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CP Violation and Flavor Violation in the Randall-Sundrum Model: Exploring Di-Higgs Couplings and Lepton Flavor-Violating Decays


แนวคิดหลัก
The Randall-Sundrum (RS) model offers a compelling framework to address the hierarchy problem and introduces new sources of CP violation and flavor violation. This paper explores the phenomenological implications of flavor-violating di-Higgs couplings in the RS model, particularly their contributions to lepton flavor-violating decays and their potential for discovery at future colliders.
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Bibliographic Information:

Ghosh, G. (2024, November 10). CP Violation and Flavour-Violating Di-Higgs Couplings in the Randall-Sundrum Model. arXiv. https://arxiv.org/abs/2411.06451v1

Research Objective:

This research paper investigates the role of CP violation and flavor-violating di-Higgs couplings within the framework of the Randall-Sundrum (RS) model. The study aims to explore the phenomenological implications of these couplings, particularly their contributions to lepton flavor-violating decays and their potential for discovery at future colliders.

Methodology:

The authors employ a combination of theoretical calculations and Monte Carlo simulations to explore the parameter space of the RS model. They derive expressions for flavor-violating di-Higgs couplings and calculate their contributions to various lepton flavor-violating decays. Monte Carlo simulations are used to generate distributions of these couplings while considering experimental constraints on branching ratios for processes like τ → 3µ, τ → µγ, µ → eγ, and µ → 3e.

Key Findings:

  • The RS model predicts enhanced flavor-violating couplings, leading to potentially observable effects in lepton flavor-violating decays.
  • The allowed parameter space for flavor-violating couplings is constrained by experimental limits on branching ratios of LFV decays.
  • The study identifies specific ranges for couplings like Cµτ, Cµµ, Cτe, and Cee that satisfy current experimental bounds.
  • Future experiments with increased sensitivity to LFV decays could further constrain the RS model parameter space or potentially reveal deviations from Standard Model predictions.

Main Conclusions:

The RS model offers a viable framework for explaining both the hierarchy problem and the origin of CP violation and flavor violation. The study demonstrates that flavor-violating di-Higgs couplings in the RS model can lead to observable effects in LFV decays, providing a potential avenue for testing the model at future colliders.

Significance:

This research contributes to the ongoing search for physics beyond the Standard Model by exploring the phenomenological implications of the RS model. The findings provide valuable insights into the interplay between flavor physics, CP violation, and extra-dimensional theories, guiding future experimental searches for new physics.

Limitations and Future Research:

The study primarily focuses on lepton flavor-violating decays. Further research could explore the implications of flavor-violating di-Higgs couplings for quark flavor physics and CP violation in other sectors. Additionally, investigating the impact of higher-order corrections and exploring alternative extra-dimensional models could provide a more comprehensive understanding of flavor violation and CP violation beyond the Standard Model.

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BR(τ →3µ) < 1.2 × 10^-8 BR(τ →µγ) < 4.4 × 10^-8 BR(µ →eγ) ≤ 4.2 × 10^-13 BR(µ →3e) ≤ 1.0 × 10^-12 BR(τ →µe+e−) < 1.2 × 10^-8
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ข้อมูลเชิงลึกที่สำคัญจาก

by Gayatri Ghos... ที่ arxiv.org 11-12-2024

https://arxiv.org/pdf/2411.06451.pdf
CP Violation and Flavour-Violating Di-Higgs Couplings in the Randall-Sundrum Model

สอบถามเพิ่มเติม

How might future collider experiments be optimized to specifically target the detection of flavor-violating di-Higgs couplings and other unique signatures predicted by the RS model?

Answer: Future collider experiments can be optimized to target flavor-violating di-Higgs couplings and other RS model signatures through a multi-pronged approach focusing on increased energy, luminosity, and detector capabilities: 1. Higher Energy Reach: Motivation: The RS model predicts new particles, such as Kaluza-Klein (KK) excitations of gravitons and gauge bosons, with masses at the TeV scale. Higher energy collisions are crucial to produce these heavy particles on-shell, allowing for direct searches and measurements of their properties. Implementation: Future colliders, like the proposed Future Circular Collider (FCC) or a 100 TeV hadron collider, would significantly extend the energy reach compared to the LHC, enabling the exploration of higher mass ranges where RS signatures are more likely to manifest. 2. Increased Luminosity: Motivation: Flavor-violating di-Higgs couplings are expected to be rare processes with small cross-sections. Higher luminosity, meaning a larger number of collisions per unit time, is essential to accumulate sufficient statistics for these rare events, improving the signal-to-background ratio. Implementation: Future colliders are designed with significantly higher luminosity targets. For example, the High-Luminosity LHC (HL-LHC) aims for a tenfold increase in integrated luminosity, while future machines like the FCC propose even higher luminosities, enhancing the discovery potential for rare processes. 3. Enhanced Detector Capabilities: Motivation: Precise reconstruction and identification of particles are crucial to distinguish RS model signals from background events. Improved detector technologies are needed to handle the higher particle multiplicities and energies expected at future colliders. Implementation: Future detectors will incorporate advancements in tracking, calorimetry, and muon systems. For instance, highly granular calorimeters can improve jet energy resolution, while advanced tracking systems can better reconstruct particle trajectories, enhancing the ability to identify and measure flavor-violating decays. 4. Targeted Analysis Strategies: Motivation: Developing dedicated analysis strategies optimized for RS model signatures is crucial. This includes identifying specific decay channels, kinematic cuts, and multivariate techniques to effectively separate signal events from background. Implementation: Monte Carlo simulations play a vital role in developing and optimizing these analysis strategies. By simulating RS model processes and comparing them to expected backgrounds, physicists can design cuts and selection criteria to maximize the sensitivity to flavor-violating di-Higgs couplings and other RS signatures. 5. Flavor Tagging: Motivation: Efficiently identifying the flavors of final-state particles is crucial for studying flavor-violating processes. This is particularly important for distinguishing between different types of di-Higgs decays, such as those involving taus, muons, or bottom quarks. Implementation: Improved flavor tagging algorithms, which use information from tracking, vertexing, and particle identification systems, can significantly enhance the ability to identify the flavors of jets originating from heavy quarks or leptons. By combining these advancements in collider technology and analysis techniques, future experiments will be well-positioned to probe the flavor sector with unprecedented precision, potentially uncovering the unique signatures predicted by the RS model and shedding light on the nature of flavor and CP violation.

Could alternative models, such as supersymmetry or composite Higgs models, offer equally compelling explanations for the observed flavor and CP violation phenomena without invoking extra dimensions?

Answer: Yes, alternative models like supersymmetry (SUSY) and composite Higgs models can also explain flavor and CP violation without extra dimensions, but they do so through different mechanisms and with distinct experimental signatures: Supersymmetry (SUSY): Flavor Violation: In SUSY, flavor violation arises from the possibility of off-diagonal terms in the squark and slepton mass matrices. These terms can induce flavor-changing neutral currents (FCNCs) at loop level, leading to processes like μ → eγ and meson mixing. CP Violation: SUSY introduces new complex phases in the soft SUSY-breaking terms, providing additional sources of CP violation beyond the CKM matrix. These phases can contribute to electric dipole moments (EDMs) of particles, as well as CP-violating observables in B-meson decays. Compelling Features: SUSY offers an elegant solution to the hierarchy problem, provides dark matter candidates, and leads to gauge coupling unification at high energies. Challenges: The lack of direct evidence for superpartners at the LHC has put constraints on SUSY models, requiring some degree of fine-tuning. Composite Higgs Models: Flavor Violation: In these models, the Higgs boson is a composite particle arising from a new strong interaction. Flavor violation can originate from the interactions between SM fermions and the constituents of the composite Higgs. CP Violation: Similar to SUSY, composite Higgs models can introduce new CP-violating phases through the interactions in the strong sector. Compelling Features: Composite Higgs models address the hierarchy problem by treating the Higgs as a pseudo-Goldstone boson, naturally explaining its lightness. Challenges: Constructing realistic composite Higgs models that satisfy flavor and electroweak precision constraints can be challenging. Comparison with RS Model: Origin of Flavor Violation: The RS model's flavor violation is geometric, arising from the localization of fermions in the extra dimension. In contrast, SUSY and composite Higgs models generate flavor violation through new particles and interactions. Experimental Signatures: The RS model predicts distinct signatures, such as KK excitations and potentially observable flavor-violating di-Higgs couplings. SUSY searches focus on finding superpartners, while composite Higgs models predict new resonances in the TeV range. Conclusion: While both SUSY and composite Higgs models offer compelling explanations for flavor and CP violation, they differ significantly from the RS model in their underlying mechanisms and predicted experimental signatures. Ultimately, distinguishing between these models requires a combination of precise measurements of flavor observables, searches for new particles, and careful analysis of their properties.

What are the broader cosmological implications of the RS model, particularly regarding its potential role in explaining the matter-antimatter asymmetry in the universe?

Answer: The Randall-Sundrum (RS) model, while primarily proposed to address the hierarchy problem, has intriguing cosmological implications, particularly regarding the matter-antimatter asymmetry. However, it faces challenges in fully explaining this asymmetry: Potential Sources of Baryogenesis: KK Mode Decays: The RS model predicts heavy Kaluza-Klein (KK) excitations of SM particles. These KK modes could have CP-violating decays in the early universe, potentially fulfilling the Sakharov conditions for baryogenesis: Baryon Number Violation: Possible through higher-dimensional operators or interactions with new particles beyond the SM. C and CP Violation: Present in the model due to complex phases in Yukawa couplings and potentially in the Higgs sector. Out-of-Equilibrium Dynamics: Achievable during the decay of heavy KK modes if their decay rates are slower than the expansion rate of the universe. Warped Leptogenesis: Similar to standard leptogenesis scenarios, the RS model could generate a lepton asymmetry through the CP-violating decays of heavy right-handed neutrinos. This lepton asymmetry could then be converted to a baryon asymmetry via sphaleron processes. The warped geometry might provide new mechanisms for generating the required lepton asymmetry. Challenges and Open Questions: Sufficient CP Violation: While the RS model introduces new sources of CP violation, it's not clear whether they are sufficient to generate the observed baryon asymmetry. Detailed calculations are needed to determine if the amount of CP violation is large enough. Washout Processes: Any baryon asymmetry generated in the early universe can be diluted or erased by washout processes, such as inverse decays or scattering processes that violate baryon number. The efficiency of these washout processes in the RS model needs to be carefully considered. Connection to Inflation: The RS model does not inherently address the inflationary epoch. Connecting the RS model to a successful inflationary scenario and understanding the interplay between the two is crucial for a complete cosmological picture. Alternative Explanations: It's important to note that other mechanisms for baryogenesis exist, such as electroweak baryogenesis or Affleck-Dine baryogenesis, which do not rely on the RS model. These mechanisms might provide more natural explanations for the matter-antimatter asymmetry. Conclusion: The RS model offers intriguing possibilities for baryogenesis, but it faces challenges in fully explaining the observed matter-antimatter asymmetry. Further theoretical work is needed to determine if the model can generate sufficient CP violation and overcome washout processes. Additionally, connecting the RS model to a successful inflationary scenario is crucial for a comprehensive cosmological understanding. While the RS model's role in baryogenesis remains an open question, it highlights the potential interplay between particle physics at the TeV scale and the evolution of the early universe.
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