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Curvature Perturbations and Primordial Black Holes

Examining how curvature perturbations influence the formation of primordial black holes.

― 6 min read


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In the universe's early stages, small irregularities in energy density could grow due to gravity, potentially leading to the formation of structures like galaxies and black holes. One interesting concept in this context is the curvature perturbation, which provides a way to describe how these irregularities develop.

Primordial Black Holes (PBHs) are one possible outcome of these density fluctuations. They form when regions of space become dense enough to collapse under their own gravity. Understanding how Curvature Perturbations influence PBH formation is crucial for deeper insights into the universe's evolution.

The Role of the Curvaton

One model used to explain the creation of curvature perturbations involves a field called the curvaton. The curvaton is a hypothetical light scalar field that exists during Inflation, the brief period of rapid expansion right after the Big Bang. This field contributes to density fluctuations by converting its energy density into curvature perturbations once inflation ends.

In our discussions, we focus on a specific scenario known as the non-minimal curvaton model. This scenario describes how the curvaton interacts with the inflaton, which is the primary field driving inflation. The interactions between these fields, particularly the effect of their associated potential energy, play a significant role in how perturbations grow.

Analyzing the Growth of Perturbations

The growth of curvature perturbations in this non-minimal curvaton scenario depends heavily on how parameters such as the field metrics are defined. A field metric can be thought of as a mathematical way to describe how the curvaton behaves in space and time.

Our examinations show that when certain conditions are met, curvaton perturbations can grow significantly. This behavior is particularly noticeable during a phase known as superhorizon growth, where perturbations evolve on scales larger than the observable universe.

The nature of the field metric is crucial. Depending on its shape and properties, it can either help or hinder the growth of perturbations. A specific kind of metric known as a Gaussian dip can lead to enhanced perturbations, meaning they become much larger than expected.

The Importance of Dip Shape

When studying curvature perturbations, the shape of the dip in the field metric matters. It is not only the depth or how low the dip goes that matters; the slope or steepness of the dip plays a significant role too. This means that different types of dips can result in varying outcomes for the growth of perturbations.

Through detailed analysis and calculations, we find that both the topography of the dip and its depth influence how the curvaton perturbations behave as inflation progresses. This leads us to conclude that focusing solely on the depth of these dips is an oversimplification when analyzing growth patterns.

Case Study: Gaussian Dip

To illustrate these findings, let’s consider a Gaussian-shaped dip in the field metric. A Gaussian dip means that the value of the metric changes with a distinct bell-shaped curve; it rises to a peak and then falls off smoothly.

In our numerical studies of this Gaussian dip, we observe significant increases in the power of curvature perturbations corresponding to the dip’s features. The characteristics of these perturbations provide insights into how they might lead to the formation of PBHs.

By running simulations, we can visualize how perturbations evolve during inflation and how eventually, when the universe transitions from inflation, the effects of the curvaton come into play. This Gaussian dip greatly impacts the final spectrum of curvature perturbations and the resulting PBH abundance.

Post-Inflation Dynamics and Non-Gaussianity

After inflation ends, the dynamics continue to evolve. The curvaton oscillates and begins to dominate over radiation, affecting how curvature perturbations behave. This phase is essential for determining the abundance of PBHs in the universe.

In our models, we adopt a simplified approach called the sudden-decay approximation, which assumes that when the curvaton decays, it does so rapidly and transfers its energy directly to radiation. Following this decay, we can analyze the nonlinear evolution of perturbations.

Non-Gaussianity arises in our studies, meaning the statistical properties of perturbations are not just standard fluctuations. These peculiar distributions can provide significant information about the formation and properties of PBHs.

Estimating PBH Formation

Once we have characterized curvature perturbations, we need to estimate how these fluctuations might lead to PBH formation. This involves understanding when and how regions of space become dense enough to collapse into black holes.

The conditions for PBH formation often relate to the size of density perturbations. A certain threshold must be exceeded for a region to undergo gravitational collapse. Our studies show that with the right parameters, particularly from the enhanced curvature perturbations, considerable portions of the universe could collapse into PBHs.

Recent findings suggest that certain mass ranges of PBHs might account for dark matter, which has implications for our understanding of the universe's composition.

Scalar-Induced Gravitational Waves

In addition to PBHs, the growth of perturbations can also lead to the production of gravitational waves (GWs). These GWs are ripples in spacetime created by various energetic processes in the universe, including the interactions between the scalar fields during inflation.

The relationship between curvature perturbations and gravitational waves is established through their second-order effects. When scalar perturbations grow, they may induce tensor modes corresponding to gravitational waves, creating another avenue for study.

Current and upcoming gravitational wave experiments aim to detect these signals. The implications of successfully observing such waves could drastically improve our understanding of early universe dynamics and promote further insights into PBH formation.

Conclusion

In summary, our exploration into the non-minimal curvaton scenario provides valuable insights into how curvature perturbations develop and their potential to form primordial black holes. The interactions between different fields and the specific properties of the curvaton reveal a complex picture, where growth patterns are influenced by both the depth and the shape of their metrics.

Further studies in this area, particularly focusing on Gaussian dips in field metrics and the subsequent dynamics, could uncover new relationships between early universe phenomena and current cosmic structures. With advancements in observational technologies, the quest to understand the universe's earliest moments and the role of black holes therein will continue to evolve.

This ongoing research holds the promise of unraveling more mysteries about the fabric of our universe, the nature of dark matter, and the framework of gravitational waves. Understanding these elements not only satisfies our curiosity about the cosmos but also enhances our grasp of fundamental physics.

Original Source

Title: Growth of curvature perturbations for PBH formation \& detectable GWs in non-minimal curvaton scenario revisited

Abstract: We revisit the growth of curvature perturbations in non-minimal curvaton scenario with a non-trivial field metric $\lambda(\phi)$ where $\phi$ is an inflaton field, and incorporate the effect from the non-uniform onset of curvaton's oscillation in terms of an axion-like potential. The field metric $\lambda(\phi)$ plays a central role in the enhancement of curvaton field perturbation $\delta\chi$, serving as an effective friction term which can be either positive or negative, depending on the first derivative $\lambda_{,\phi}$.Our analysis reveals that $\delta\chi$ undergoes the superhorizon growth when the condition $\eta_\text{eff} \equiv - 2 \sqrt{2\epsilon} M_\text{Pl} { \lambda_{,\phi} \over \lambda} < -3$ is satisfied. This is analogous to the mechanism responsible for the amplification of curvature perturbations in the context of ultra-slow-roll inflation, namely the growing modes dominate curvature perturbations. As a case study, we examine the impact of a Gaussian dip in $\lambda(\phi)$ and conduct a thorough investigation of both the analytical and numerical aspects of the inflationary dynamics.Our findings indicate that the enhancement of curvaton perturbations during inflation is not solely determined by the depth of the dip in $\lambda(\phi)$. Rather, the first derivative $\lambda_{,\phi}$ also plays a significant role, a feature that has not been previously highlighted in the literature. Utilizing the $\delta \mathcal{N}$ formalism, we derive analytical expressions for both the final curvature power spectrum and the non-linear parameter $f_\text{NL}$ in terms of an axion-like curvaton's potential leading to the non-uniform curvaton's oscillation. Additionally, the resulting primordial black hole abundance and scalar-induced gravitational waves are calculated, which provide observational windows for PBHs.

Authors: Chao Chen, Anish Ghoshal, Zygmunt Lalak, Yudong Luo, Abhishek Naskar

Last Update: 2023-08-14 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2305.12325

Source PDF: https://arxiv.org/pdf/2305.12325

Licence: https://creativecommons.org/licenses/by-sa/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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