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$S-P-D$ Mixing in Vector Quarkonia from the Salpeter Equation with Optimized Wave Function Representations

Wen-Yuan Ke, Qiang Li, Tianhong Wang, Tai-Fu Feng, Guo-Li Wang

TL;DR

Using the instantaneous Bethe-Salpeter (Salpeter) framework, this work investigates $S$-$D$ mixing in vector quarkonia by testing eight relativistic wave function representations for the $1^{--}$ state. It shows that tensor forces alone are insufficient and that a $S$-$P$-$D$ mixed structure emerges naturally when relativistic components are included, with the eight representations reduced to four independent radial functions. Among the eight representations, $\varphi_2$ best reproduces charmonium and bottomonium spectra and dileptonic widths, yielding mixing angles $ \theta_{\psi(2S)}=(6.67^{+1.71}_{-1.50})^\circ$, $ \theta_{\psi(1D)}=(7.92^{+1.70}_{-1.43})^\circ$, and $ \theta_{\psi(2D)}=(26.3^{+3.3}_{-3.4})^\circ$ for charmonium, and $ \theta_{\Upsilon(1D)}=(1.78^{+0.32}_{-0.25})^\circ$, $ \theta_{\Upsilon(2D)}=(5.44^{+1.10}_{-0.76})^\circ$ for bottomonium. It also predicts dileptonic widths for the yet-unobserved $\Upsilon(1D)$ and $\Upsilon(2D)$ states: $\Gamma(\Upsilon(1D)\to e^+e^-) = 2.29^{+0.86}_{-0.69}$ eV and $\Gamma(\Upsilon(2D)\to e^+e^-) = 10.5^{+4.2}_{-3.1}$ eV, demonstrating the model’s predictive power and the importance of relativistic multi-wave mixing in vector quarkonia.

Abstract

This paper proposes a novel mechanism based on the instantaneous Bethe-Salpeter (Salpeter) equation for investigating wave function mixing in vector mesons such as $ψ(3770)$. Conventional theories typically treat $ψ(3770)$ as a $2S-1D$ mixed state; however, considering only tensor forces or relativistic corrections alone often leads to mixing angles that are too small and inconsistent with experimental data. Phenomenological $2S-1D$ mixing requires experimental data as input to determine the mixing angles, resulting in limited theoretical studies on states like $Υ(1D, 2D)$ in the absence of experimental data. To more accurately describe $S-D$ mixing and its relativistic effects, this paper systematically compares eight possible relativistic wave function representations ($\varphi_1$ to $\varphi_8$) by solving the Salpeter equation and calculates the mass spectra and dileptonic decay widths of charmonium and bottomonium. The study finds that the wave function representation $\varphi_2$ can simultaneously reproduce the experimental data of both charmonium and bottomonium well. Further analysis reveals that, in addition to $S-D$ mixing, the wave functions of vector mesons contain a non-negligible $P$-wave component, meaning they are $S-P-D$ mixed states. We predict the mixing angles for bottomonium $Υ(1D)$ and $Υ(2D)$ to be $(1.78^{+0.32}_{-0.25})^\circ$ and $(5.44^{+1.10}_{-0.76})^\circ$, with dileptonic decay widths of $2.29^{+0.86}_{-0.69}$ eV and $10.5^{+4.2}_{-3.1}$ eV, respectively.

$S-P-D$ Mixing in Vector Quarkonia from the Salpeter Equation with Optimized Wave Function Representations

TL;DR

Using the instantaneous Bethe-Salpeter (Salpeter) framework, this work investigates - mixing in vector quarkonia by testing eight relativistic wave function representations for the state. It shows that tensor forces alone are insufficient and that a -- mixed structure emerges naturally when relativistic components are included, with the eight representations reduced to four independent radial functions. Among the eight representations, best reproduces charmonium and bottomonium spectra and dileptonic widths, yielding mixing angles , , and for charmonium, and , for bottomonium. It also predicts dileptonic widths for the yet-unobserved and states: eV and eV, demonstrating the model’s predictive power and the importance of relativistic multi-wave mixing in vector quarkonia.

Abstract

This paper proposes a novel mechanism based on the instantaneous Bethe-Salpeter (Salpeter) equation for investigating wave function mixing in vector mesons such as . Conventional theories typically treat as a mixed state; however, considering only tensor forces or relativistic corrections alone often leads to mixing angles that are too small and inconsistent with experimental data. Phenomenological mixing requires experimental data as input to determine the mixing angles, resulting in limited theoretical studies on states like in the absence of experimental data. To more accurately describe mixing and its relativistic effects, this paper systematically compares eight possible relativistic wave function representations ( to ) by solving the Salpeter equation and calculates the mass spectra and dileptonic decay widths of charmonium and bottomonium. The study finds that the wave function representation can simultaneously reproduce the experimental data of both charmonium and bottomonium well. Further analysis reveals that, in addition to mixing, the wave functions of vector mesons contain a non-negligible -wave component, meaning they are mixed states. We predict the mixing angles for bottomonium and to be and , with dileptonic decay widths of eV and eV, respectively.
Paper Structure (5 sections, 7 equations, 1 figure, 8 tables)

This paper contains 5 sections, 7 equations, 1 figure, 8 tables.

Figures (1)

  • Figure 1: Radial wave functions of the wave function $\varphi_{2}$ for charmonium, where $q\equiv |\vec{q}|$.