SearcharxivSearch

arXiv subjects

Chia-Wei Liu

Publications and source records attributed to Chia-Wei Liu.

At least 19 recordsLinked to original sources

Probing the imaginary parts and their $q^2$ dependences for the tau $g-2$ and EDM

The $τ$ anomalous magnetic dipole moment (MDM) $a_τ= (g-2)_τ/2$ and electric dipole moment (EDM) $d_τ$, are precision probes of electroweak dynamics and possible new physics sources, yet both remain weakly constrained experimentally. Treated as generalized form factors, these quantities exhibit a generic $q^2$ dependence for an off-shell interacting photon. For timelike momentum transfer above the $τ^+τ^-$ threshold, $q^2 = s > 4m_τ^2$, the form factors can acquire absorptive imaginary parts. We investigate how such a $q^2$ dependence and the associated imaginary parts are generated from two complementary perspectives: the model-independent Standard Model Effective Field Theory (SMEFT) and a UV-complete Two-Higgs-Doublet Model (2HDM). The effective framework reveals the intimate correlation between $a_τ$ and $d_τ$. New CP-violating interactions which generate a non-zero $d_τ$, can also generically have non-zero contributions to $a_τ$, thereby deeply linking their phenomenological studies. Within the 2HDM, we demonstrate that sizable imaginary parts and significant $q^2$ running can be generated at levels accessible by $e^+e^-$ colliders. Motivated by these features, we propose experimental methods to extract both the real and imaginary components of the dipole form factors. Utilizing these techniques, we show that Belle II and the Super Tau-Charm Facility (STCF) can improve current bounds on $a_τ$ by more than one order of magnitude. Finally, we highlight that combining measurements across the distinct center-of-mass energies of Belle II and STCF provides a unique, previously unexplored avenue to explicitly obtain information about the $q^2$ evolution of these dipole form factors.

hep-ph

Mixing-angle sensitivity of inclusive $Ξ_{bc} $ and $Ω_{bc}$ lifetimes

We study the inclusive lifetimes of $Ξ_{bc}^{+}$, $Ξ_{bc}^{0}$, and $Ω_{bc}^{0}$, with emphasis on the mixing between the spin-zero and spin-one $bc$-diquark configurations. The relevant hadronic matrix elements are evaluated in both the homogeneous bag model (HBM) and the nonrelativistic quark model (NRQM). At the benchmark mixing angles of $-23.0^\circ$ for $Ξ_{bc}$ and $-23.5^\circ$ for $Ω_{bc}$, the corresponding lifetime triplets are $\left(τ_{Ξ_{bc}^{+}},τ_{Ξ_{bc}^{0}},τ_{Ω_{bc}^{0}}\right)=\left(0.421^{+0.093}_{-0.093},0.075^{+0.035}_{-0.010},0.223^{+0.074}_{-0.043}\right)\,\mathrm{ps}$ in the HBM and $\left(τ_{Ξ_{bc}^{+}},τ_{Ξ_{bc}^{0}},τ_{Ω_{bc}^{0}}\right)=\left(0.367^{+0.076}_{-0.070},0.100^{+0.032}_{-0.014},0.229^{+0.066}_{-0.042}\right)\,\mathrm{ps}$ in the NRQM. Relative to the unmixed spin-one reference points, the $Ξ_{bc}^{0}$ and $Ω_{bc}^{0}$ lifetimes decrease by approximately $17\%$-$19\%$. Neither the minimum nor the maximum of the central lifetime curves occurs at a pure $S_{bc}=0$ or $S_{bc}=1$ configuration; the extrema instead lie at mixed angles with $\left|ϕ_{\mathcal{B}}\right|\simeq27^\circ$-$63^\circ$. The two pure-spin limits alone are therefore insufficient to characterize the full mixing-angle dependence.

hep-ph

Nonstandard Solution for Anomaly Cancellation as Seesaw Neutrino Origin in the SM

For fixed Standard Model (SM) non-Abelian representations of 15 chiral fermions with arbitrary hypercharges, anomaly cancellation admits the usual assignment and a distinct nonstandard solution. In the latter, the colored exotic quark and exotic lepton weak doublets and exotic lepton singlet have zero hypercharge, whereas the two colored exotic quark singlets carry opposite hypercharges $-q$ and $q$. The exotic neutral lepton singlets naturally play the role of the heavy neutrinos. The minimal model with two exotic lepton copies gives a rank-two seesaw, the minimal seesaw model, with one massless active neutrino and predicts $m_{ββ} = 1.2 \text{-} 4.1 \, \mathrm{meV}$ for normal ordering or $15.9\text{-}48.9 \,\mathrm{meV}$ for inverted ordering. In a direct SM realization, generating exotic quark masses through the SM Higgs mechanism forces the exotic quarks to carry electric charges $\pm 1/2$. A separate $\mathrm{SU}(2)_{L'}$ realization of the nonstandard solution can allow exotic quarks from several TeV to $10\,\mathrm{TeV}$ with order-one Yukawa couplings. In this model, the charged exotic quarks and leptons carry electric charges $\pm q$. In both cases, the lightest exotic quark and lepton are stable, but suitable choices of their charges and masses can satisfy experimental constraints.

hep-ph

Study of doubly heavy baryon lifetimes

We study the lifetimes and inclusive semileptonic decay widths of doubly heavy baryons within the framework of heavy quark expansion. Our analysis includes next-to-leading-order corrections to the dimension-3, -5, and -6 operators, together with the leading dimension-7 contributions, while the nonperturbative matrix elements are evaluated in a bag model with translationally improved baryon wave functions. We obtain $( τ_{Ξ_{cc}^{++}} , τ_{Ξ_{cc}^{+}} , τ_{Ω_{cc}^{+}} ) = ( 2.67^{+0.95}_{-0.94},\, 0.47^{+0.09}_{-0.08},\, 1.79^{+0.64}_{-0.62} ) \times 10^{-13}\,{\rm s}$ and $( τ_{Ξ_{bb}^{0}} , τ_{Ξ_{bb}^{-}} , τ_{Ω_{bb}^{-}} ) = ( 0.75^{+0.13}_{-0.11},\, 0.92^{+0.15}_{-0.15},\, 0.93^{+0.15}_{-0.15} ) \times 10^{-12}\,{\rm s}$. The lifetime hierarchy patterns are found to be $τ(Ξ_{cc}^{++})>τ(Ω_{cc}^+)>τ(Ξ_{cc}^+)$ and $τ(Ω_{bb}^{-})\simτ(Ξ_{bb}^-)>τ(Ξ_{bb}^0)$ for doubly charmed and bottom baryons, respectively. The $W$-exchange contribution plays a crucial role in generating the large lifetime splitting in the doubly charmed sector and remains phenomenologically important for doubly bottom baryons. In particular, for $Ξ_{cc}^{+}$ the dominant dimension-6 spectator effect, namely $W$-exchange, surpasses the nominally leading term. The same spectator operator is realized as destructive Pauli interference in $D^+$, owing to the $d$ versus $\bar d$ spectator. Although the $Ξ_{cc}^{+}$ case does not lead to the negative decay width encountered for $D^+$, the absolute value of $τ(Ξ_{cc}^{+})$ should nevertheless be regarded as only indicative. In addition to the total lifetimes, we calculate the separate nonleptonic and semileptonic contributions, which allow us to trace the pattern of spectator effects in each baryon channel.

hep-ph

New $CP$ sum rules from exact $U$-spin degeneracy

We propose a new class of $CP$ sum rules in the $U$-spin limit, based on the observation that the weak phase in the Standard Model can be removed in the degenerate limit $m_d=m_s$. Unlike previous $U$-spin analyses formulated at the amplitude level, our sum rules are expressed directly in terms of decay widths. They apply to matched partial waves, spin observables, and angular moments and include nonpairwise cases beyond the usual single-insertion $d\leftrightarrow s$ relation.

hep-ph

Strange Quark Electric Dipole Moment withTopological Anomalies

We introduce an anomaly-based framework to probe quark electric dipole moments in exclusive hadronic final states produced in $e^+e^-$ annihilation. Chern-Simons-induced anomalous couplings yield a clean T-odd asymmetry $A_T$ from interference between the Standard-Model amplitude and dipole-moment contributions. As an application, $γ^\ast\to K^+K^-π^0$ provides direct sensitivity to the strange-quark EDM $d_s$ in the chiral limit. The precision on $d_s$ can reach $\mathcal{O}(10^{-16})\,e\cdot\mathrm{cm}$ with existing CMD--3 data and $\mathcal{O}(10^{-18})\,e\cdot\mathrm{cm}$ using current $J/ψ$ samples at BESIII, improving the current direct constraint from hyperon EDM by two to three orders.

hep-ph

Puzzles in charmed baryon semileptonic decays with $SU(3)_F$ flavor symmetry and lattice inputs

Recent measurements of charmed-baryon semileptonic decays signal large tensions between experiment and theory, including $SU(3)_F$ analyses and lattice-quantum chromodynamics simulations. Possible sources of the discrepancy include the experimental normalization mode $Ξ_c^0 \to Ξ^- π^+$. Using lattice-QCD inputs in an $SU(3)_F$ analysis including first-order symmetry breaking, we predict ${\cal B}( Ξ_c^+ \to Σ^0 \ell^+ ν_\ell ) / {\cal B}( Ξ_c^+ \to Ξ^0 \ell^+ ν_\ell )=(2.6\pm0.3)\%, $ and ${\cal B}( Ξ_c^+ \to Λ\ell^+ ν_\ell )/{\cal B}( Ξ_c^+ \to Ξ^0 \ell^+ ν_\ell )=(1.1\pm0.1)\%, $ with $\ell^+=(e^+,μ^+)$. These ratios provide normalization-independent tests and may help clarify the origin of the present tension.

hep-ph

The Negative-$Σ\barΣ$ Angular-Parameter Puzzle in $J/ψ$ and $ψ(2S)$ Decays

Experimental measurements of $J/ψ$ and $ψ(2S)$ decays to octet baryon pairs reveal a negative-$Σ\barΣ$ puzzle in the angular distributions: $α_Σ^{J/ψ}<0$, whereas the other measured $J/ψ$ octet channels and the corresponding $ψ(2S)$ channels have positive angular parameters. We show that an $\mathrm{SU}(3)_F$-exact singlet description is strongly disfavored in a $χ^2$ fit, giving $χ^2\simeq 10^5$. By contrast, a reduced scenario in which a common final-state interaction mixes the $\mathrm{S}$- and $\mathrm{D}$-wave amplitudes, with an antisymmetric direct octet and a full diagonal $\mathrm{S}$-$\mathrm{D}$ rescattering block, gives $χ^2=4.21$ for two nominal degrees of freedom. The negative $Σ\barΣ$ angular parameter is traced to the pattern of the rescattered $\mathrm{S}$- and $\mathrm{D}$-wave amplitudes. The apparent large $\mathrm{SU}(3)_F$-breaking effect is decomposed into three ingredients: the fitted $\mathrm{D}$-wave source is much larger than the $\mathrm{S}$-wave source, the breaking remains modest when normalized to the $\mathrm{D}$ wave, and $\mathrm{D}\to\mathrm{S}$ rescattering transfers the $\mathrm{SU}(3)_F$-breaking effect from the $\mathrm{D}$ wave into the small $\mathrm{S}$-wave baseline, where it appears large. The largest remaining pull comes from the $ψ(2S)\to N\bar{N}$ angular input, motivating a renewed experimental check of $ψ(2S)\to n\bar{n}$.

hep-ph

Complex $τ$ Electric Dipole Moment from GeV-Scale New Physics

Among the charged leptons, the $τ$ electric dipole moment~($d_τ$) is the least constrained. We show that the Im[$d_τ$] imposes strong constraints on new physics that have yet to be discussed. Motivated in particular by the Super Tau-Charm Facility (STCF), which will provide a uniquely clean environment for precision $τ$-physics, we study the momentum-transfer dependence of $d_τ(q^2)$ and compare the projected sensitivities of STCF and Belle II. Our analysis shows that an axion-like coupling of the $τ$ lepton can induce sizable real and imaginary components of the EDM. The predicted EDM values may approach the present experimental sensitivities, making them accessible to future measurements at Belle II and the STCF.

hep-ph

Spin-flavor entanglement in $Λ_b \to ΛD$ and weak phase extraction

We identify a new spin-flavor entanglement structure in $Λ_b\toΛD$ decays, formed by the correlation between the $Λ$ spin and the $D$ flavor states ($D=D^0,\overline D^0,D_1,D_2$). The entanglement information is encoded in the decay rates and Lee-Yang parameters of the four neutral-$D$ modes. We then show that the same spin-flavor structure provides a new method to determine the weak phase $γ$, a key angle of the Cabibbo-Kobayashi-Maskawa unitarity triangle. We find that the experimental uncertainty scales as $σ_γ\propto 1/{\cal C}$, where ${\cal C}$ is the Wootters concurrence, thereby quantitatively relating the precision of the weak-phase extraction to the amount of spin-flavor entanglement.

hep-ph

Topological quantization of vector meson anomalous couplings

We identify an overlooked Wess--Zumino--Witten structure in the hidden-local-symmetry~(HLS) formulation of vector mesons. The newly identified term generically leads to the topological quantization of the vector-meson anomalous couplings. If confirmed experimentally, this structure would expose the gauge nature of vector mesons in the anomalous sector and single out HLS over matter-field descriptions. The observed success of vector-meson dominance in anomalous interactions can then be explained by topological-action saturation of the odd-intrinsic-parity processes. Precision measurements of $η^{(\prime)}\toπ^+π^-γ^*$ form factors at BESIII and the Super $τ$-Charm Facility can directly test this saturation picture.

hep-ph

Potential of discovering $Ξ_{cc}^+$ in $Λ_b $ decays

We propose to search for $Ξ_{cc}^+$ in the decay $Λ_b \to Ξ_{cc}^+ D^-$, which serves as a tagged and reconstructible source of $Ξ_{cc}^+$, providing an experimentally clean environment for its discovery. A possible fully charged final state is $[(pK^- K^- π^+)_{Ξ^0_c} π^ + ]_{Ξ_{cc}^+} \,(K^+ π^- π^-)_{D^-}$, where the subscripts indicate the parent hadron in the decay chain. We estimate the branching fraction to be ${\cal B}(Λ_b \to Ξ_{cc}^+ D^-) = ( 5.1 \pm 3.9) \times 10^{-4}$, while the fully charged final state corresponds to an effective branching fraction of order $10^{-8}$. These results indicate that LHCb has the potential to discover the $Ξ_{cc}^+$. The prospects for observing $Ω_{cc}^+$ are also briefly discussed.

hep-ph

Charmed baryon decays: $SU(3)_F$ breaking and CP violation

We present a comprehensive study of anti-triplet charmed baryon decays into octet baryons and pseudoscalar mesons using the $SU(3)_F$ flavor symmetry framework. By decomposing the flavor structure, all decay amplitudes are parametrized with a minimal set of irreducible amplitudes, and the Körner-Pati-Woo theorem further reduces the number of independent parameters from the original 35 to 19 under exact symmetry when small terms proportional to $λ_b = V_{cb}^*V_{ub}$ are neglected. The independent number becomes 27 with leading $SU(3)_F$ breaking effects. A global fit to 51 experimental measurements yields a $χ^2$/d.o.f. of 2.36 and provides precise values for the decay amplitudes. Notable discrepancies are observed in the fitted branching fractions of $Ξ_c^0 \to Ξ^- π^+$ and $Ξ_c^+ \to Ξ^- π^+ π^+$, which exceed current measurements by more than $2σ$. Incorporating final-state rescattering effects to recover the main effects of terms proportional to $λ_b$, we predict enhanced CP violation, with $A_{CP}$ reaching up to $10^{-3}$ in golden channels such as $Ξ_c^0 \to p K^-$ and $Ξ_c^0 \to Σ^+ π^-$. Our analysis also finds that the branching ratio for $Ξ_c^+ \to Λπ^+$ is enhanced to $(9.7 \pm 1.2) \times 10^{-4}$ due to significant cancellations.

hep-ph

Demonstration of TFTs 3D Monolithically Integrated on GaN HEMTs using Cascode Configuration with High Breakdown Voltage (>1900V)

This study demonstrates 3D monolithic integration of amorphous indium-gallium-zinc oxide (a-IGZO) thin-film transistors (TFTs) on Gallium Nitride (GaN) high electron mobility transistors (HEMTs) in a cascode configuration, achieving high breakdown voltage capabilities exceeding 1900 V. Two device configurations, differing in a-IGZO channel thickness (30 nm / 10 nm), are fabricated and evaluated. Sample B, with a 10 nm a-IGZO channel, demonstrates superior electrical performance, including a high ON/OFF current ratio (~10^7), low subthreshold swing (SS), and a high breakdown voltage exceeding 1900 V comparable to standalone GaN power HEMTs. The results highlight the feasibility and potential of 3D integrated TFT on GaN power HEMTs, paving the way for new opportunities for the TFTs for high voltage applications.

physics.app-ph

Large CP Asymmetries from Final-State Interactions in Charmful Baryonic Decays of $B^0 \to Ξ_c^+ \overlineΞ_c^-$ and $B_s^0 \to Λ_c^+ \overlineΛ_c^-$

We study the direct CP asymmetries in the decays of $B^0 \to Ξ_c^+ \overlineΞ_c^-$ and $B_s^0 \to Λ_c^+ \overlineΛ_c^-$, emphasizing the critical role of final-state interactions (FSIs). In these channels, the small energy release and annihilation topology suppress short-distance contributions while enhancing long-distance effects. By separating the decay amplitudes into S and P waves, we show that the P-wave component, carrying only a single weak phase, contributes negligibly to CP asymmetries. In contrast, the S-wave amplitude, strongly modified by FSIs, acquires a substantial strong phase that enables interference among multiple weak phases, producing large CP-violating effects. Numerically, we find sizable asymmetries of $a_{CP}^{\text{dir}} = 0.88 \pm 0.05 \pm 0.10$ for $B^0 \to Ξ_c^+ \overlineΞ_c^-$ and $a_{CP}^{\text{dir}} = -0.106 \pm 0.019 \pm 0.010$ for $B_s^0 \to Λ_c^+ \overlineΛ_c^-$, where the first and second uncertainties stem from the poorly known hadron couplings and the omission of the $B^0 \to K^+ K^- \to Ξ_c^+ \overlineΞ_c^-$ rescattering process. For practical feasibility, we restrict our analysis to intermediate states involving pseudoscalar mesons, which yield tractable loop integrals. Excited intermediate states, such as $D^{(*)} \overline{D}^{(*)}$, are omitted because their inclusion would require handling non-renormalizable interactions, introducing substantial ambiguity. These results, combined with the relatively large branching fractions, make these modes prime targets for experimental searches at LHCb and Belle II, potentially offering new insights into strong dynamics and nonperturbative QCD in heavy-hadron decays.

hep-ph

Large CP violation in charmed baryon decays

This work presents the first detailed numerical predictions of CP violation in antitriplet charmed baryon decays. Adopting the flavor $SU(3)_F$ symmetry and the final state re-scattering framework, we relate the CKM-suppressed amplitudes to the leading ones, which are proportional to $λ_b$ and $λ_d$, respectively, with $λ_q = V_{uq}V^*_{cq}$. Larger-than-expected CP violations are found, reaching the order of $10^{-3}$, similar in magnitude to those in $D^0 \to π^+π^- ,K^+K^-$. This opens a promising avenue for observing CP violation in charmed baryon decays and testing the Standard Model.

hep-ph

Identify hadron anomalous couplings at colliders

We investigate the identification of the Wess-Zumino-Witten (WZW) Lagrangian at colliders such as BESIII and the Super-$τ$-Charm Facility. Our analysis concentrates on the radiative decays of $η$ and $η'$ mesons, including $η^{(\prime)} \to γγ$, $η^{(\prime)} \to γ\ell^+ \ell^-$, $η^{(\prime)} \to π^+π^-γ$, and $η^{(\prime)} \to π^+π^-\ell^+\ell^-$, as well as semileptonic kaon decays such as $K^+ \to π^+π^- e^+ ν_e$. Employing the hidden local symmetry framework to incorporate vector meson contributions, we compute the decay amplitudes and form factors. For the decay $η\to π^+π^-γ$, the box anomaly dominates, and we find that the anomalous coupling can be experimentally determined to percent-level precision at BESIII. In contrast, vector meson contributions are significant in the decay $η' \to π^+π^-γ$. Using experimental data for $η' \to π^+π^-γ$, we obtain ${\cal B}_{\mathrm{box}}^{\text{exp}} = (1.70 \pm 0.05)\%$, which is approximately ten times larger than previously expected experimentally. We observe good agreement between our calculated anomalous couplings and experimental results. In kaon decays, WZW terms uniquely contribute to the form factor $H$, which can be extracted from parity-conserving decay distributions. While predictions at the chiral point closely match experimental values (e.g., $H^+ = -2.31$ versus $-2.27 \pm 0.10$), we find that intermediate vector meson states introduce substantial corrections, potentially as large as 25%. We strongly advocate for revisiting these experiments to achieve improved precision in form factor extractions.

hep-ph

Large CP violation in $Λ^0_b \to pK^-π^+π^-$ and its U-spin partner decays

The LHCb Collaboration has recently found a large CP-violating rate asymmetry in the $b$-baryon decay $Λ^0_b \to pK^-π^+π^-$. This is the first observation of CP violation in baryon processes, opening a new window to test its standard model origin. Many more baryon decays are expected to exhibit observable signals of CP violation. We show that there also exists large CP violation in the U-spin partner decay mode, $Ξ^0_b \to Σ^+π^- K^+K^-$, with rate asymmetry $$A_{CP}(Ξ^0_b \to Σ^+π^- K^+ K^-) = - A_{CP}(Λ^0_b \to p K^- π^+ π^-)~ \frac{Br(Λ^0_b \to p K^- π^+ π^-)}{Br(Ξ^0_b \to Σ^+ π^- K^+ K^-)}~ \frac{τ^{Ξ_b}}{τ^{Λ_b}} $$ in the U-spin symmetry limit. By neglecting a subleading contribution in the amplitudes, we obtain $$A_{CP}(Λ^0_b \to p π^+ π^- π^-) = A_{CP}( Ξ^0_b \to Σ^+π^- K^+ K^-) = -(12 \pm 3 ) \%. $$ These predictions provide crucial tests for the standard model.

hep-ph