Understanding the Scotogenic Model in Particle Physics
A look into the scotogenic model's implications for dark matter and neutrinos.
― 4 min read
Table of Contents
- The Scotogenic Model
- Basic Concepts
- The Role of Neutrinos
- Gauge Symmetry
- Parameter Space Exploration
- Collider Signatures
- Astrophysical Observations
- Dark Matter Candidate
- Neutrino Masses
- Experimental Constraints
- Stability Conditions
- Unitarity Constraints
- Theoretical Implications
- Conclusion
- Original Source
- Reference Links
Particle physics is the study that investigates the most basic building blocks of matter and the forces acting upon them. A recent topic of interest is dark matter (DM), an invisible substance that makes up a significant portion of the universe. Despite its prominence, its properties and origins remain largely unknown. This article delves into a new theoretical model that explores the nature of dark matter, the behavior of Neutrinos, and the implications for future research.
Scotogenic Model
TheThe scotogenic model introduces new particles and symmetries to explain the dark matter and neutrino mass problems. It suggests that the lightest particle in the model can act as a candidate for dark matter. This model incorporates a Gauge Symmetry that extends beyond the Standard Model (SM) of particle physics. The SM has been incredibly successful in explaining many phenomena, but it struggles with dark matter and neutrino masses.
Basic Concepts
Dark matter is known to exist due to its gravitational effects on visible matter, such as galaxies. However, it does not interact with electromagnetic radiation, making it invisible to telescopes. Neutrinos are another mystery, initially thought to be massless, but experiments have shown they have mass. The scotogenic model seeks to unify these ideas.
The Role of Neutrinos
Neutrinos are extremely light particles that come from nuclear reactions in the sun and other stars. They interact very weakly with regular matter, making them difficult to detect. The scotogenic model proposes a way to give neutrinos mass through a loop mechanism, where new particles contribute to the mass of the known neutrinos.
Gauge Symmetry
Gauge symmetry refers to the invariance of certain physical systems under specific transformations. The idea is that new particles can interact with known particles through new forces. In this model, new gauge bosons represent these interactions, helping connect dark matter with the particles that we are more familiar with.
Parameter Space Exploration
In this context, parameter space refers to the range of values for various physical quantities that allow the model to fit observational data. The scotogenic model predicts a region in parameter space where the density of dark matter is consistent with measurements from cosmology. This exploration helps identify which values might lead to observable signals in future experiments.
Collider Signatures
Particle colliders, like the Large Hadron Collider (LHC), can search for signs of new physics by smashing particles together at high energies. In the context of the scotogenic model, certain signals could point to the existence of the new particles predicted by the model.
Astrophysical Observations
Astrophysical data, such as the cosmic microwave background and galaxy rotation curves, support the idea of dark matter. These observations provide crucial information for testing the scotogenic model and determining whether it accurately describes reality.
Dark Matter Candidate
In the scotogenic model, one possibility for dark matter is a light scalar particle. This particle interacts with the Standard Model particles through a new force, mediated by the additional gauge bosons. Understanding how this particle behaves will be key to verifying the model's predictions.
Neutrino Masses
The masses of neutrinos pose a challenge to the Standard Model, which originally assumed they were massless. The scotogenic model offers a solution by introducing new interactions that allow neutrinos to acquire mass through loop diagrams. This aspect may have implications for understanding the universe's evolution and the matter-antimatter asymmetry.
Experimental Constraints
While the scotogenic model provides a framework for understanding dark matter and neutrino masses, it also faces constraints from experiments. Results from particle colliders, electroweak precision tests, and direct searches for dark matter help narrow down the range of possible parameters.
Stability Conditions
It is essential for the model's potential energy to remain stable under various conditions. This stability ensures that the particles involved do not lead to unphysical behavior, such as producing negative energy. Stability conditions are rigorously analyzed in the model to ensure its viability.
Unitarity Constraints
Unitarity refers to the principle that probabilities must sum to one in quantum mechanics. For the scotogenic model, this means that the possible outcomes of particle interactions must be consistent with observable probabilities. Violations of unitarity could indicate that the model is incorrect.
Theoretical Implications
The new model sheds light on the relationship between dark matter, neutrinos, and the forces that govern their interactions. Future research will likely focus on refining the model and exploring any direct evidence that may arise from experiments.
Conclusion
The scotogenic model offers a promising avenue for exploring the mysteries of dark matter and neutrinos in particle physics. By introducing new particles and symmetries, it seeks to address some fundamental questions about the universe's structure and contents. As experimental techniques improve, the hopes of confirming or disproving this model will advance, enabling a deeper understanding of the invisible aspects of our universe.
Title: A Scotogenic model with U(1) symmetry and a scalar dark matter
Abstract: We study a scotogenic model augmented with an additional U(1) gauge and a discrete Z2 symmetry. The lightest Z2-odd particle in our model becomes the dark matter (DM) candidate while tiny neutrino masses are realized at one loop. We explore the parameter space of the model for which the DM relic density is satisfied, and the correct low-energy neutrino observables are reproduced. The extended gauge symmetry includes beyond Standard Model (SM) particle spectrum consisting of vector-like fermions and scalars. We also highlight possible collider signatures of these particles at the LHC.
Authors: Anjan Kumar Barik, Najimuddin Khan, Santosh Kumar Rai
Last Update: 2024-06-24 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2406.16546
Source PDF: https://arxiv.org/pdf/2406.16546
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.
Reference Links
- https://orcid.org/
- https://arxiv.org/abs/#1
- https://dx.doi.org/
- https://arxiv.org/abs/1207.7214
- https://arxiv.org/abs/1207.7235
- https://arxiv.org/abs/astro-ph/0608407
- https://arxiv.org/abs/nucl-ex/0204008
- https://arxiv.org/abs/hep-ex/9807003
- https://arxiv.org/abs/0801.1345
- https://arxiv.org/abs/hep-ph/9805494
- https://arxiv.org/abs/hep-ph/0610104
- https://arxiv.org/abs/hep-ph/0611205
- https://arxiv.org/abs/1707.02424
- https://arxiv.org/abs/1912.04776
- https://arxiv.org/abs/hep-ph/0601225
- https://arxiv.org/abs/hep-ph/9507455
- https://arxiv.org/abs/hep-ph/0601097
- https://arxiv.org/abs/1311.5666
- https://arxiv.org/abs/1407.3792
- https://arxiv.org/abs/1201.2644
- https://arxiv.org/abs/hep-ph/0603188
- https://arxiv.org/abs/1207.4235
- https://arxiv.org/abs/1803.01853
- https://arxiv.org/abs/1906.07821
- https://arxiv.org/abs/2205.12641
- https://arxiv.org/abs/2201.11585
- https://arxiv.org/abs/2207.00348
- https://arxiv.org/abs/hep-ph/0503173
- https://arxiv.org/abs/1801.04688
- https://arxiv.org/abs/0908.2381
- https://arxiv.org/abs/2308.06230
- https://arxiv.org/abs/hep-ex/0602035
- https://arxiv.org/abs/2104.03281
- https://arxiv.org/abs/2311.08282
- https://arxiv.org/abs/2006.04822
- https://arxiv.org/abs/1403.6400
- https://arxiv.org/abs/1908.00921
- https://arxiv.org/abs/1706.09436
- https://arxiv.org/abs/1802.02995
- https://arxiv.org/abs/1810.00007
- https://arxiv.org/abs/1907.01556
- https://arxiv.org/abs/1911.00367
- https://arxiv.org/abs/1911.08123
- https://arxiv.org/abs/2002.12347
- https://arxiv.org/abs/2206.06582
- https://arxiv.org/abs/2206.15084
- https://arxiv.org/abs/2211.15581
- https://arxiv.org/abs/2302.08834
- https://arxiv.org/abs/2007.14792
- https://arxiv.org/abs/2111.03086
- https://arxiv.org/abs/1807.06209
- https://arxiv.org/abs/1805.12562
- https://arxiv.org/abs/2207.03764
- https://arxiv.org/abs/1602.06563
- https://arxiv.org/abs/1310.1921
- https://arxiv.org/abs/1801.03509
- https://arxiv.org/abs/1309.7223
- https://arxiv.org/abs/1503.04200
- https://arxiv.org/abs/1104.1573
- https://arxiv.org/abs/0911.1120
- https://arxiv.org/abs/1705.01987
- https://arxiv.org/abs/1503.03085
- https://arxiv.org/abs/1407.6015
- https://arxiv.org/abs/0803.2799
- https://arxiv.org/abs/1708.00328
- https://arxiv.org/abs/1006.5019
- https://arxiv.org/abs/2106.01362
- https://arxiv.org/abs/2109.07980