早期宇宙中的张量涨落

IF 4.2 3区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS
F. Melia
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引用次数: 1

摘要

在标准的暴胀宇宙学中,标量和张量扰动随着宇宙的膨胀而增长,当它们的波长超过哈勃视界时就会冻结,在宇宙微波背景(CMB)的波动光谱和振幅中产生一个明显的特征。但现在有很好的理由来研究结构的形成是否也可以通过在非暴胀领域中播种量子涨落而开始。在本文中,我们研究并比较了在这两种情况下产生的标量模和张量模,并证明了即将进行的测量CMB b模偏振的观测可能能够区分它们。如果场是暴胀的,那么标量模式和张量模式都应该是可见的,如果不是暴胀的,那么在CMB中只有标量模式会出现。然而,如果引力是纯经典的,那么张量模就会在所有情况下避免正则量子化,从而导致无法测量的弱引力波。因此,如果没有探测到b模极化,就不能完全排除暴胀的可能。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Tensor fluctuations in the early universe

In standard inflationary cosmology, scalar and tensor perturbations grew as the Universe expanded and froze when their wavelengths exceeded the Hubble horizon, producing a tell-tale signature in the fluctuation spectrum and amplitude of the cosmic microwave background (CMB). But there are now very good reasons to examine whether structure formation could also have begun via the seeding of quantum fluctuations in a non-inflationary field. In this Letter, we study and compare the scalar and tensor modes produced in these two scenarios, and demonstrate that upcoming observations to measure the B-mode polarization of the CMB may be able to differentiate between them. Whereas both scalar and tensor modes should be observable if the field was inflationary, only scalar modes would be present in the CMB if it were not. Should gravity be purely classical, however, the tensor modes would have avoided canonical quantization in all cases, resulting in unmeasurably weak gravitational waves. A non-detection of B-mode polarization would thus not completely rule out inflation.

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来源期刊
Astroparticle Physics
Astroparticle Physics 地学天文-天文与天体物理
CiteScore
8.00
自引率
2.90%
发文量
41
审稿时长
79 days
期刊介绍: Astroparticle Physics publishes experimental and theoretical research papers in the interacting fields of Cosmic Ray Physics, Astronomy and Astrophysics, Cosmology and Particle Physics focusing on new developments in the following areas: High-energy cosmic-ray physics and astrophysics; Particle cosmology; Particle astrophysics; Related astrophysics: supernova, AGN, cosmic abundances, dark matter etc.; Gravitational waves; High-energy, VHE and UHE gamma-ray astronomy; High- and low-energy neutrino astronomy; Instrumentation and detector developments related to the above-mentioned fields.
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