论文标题
高谐波环的尖端特性
The cusp properties of High Harmonic Loops
论文作者
论文摘要
在确定来自宇宙字符串循环网络的尖牙的重力信号时,必须假定许多关键参数。其中包括每个弦振荡周期的典型尖数以及在cusp事件中评估的左右移动波的夏形参数的典型值。这两者都很重要,因为从字符串环发出的重力波中存储的功率与每个周期的尖数数成正比,并且与与字符串上的左右移动模式相关的清晰度参数的乘积成反比。在合适的单位中,这两个数量通常都被认为是秩序的统一。为了尝试将这些参数放置在更强大的基础上,我们详细分析了大量随机选择的弦乐循环,这些弦可以与它们相关联,例如人们可能希望通过在早期宇宙中砍掉无限字符串来形成。这使我们能够分析数万个循环,并获得有关这些关键参数的详细统计数据。虽然我们通常发现清晰度参数确实接近统一,如先前的工作(偶尔有例外,它们都可以变成$ o(10^{ - 2})$),但每期量表的尖数与环上的谐波数量直接在环上,并且可以明显大于Unity。这打开了比原本预期的更大信号的可能性,这可能会导致无量纲宇宙弦张力$gμ$上的更紧密的界限。
In determining the gravitational signal of cusps from a network of cosmic strings loops, a number of key parameters have to be assumed. These include the typical number of cusps per period of string oscillation and the typical values of the sharpness parameters of left and right moving waves on the string, evaluated at the cusp event. Both of these are important, as the power stored in the gravitational waves emitted from the loops of string is proportional to the number of cusps per period, and inversely proportional to the product of the sharpness parameters associated with the left and right moving modes on the string. In suitable units both of these quantities are usually thought to be of order unity. In order to try and place these parameters on a more robust footing, we analyse in detail a large number of randomly chosen loops of string that can have high harmonics associated with them, such as one might expect to form by chopping off an infinite string in the early universe. This allows us to analyse tens of thousands of loops and obtain detailed statistics on these crucial parameters. While we find in general the sharpness parameters are indeed close to unity, as assumed in previous work (with occasional exceptions where they can become $O(10^{-2})$), the cusp number per period scales directly with the number of harmonics on the loop and can be significantly larger than unity. This opens up the possibility of larger signals than would have otherwise been expected, potentially leading to tighter bounds on the dimensionless cosmic string tension $Gμ$.