The Impact of a Light Boson on Cosmic Observations
Examining how a light boson influences the early universe and cosmic microwave background.
― 6 min read
Table of Contents
- The Role of the Boson
- Understanding the Mass Range
- Energy Redistribution
- Future Observations
- Gauged Symmetry and Neutrino Types
- Neutrino Decay Implications
- Experimental Constraints
- Calculating Effective Particle Numbers
- Boltzmann Equations and Their Solutions
- Analyzing Particle Interaction Rates
- Thermal Equilibrium Considerations
- Mass Regimes of the Boson
- Predictions from CMB Observations
- Connecting to Big Bang Nucleosynthesis
- Implications of Right-Handed Neutrinos
- Predictions and Future Studies
- Summary of Findings
- Future Directions
- Original Source
- Reference Links
In the study of the universe, scientists often investigate how new particles affect what we observe. One area of focus is a light boson, a type of particle that may interact very weakly with other known particles. This paper explores how such a boson could change our understanding of the cosmic microwave background (CMB) and the formation of elements shortly after the Big Bang, known as Big Bang Nucleosynthesis (BBN).
The Role of the Boson
The boson considered here arises from a symmetry that has been broken. When this boson is present, it can affect measurements from the CMB and influence the early universe's conditions. The effects we are interested in depend on the mass of the boson. Lighter Bosons are heavily constrained by existing theories, while heavier bosons are still analyzed in various probes.
Understanding the Mass Range
We categorize the mass of the boson into different ranges. Bosons with masses below a certain threshold are tightly constrained by what we call "fifth force" laws. In contrast, bosons with heavier masses are constrained by experiments conducted on Earth and through cosmic observations. We also explore the idea that the boson did not start in an energy state of thermal equilibrium but rather gained its presence through weak interactions.
Energy Redistribution
As the universe evolves, the energy density in the universe can change, impacting the behavior of particles. In our scenario, electrons and Neutrinos slowly give way to bosons as they become non-relativistic. Over time, these bosons decay and release energy back into the standard model particles, thereby affecting the overall energy density of the universe.
Future Observations
To understand these effects, future CMB observations from facilities like the Simons Observatory and CMB-S4 will be crucial. These upcoming studies aim to provide insights into areas of mass and coupling properties that have not been thoroughly explored before.
Gauged Symmetry and Neutrino Types
To gauge the effects of the boson precisely, we need to consider how anomalies, which complicate calculations, are canceled out. We consider two scenarios for neutrinos: one where they have Dirac masses and another where they have Majorana masses. These variations can significantly influence the implications of the boson’s behavior during the early universe, particularly during the BBN period.
Neutrino Decay Implications
Neutrinos that achieve thermal equilibrium can contribute to the energy density observed in the universe. When right-handed neutrinos decay, they can release energy back into left-handed neutrinos and other particles, potentially affecting the amount of helium produced during BBN. This connection between neutrino dynamics and the amount of helium is vital for understanding the early cosmos.
Experimental Constraints
Various experiments have been devised to understand the interactions of these light bosons with known particles. These include stellar cooling processes and the emissions from supernovae, which can offer alternative pathways to constrain the boson’s properties. By analyzing the energy loss from these cosmic events, we can detect signs of the boson’s presence and effects.
Calculating Effective Particle Numbers
One of the key measurements in cosmology is the effective number of relativistic species in the universe. This measure relates to the energy density beyond just standard model particles like photons and neutrinos. If new physics from a boson adds to this energy density, it changes how we calculate the effective number of species present during the CMB formation.
Boltzmann Equations and Their Solutions
To derive the effects of all these interactions, we use a series of equations that represent how particles evolve. These Boltzmann equations take into account the interactions between various particle species as the universe expands. We can adjust these equations to understand how the inclusion of our new light boson influences the cosmic landscape.
Analyzing Particle Interaction Rates
Understanding how different particles interact is critical. In our model, the interactions between electrons and neutrinos are governed by weak forces. When introducing the boson, we also have to look at how it interacts with these particles, as these rates significantly impact the overall evolution of the energy density in the universe.
Thermal Equilibrium Considerations
The dynamics of particles depend heavily on their ability to reach thermal equilibrium. In scenarios where the boson remains out of equilibrium, we expect some interesting phenomena regarding how energy and particle densities evolve. The presence of a chemical potential, which indicates a non-zero distribution of particles, tells us how particles feed off each other in the thermal landscape.
Mass Regimes of the Boson
As we consider the properties of our light boson, we categorize its effects based on various mass regimes: heavy, intermediate, and light. Each mass range presents unique challenges and characteristics in terms of interactions and the resulting impact on the universe's expansion and composition.
Predictions from CMB Observations
The CMB serves as a crucial tool for probing the early universe. By analyzing its power spectra and primordial abundance of elements, we can gauge how much our light boson may contribute to the relativistic species present. Understanding these contributions is vital for testing theories beyond the standard model of particle physics.
Connecting to Big Bang Nucleosynthesis
During BBN, the interactions of particles determine the types of elements formed, notably helium. If new physics interferes with the established reactions, we may observe deviations in observed abundances relative to theoretical predictions, which can be traced back to the influence of our light boson.
Implications of Right-Handed Neutrinos
When considering right-handed neutrinos, their behavior affects the overall dynamics of the boson interactions. If these neutrinos gain mass, they may contribute to Energy Densities actively, leading to alterations in expected outcomes in both CMB and BBN contexts.
Predictions and Future Studies
As we outline predictions for how our light boson affects cosmological parameters, we also highlight the potential for future studies to clarify these relationships. Upcoming observations aiming to measure changes in the effective number of relativistic species will be important for checking our theoretical models.
Summary of Findings
In conclusion, our work sheds light on how a weakly interacting light boson could reshape our understanding of early universe cosmology. The effects on the CMB and BBN offer a pathway to testing new physics, significantly impacting our current understanding of particle interactions and cosmic development.
Future Directions
To better understand these dynamics, scientists will need to conduct more observational studies and refine their models. The interplay between the new boson and existing particles opens up an exciting area of research that could provide profound insights into the composition and evolution of the universe we inhabit.
Title: Cosmological Implications of Gauged $U(1)_{B-L}$ on $\Delta N_{\rm eff}$ in the CMB and BBN
Abstract: We calculate the effects of a light, very weakly-coupled boson $X$ arising from a spontaneously broken $U(1)_{B-L}$ symmetry on $\Delta N_{\rm eff}$ as measured by the CMB and $Y_p$ from BBN. Our focus is the mass range $1 \; {\rm eV} \lesssim m_X \lesssim 100 \; {\rm MeV}$; masses lighter than about an ${\rm eV}$ have strong constraints from fifth-force law constraints, while masses heavier than about 100 MeV are constrained by other probes. We do not assume $X$ began in thermal equilibrium with the SM; instead, we allow $X$ to freeze-in from its very weak interactions with the SM. We find $U(1)_{B-L}$ is more strongly constrained by $\Delta N_{\rm eff}$ than previously considered. The bounds arise from the energy density in electrons and neutrinos slowly siphoned off into $X$ bosons, which become nonrelativistic, redshift as matter, and then decay, dumping their slightly larger energy density back into the SM bath causing $\Delta N_{\rm eff} > 0$. While some of the parameter space has complementary constraints from stellar cooling, supernova emission, and terrestrial experiments, we find future CMB observatories can access regions of mass and coupling space not probed by any other method. In gauging $U(1)_{B-L}$, we assume the $[U(1)_{B-L}]^3$ anomaly is canceled by right-handed neutrinos, and so our $\Delta N_{\rm eff}$ calculations have been carried out in two scenarios: neutrinos have Dirac masses, or, right-handed neutrinos acquire Majorana masses. In the latter scenario, we comment on the additional implications of thermalized right-handed neutrinos decaying during BBN. We also briefly consider the possibility that $X$ decays into dark sector states. If these states behave as radiation, we find weaker constraints, whereas if they are massive, there are stronger constraints, though now from $\Delta N_{\rm eff} < 0$.
Authors: Haidar Esseili, Graham D. Kribs
Last Update: 2024-04-29 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2308.07955
Source PDF: https://arxiv.org/pdf/2308.07955
Licence: https://creativecommons.org/licenses/by/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.