论文标题

通过几何驱动的非规范再加热时代对原始引力波的扩增

Amplification of Primordial Gravitational Waves by a Geometrically Driven non-canonical Reheating Era

论文作者

Odintsov, S. D., Oikonomou, V. K.

论文摘要

为了描述一般相对论中的通货膨胀,必须不可避免地使用标量字段,并在该描述的所有挫折中使用。另一方面,$ f(r)$重力和其他修改的重力理论似乎提供了对早期和晚期动态的统一描述,而无需诉诸标量或幻影理论。问题是,修饰的重力能否直接影响神秘的辐射统治时代?解决这个问题是这项工作的重点,我们将考虑在辐射统治时代初期的情况,即在加热时代,状态参数的背景方程与$ W = 1/3 $不同。如我们所示,在$ f(r)$重力的背景下,异常的再加热时代可能会影响当今原始的引力波能谱。由于未来的干涉仪将精确探测这个时代,该时代由次摩恩模式组成,在辐射统治时代的早期阶段重新进入了地平线,因此这项工作的重点是如何以$ w \ neq 1/3 $产生的速度效果的范围偏离标准的完美流体模式的短期异常重新加热时代,会影响频率的范围。使用WKB方法,我们计算出$ f(r)$重力产生异常再加热时代的效果,并且当我们表明原始引力波谱得到显着扩增,这与一般相关病例相反,在效果较小的情况下。

In order to describe inflation in general relativity, scalar fields must inevitably be used, with all the setbacks of that description. On the other hand, $f(R)$ gravity and other modified gravity theories seem to provide a unified description of early and late-time dynamics without resorting to scalar or phantom theories. The question is, can modified gravity affect directly the mysterious radiation domination era? Addressing this question is the focus in this work, and we shall consider the case for which in the early stages of the radiation domination era, namely during the reheating era, the background equation of state parameter is different from $w=1/3$. As we show, in the context of $f(R)$ gravity, an abnormal reheating era can affect the primordial gravitational wave energy spectrum today. Since future interferometers will exactly probe this era, which consists of subhorizon modes that reentered the horizon during the early stages of the radiation domination era, the focus in this work is how a short abnormal reheating era that deviates from the standard perfect fluid pattern with $w\neq 1/3$, and generated by higher order curvature terms, can affect the primordial gravitational wave energy spectrum. Using a WKB approach, we calculate the effect of an $f(R)$ gravity generated abnormal reheating era, and as we show the primordial gravitational wave spectrum is significantly amplified, a result which is in contrast to the general relativistic case, where the effect is minor.

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