有对膜和体度量/框架的描述,它们通过依赖于暴胀子及其导数的共形/非形式变换连接。已经证明,暴胀子产生的曲率扰动在两个框架中是相同的,这意味着诸如宇宙微波背景(CMB)各向异性的光谱等可观测量与物质场(包括粒子物理学的标准模型中的物质场)是否最低限度地耦合到膜或体度规/框架无关。尽管可观测量最终是由物质场来测量的,而且包括物质场在内的总作用量在两种情况下是不同的,但这是正确的。相反,在曲率场景中,可观测量取决于曲率最小耦合的框架。在所有的通货膨胀的情况下,我们专注于两个模型的动机KKLMMT微调问题:一个缓慢滚动的通货膨胀与拐点潜力和一个模型的快速滚动的暴胀,共形耦合到重力。在第一个模型中,曲率所在的帧之间的差异被编码在曲率扰动的谱指数中,描述了帧变换的性质。在第二个模型中,膜上的曲率导致了与体相显著不同的光谱指数,甚至被观测所证伪。因此,这项工作表明,由共形/非形式变换连接的两个框架导致不同的物理观测量,如曲率模型中的CMB各向异性。

英文摘要:

Some classes of inflationary models naturally introduce two distinct metrics/frames, and their equivalence in terms of observables has often been put in question. D-brane inflation proposes candidates for an inflaton embedded in the string theory and possesses descriptions on the brane and bulk metrics/frames, which are connected by a conformal/disformal transformation that depends on the inflaton and its derivatives. It has been shown that curvature perturbations generated by the inflaton are identical in both frames, meaning that observables such as the spectrum of cosmic microwave background (CMB) anisotropies are independent of whether matter fields---including those in the standard model of particle physics---minimally couple to the brane or the bulk metric/frame. This is true despite the fact that the observables are eventually measured by the matter fields and that the total action including the matter fields is different in the two cases. In contrast, in curvaton scenarios, the observables depend on the frame to which the curvaton minimally couples. Among all inflationary scenarios, we focus on two models motivated by the KKLMMT fine-tuning problem: a slow-roll inflation with an inflection-point potential and a model of a rapidly rolling inflaton that conformally couples to gravity. In the first model, the difference between the frames in which the curvaton resides is encoded in the spectral index of the curvature perturbations, depicting the nature of the frame transformation. In the second model, the curvaton on the brane induces a spectral index significantly different from that in the bulk and is even falsified by the observations. This work thus demonstrates that two frames connected by a conformal/disformal transformation lead to different physical observables such as CMB anisotropies in curvaton models.

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