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Junxu Lu

Publications and source records attributed to Junxu Lu.

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The $πη$ interaction and $a_0$ resonances in photon-photon scattering

We revisit the information on the two lightest $a_0$ resonances and $S$-wave $πη$ scattering that can be extracted from photon-photon scattering experiments. For this purpose we construct a model for the $S$-wave photon-photon amplitudes which satisfies analyticity properties, two-channel unitarity and obeys the soft photon as well as the soft pion constraints. The underlying I=1 hadronic $T$-matrix involves six phenomenological parameters and is able to account for two resonances below 1.5 GeV.We perform a combined fit of the $γγ\to πη$ and $γγ\to K_SK_S$ high statistics experimental data from the Belle collaboration. Minimisation of the $χ^2$ is found to have two distinct solutions with approximately equal $χ^2$. One of these exhibits a light and narrow excited $a_0$ resonance analogous to the one found in the Belle analysis. This however requires a peculiar coincidence between the $J=0$ and $J=2$ resonance effects which is likely to be unphysical. In both solutions the $a_0(980)$ resonance appears as a pole on the second Riemann sheet. The location of this pole in the physical solution is determined to be $m-iΓ/2=1000.7^{+12.9}_{-0.7} -i\,36.6^{+12.7}_{-2.6}$ MeV. The solutions are also compared to experimental data in the kinematical region of the decay $η\toπ^0γγ$. In this region an isospin violating contribution associated with $π^+π^-$ rescattering must be added for which we provide a dispersive evaluation.

hep-ph

Meson-baryon Scattering in Extend-on-mass-shell scheme at $\mathcal{O}(p^3)$

In this present work, we study the scattering of a pseudoscalar meson off one ground state octet baryon in covariant baryon chiral perturbation theory up to the next-to-next-to-leading order. We remove the power counting breaking terms with the extended-on-mass-shell scheme. We perform the first combined study of the pion-nucleon and kaon-nucleon scattering data and show that the covariant baryon Chiral perturbation theory can provide a reasonable description of the experimental data for both channels.

hep-ph

Scale Invariance in Heavy Hadron Molecules

We discuss a scenario in which the $P_c(4450)^{+}$ heavy pentaquark is a $Σ_c \bar{D}^*$-$Λ_{c}(2595) \bar{D}$ molecule. The $Λ_{c1} \bar{D} \to Σ_c \bar{D}^*$ transition is mediated by the exchange of a pion almost on the mass shell that generates a long-range $1/r^2$ potential. This is analogous to the effective force that is responsible for the Efimov spectrum in three-boson systems interacting through short-range forces. The equations describing this molecule exhibit approximate scale invariance, which is anomalous and broken by the solutions. If the $1/r^2$ potential is strong enough this symmetry survives in the form of discrete scale invariance, opening the prospect of an Efimov-like geometrical spectrum in two-hadron systems. For a molecular pentaquark with quantum numbers $\frac{3}{2}^{-}$ the attraction is not enough to exhibit discrete scale invariance, but this prospect might very well be realized in a $\frac{1}{2}^{+}$ pentaquark or in other hadron molecules involving transitions between particle channels with opposite intrinsic parity and a pion near the mass shell. A very good candidate is the $Λ_{c}(2595) \barΞ_b - Σ_c \barΞ_b'$ molecule. Independently of this, the $1/r^2$ force is expected to play a very important role in the formation of this type of hadron molecule, which points to the existence of $\frac{1}{2}^{+}$ $Σ_c D^*$-$Λ_{c}(2595) D$ and $1^+$ $Λ_{c}(2595) Ξ_b - Σ_c Ξ_b'$ molecules and $0^{+}$/$1^{-}$ $Λ_{c}(2595) \barΞ_b - Σ_c \barΞ_b'$ baryonia.

hep-ph