Yang-Hwan Ahn

Dr. Yang-Hwan Ahn


Research Focus & Metrics

Academic Career Length

15Years (2012-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

View All Publications
2 November 2012 in Physical Review D
Verified
Journal Article
Closed access
YAYang-Hwan Ahn
Yang-Hwan Ahn
SKSin Kyu Kang
Sin Kyu Kang
Motivated by recent observations of nonzero $\theta${}13 from the Daya Bay and RENO experiments, we propose a renormalizable neutrino model with A4 discrete symmetry accounting for deviations from the tri-bimaximal mixing pattern of the neutrino mixing matrix indicated by neutrino oscillation data. In the model, the light neutrino masses can be generated by radiative corrections, and we show how the light neutrino mass matrix can be diagonalized by the Pontecorvo-Maki-Nakagawa-Sakata mixing matrix whose entries are determined by the current neutrino data, including the Daya Bay result. We show that the origin of the deviations from the tri-bimaximal mixing is nondegeneracy of the neutrino Yukawa coupling constants, and unremovable CP phases in the neutrino Yukawa matrix give rise to both low energy CP violation measurable from neutrino oscillation and high energy CP violation.

9 March 2015 in Physical Review D
Verified
Journal Article
Open access
YAYang-Hwan Ahn
Yang-Hwan Ahn
In an attempt to uncover any underlying physics in the standard model (SM), we suggest a μ–τ power law in the lepton sector, such that relatively large 13 mixing angle with bilarge ones can be derived. On the basis of this, we propose a neat and economical model for both the fermion mass hierarchy problem of the SM and a solution to the strong charge parity (CP) problem, in a way that no domain wall problem occurs, based on A4×U(1)X symmetry in a supersymmetric framework. Here we refer to the global U(1)X symmetry that can explain the above problems as “flavored Peccei-Quinn symmetry.” In the model, a direct coupling of the SM gauge singlet flavon fields responsible for spontaneous symmetry breaking to ordinary quarks and leptons, both of which are charged under U(1)X, comes to pass through Yukawa interactions, and all vacuum expectation values breaking the symmetries are connected to each other. So the scale of Peccei-Quinn symmetry breaking is shown to be roughly located around the 1012  GeV section through its connection to the fermion masses. The model predictions are shown to lie on the testable regions in the very near future through on-going experiments for neutrino oscillation, neutrinoless double beta decay, and the axion. We examine the model predictions, arisen from the μ–τ power law, on leptonic CP violation, neutrinoless double beta decay, and atmospheric mixing angle, and show that the fermion mass and mixing hierarchies are in good agreement with the present data. Interestingly, we show the model predictions on the axion mass ma≃2.53×10−5  eV and the axion coupling to photon gaγγ≃1.33×10−15  GeV−1. And subsequently the square of the ratio between them is shown to be one or two orders of magnitude lower than that of the conventional axion model.

18 April 2012 in Physical Review D
Verified
Journal Article
Closed access
YAYang-Hwan Ahn
Yang-Hwan Ahn
HOHiroshi Okada
Hiroshi Okada
We propose a new scenario in a radiative seesaw model based on A4 flavor symmetry. In this model, we explore a possibility of linking nonzero $\theta${}13 to dark matter. And we analyze the lepton sector to predict the observed neutrinos and mixings, especially obtaining a lower bound of $\theta${}13$\gtrsim${}3.5\ifmmode^\circ\else\textdegree\fi{}. We show that the nonzero $\theta${}13 is correlated with our heavy Majorana type of dark matter. Also we predict that the mass be O(1\char21{}10)\,\,TeV, as a result of analyzing the Wilkinson-Microwave-Anisotropy-Probe and lepton flavor violation.

25 June 2013 in Physical Review D
Verified
Journal Article
Closed access
PDF file
YAYang-Hwan Ahn
Yang-Hwan Ahn
SKSin Kyu Kang
Sin Kyu Kang
Choong Sun KimChoong Sun Kim
Choong Sun Kim
We propose a simple renormalizable model for the spontaneous CP violation based on SU(2)L×U(1)Y×A4 symmetry in a radiative seesaw mechanism, which can be guaranteed by an extra Z2 symmetry. In our model CP is spontaneously broken at high energies, after the breaking of flavor symmetry, by a complex vacuum expectation value of the A4 triplet and gauge-singlet scalar field. We show that the spontaneously generated CP phase could become a natural source of leptogenesis, and also investigate CP violation at low energies in the lepton sector and show how the CP phases in the Pontecorvo-Maki-Nakagawa-Sakata formalism could arise through a spontaneous symmetry-breaking mechanism. As a numerical study, interestingly, we show that the normal mass hierarchy favors relatively large values of θ13, large deviations from maximality of θ23<π/4, and the Dirac-CP phase 0°≤δCP≤50° and 300°≤δCP≤360°. For the inverted hierarchy case, the experimentally measured values of θ13 favors θ23>π/4 and discrete values of δCP around 100°, 135°, 255°, and 300°. Finally, with a successful leptogenesis our numerical results give more predictive values on the Dirac CP phase: for the normal mass hierarchy 1°≲δCP≲10° and for inverted one δCP∼100°, 135°, 300°.

21 January 2015 in Physical Review D
Verified
Journal Article
Open access
PDF file
YAYang-Hwan Ahn
Yang-Hwan Ahn
PGPaolo Gondolo
Paolo Gondolo
To explain the fermion masses and mixings naturally, we introduce a specific flavor symmetry and mass suppression pattern that constrain the flavor structure of the fermion Yukawa couplings. Our model describes why the hierarchy of neutrino masses is milder than the hierarchy of charged fermion masses in terms of successive powers of flavon fields. We investigate CP violation and neutrinoless double beta (0νββ) decay and show how they can be predicted and constrained in our model by present and upcoming experimental data. Our model predicts that the atmospheric neutrino mixing angle θ23 should be within ∼1° of 45° for the normal neutrino mass ordering and between ∼4° and ∼8° degrees away from 45° (in either direction) for the inverted neutrino mass ordering. For both neutrino mass ordering and inverted neutrino mass ordering, our model predicts that a 0νββ Majorana mass in the limited range 0.035  eV<|mee|≲0.15  eV, which can be tested in current experiments. Moreover, our model can successfully accommodate flavorless leptogenesis as the mechanism to generate the baryon asymmetry in the Universe, provided the neutrino mass ordering is normal, |mee|≃0.072±0.012  eV, and either θ23≃44° and the Dirac CP-violating phase δCP≃20° or 60° or θ23≃46° and δCP≃205° or 245°.

10 September 2012 in Physical Review D
Verified
Journal Article
Open access
YAYang-Hwan Ahn
Yang-Hwan Ahn
SBSeungwon Baek
Seungwon Baek
PGPaolo Gondolo
Paolo Gondolo
The recent measurement of a nonzero neutrino mixing angle ${$\theta${}}_{13}$ requires a modification of the tri-bimaximal mixing pattern that predicts a zero value for it. We propose a new neutrino mixing pattern based on a spontaneously broken ${A}_{4}$ flavor symmetry and a type-I seesaw mechanism. Our model allows for approximate tri-bimaximal mixing and nonzero ${$\theta${}}_{13}$, and contains a natural way to implement low- and high-energy $CP$ violations in neutrino oscillations, and leptogenesis with a renormalizable Lagrangian. Both normal and inverted mass hierarchies are permitted within $3$\sigma${}$ experimental bounds, with the prediction of small (large) deviations from maximality in the atmospheric mixing angle for the normal (inverted) case. Interestingly, we show that the inverted case is excluded by the global analysis in $1$\sigma${}$ experimental bounds, while the most recent MINOS data seem to favor the inverted case. Our model make predictions for the Dirac $CP$ phase in the normal and inverted hierarchies, which can be tested in near-future neutrino oscillation experiments. Our model also predicts the effective mass $|{m}_{ee}|$ measurable in neutrinoless double beta decay to be in the range $0.04$\lesssim${}|{m}_{ee}|$\lesssim${}0.15\text{ }\text{ }\mathrm{eV}$ for the normal hierarchy and $0.06$\lesssim${}|{m}_{ee}|$\lesssim${}0.11\text{ }\text{ }\mathrm{eV}$ for the inverted hierarchy, both of which are within the sensitivity of the next generation experiments.