arXiv subjects

Ying-Quan Peng

Publications and source records attributed to Ying-Quan Peng.

7 recordsLinked to original sources

arXiv2024

Supermassive black holes triggered by QCD axion bubbles

The supermassive black holes (SMBHs) are ubiquitous in the center of galaxies, although the origin of their massive seeds is still unknown. In this paper, we investigate the SMBHs formation from the QCD axion bubbles. In this case, the primordial black holes (PBHs) are considered as the seeds of SMBHs, which are generated from the QCD axion bubbles due to an explicit Peccei-Quinn (PQ) symmetry breaking after inflation. The QCD axion bubbles are formed when the QCD axion starts to oscillate during the QCD phase transition. We consider a general case in which the axion bubbles are formed with the bubble effective angle $θ_{\rm eff}\in(0, \, π]$, leading to the minimum PBH mass $\sim\mathcal{O}(10^4-10^7)M_\odot$ for the axion decay constant $f_a\sim\mathcal{O}(10^{16})\, \rm GeV$. The PBHs at this mass region may account for the seeds of SMBHs.

hep-ph↗

arXiv2024

Light QCD Axion Dark Matter from Double Level Crossings

The even light QCD axion called the $Z_{\mathcal N}$ axion can both solve the strong CP problem and account for the dark matter (DM). We point out that the single and double level crossings can naturally take place in the mass mixing between the $Z_{\mathcal N}$ axion and axionlike particle (ALP). The first level crossing occurs much earlier than the QCD phase transition, while the second level crossing occurs exactly during the QCD phase transition if it exists. We also find that the single level crossing can transform into the double level crossings, depending on the ALP mass $m_A$ versus the zero-temperature $Z_{\mathcal N}$ axion mass $m_{a,0}$. Compared with the no level crossing case, the $Z_{\mathcal N}$ axion relic density can be suppressed in the single level crossing, and enhanced or suppressed in the double level crossings.

hep-ph↗

arXiv2023

Majorana Majoron and the Baryon Asymmetry of the Universe

The spontaneous breaking of the global lepton number, an accidental symmetry in the Standard Model of particle physics, results in a massless goldstone boson, the Majoron, which can be taken as a cold dark matter candidate with properties similar to these of the axion. In this letter, we propose a novel mass generation mechanism for the Majoron via radiative corrections induced by the interaction of a tiny lepton-number-violating (LNV) Majorana mass term of right-handed neutrinos in the canonical seesaw mechanism. We show that this LNV Majorana mass term not only generates the mass of the Majoron but also leads to a non-zero initial velocity of the Majoron, which subsequently impacts on the relic abundance of the Majoron generated in the early universe via the misalignment mechanism. With the assistance of the Weinberg operator, the same initial velocity may also generate the lepton asymmetry, which is subsequently transported into the baryon asymmetry of the universe (BAU) via the weak sphaleron process. As a result, the neutrino masses, dark matter and the BAU can be addressed in this concise theoretical framework.

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arXiv2022

Axion-like Dark Matter from the Type-II Seesaw Mechanism

Although axion-like particles (ALPs) are popular dark matter candidates, their mass generation mechanisms as well as cosmic thermal evolutions are still unclear. In this letter, we propose a new mass generation mechanism of ALP during the electroweak phase transition in the presence of the type-II seesaw mechanism. As ALP gets mass uniquely at the electroweak scale, there is a cutoff scale on the ALP oscillation temperature irrelevant to the specific mass of ALP, which is a distinctive feature of this scenario. The ALP couples to the active neutrinos, leaving the matter effect of neutrino oscillations in a dense ALP environment as a smoking gun. As a by-product, the recent $W$-boson mass anomaly observed by the CDF collaboration is also quoted by the TeV-scale type-II seesaw. We explain three kinds of new physics phenomena are with one stroke.

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arXiv2021

Direct detection of Sub-GeV Dark Matter via 3-body Inelastic Scattering Process

Direct detection of Sub-GeV dark matter (DM) is challenging because the recoil energy of the nuclei or electron from the elastic scattering of a sub-GeV DM off the target can hardly reach the detector threshold. In this paper, we present a new direct detection strategy for sub-GeV DM via the three-body inelastic scattering process, $χ+ χ+ {\rm SM} \to η+ {\rm SM}$, where $χ$ is DM candidate and $η$ is either a DM composite state or any dark radiation. This process is common for a large class of DM models without presuming particular thermal history in the early Universe. The typical signature from this process is almost a monoenergetic pulse signal where the recoil energy comes from either the binding energy or the consumed DM particle. We show that detectable DM mass range can be effectively enlarged compared to the elastic scattering process.

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arXiv2020

Study of semileptonic decay of $\bar{B}_s^0\to ϕl^+ l^-$ in QCD sum rule

In this work we study the semi-leptonic decay of $\bar{B}_s^0\to ϕl^+ l^-$($l=e, μ, τ$) with QCD sum rule method. We calculate the $\bar{B}_s^0\to ϕ$ translation form factors relevant to this semi-leptonic decay, then the branching ratios of $\bar{B}_s^0\to ϕl^+ l^-$($l=e, μ, τ$) decays are calculated with the form factors obtained here. Our result for the branching ratio of $\bar{B}_s^0\to ϕμ^+ μ^-$ agrees very well with the recent experimental data. For the unmeasured decay modes such as $\bar{B}_s^0\to ϕe^+ e^-$ and $\bar{B}_s^0\to ϕτ^+ τ^-$, we give theoretical predictions.

hep-ph↗

arXiv2020

Form Factors and Decay of $\bar{B}_s^0\to J/ψϕ$ From QCD Sum Rule

We calculate $\bar{B}_s^0\to ϕ$ translation form factors $V$, $A_0$, $A_1$, $A_2$ based on QCD sum rule and study the nonleptonic two-body decay of $\bar{B}_s^0\to J/ψϕ$ with the form factors obtained. We calculate the time-integrated branching ratio of $\bar{B}_s^0\to J/ψϕ$ decay. The results for both the total branching ratio and the cases for the final vectors in longitudinal and transverse polarizations are consistent with experimental data.

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