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Addressing the SS-wave scalar f0(1500)f_0(1500)-resonance in quasi-four-body FCNC rare Bs→f0(1500)(→π+π−)ℓ+ℓ−/ννˉB_s \to f_0(1500) (\to π^+ π^- ) \ell^+ \ell^- / ν\bar ν decays

Published 16 Sep 2026 in hep-ph | (2609.18890v1)

Abstract: The f0(1500)f_0(1500) is a quite special resonance in the light scalar spectrum. Compared with other nearby resonance, it has an unexpectedly narrow decay width. Since its mass region overlaps strongly with f0(1370)f_0(1370) and f0(980)f_0(980), physicists have long debated its internal structure. To explore this issue, this work adopted the conventional quark-antiquark qqˉq\bar{q} picture and investigated the behavior of the f0(1500)f_0(1500)-resonance in quasi-four-body decay channels. Based on this, we constructed a twist-2 light-cone distribution amplitude(LCDA) schemes based on the light-cone harmonic oscillator model, and presented their moments ⟨ξ<sup>n</sup><em>2;f0(1500)⟩∣</em>μ\langle ξ<sup>n</sup> <em>{2;f_0(1500)} \rangle |</em>μ and Gegenbauer moments an;f0(1500)(μ)a_{n;f_0(1500)}(μ) at μ<em>0=1 GeVμ<em>0=1~\mathrm{GeV} and μk=3 GeVμ_k= 3~\mathrm{GeV} for n=1,3,5n=1,3,5. Meanwhile, the Bs→f0(1500)B_s\to f_0(1500) transition form factors (TFFs) are calculated by using the QCD light-cone sum rule. Then, we obtained the three TFFs at large recoil point, {\it i.e.,} f</em>+<sup>Bs</sup>f0(1500)(0)=0.390−0.046<sup></sup>+0.047f</em> + <sup>{B_s</sup> f_0(1500)}(0)= 0.390_{-0.046}<sup>{</sup> + 0.047}, f−<sup>Bs</sup>f0(1500)(0)=−0.460−0.055<sup></sup>+0.051f_-<sup>{B_s</sup> f_0(1500)}(0)= -0.460_{-0.055}<sup>{</sup> + 0.051}, and fT<sup>Bs</sup>f0(1500)(0)=0.568<sup></sup>+0.069−0.065f_{\rm T}<sup>{B_s</sup> f_0(1500)}(0)= 0.568<sup>{</sup> + 0.069}_{-0.065}. In addition, we extrapolated TFFs to the whole physical q<sup>2q<sup>2-region by using the simplified z(q<sup>2)z(q<sup>2)-series expansion. Then we computed the branching fractions of the quasi-four-body rare decays Bs→f0(1500)(→π+π<sup>−)ℓ</sup>+ℓ<sup>−B_s \to f_0(1500)(\to π^ + π<sup>-)\ell^</sup> + \ell<sup>- and Bs→f0(1500)(→π+π<sup>−)ννˉB_s \to f_0(1500)(\to π^ + π<sup>-)ν\barν. For comparison, we also present the results of the corresponding three-body decays obtained under the narrow-width approximation. Finally, we show the distribution of the double-differential decay width d<sup>2Γ/ds</sup>dq<sup>2d<sup>2Γ/ds</sup> dq<sup>2 for the quasi-four-body decay Bs→f0(1500)(→π+π<sup>−)μ</sup>+μ<sup>−B_s\to f_0(1500)(\toπ^ + π<sup>-)μ^</sup> + μ<sup>-. We hope that our predictions can provide a useful theoretical reference for future experimental measurements and phenomenological research.

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