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J. Esmaili

Publications and source records attributed to J. Esmaili.

3 recordsLinked to original sources

Trace of $Λ(1405)$ resonance in low energy $K^{-}+\, ^{3}\mathrm{He}\rightarrow (π^{0}Σ^{0})+d$ reaction

In present work, we investigated $K^{-}+\, ^{3}\mathrm{He}$ reaction at low energies. The coupled-channel Faddeev AGS equations were solved for $\bar{K}Nd-πΣ{d}$ three-body system in momentum representation to extract the scattering amplitudes. To trace the signature of the $Λ$(1405) resonance in the $πΣ$ invariant mass, the deuteron energy spectrum for $K^{-}+\,^{3}\mathrm{He}\rightarrowπΣ{d}$ reaction was obtained. Different types of $\bar{K}N-πΣ$ potentials based on phenomenological and chiral SU(3) approaches were used. As a remarkable result of this investigation, it was found that the deuteron energy spectrum, reflecting the $Λ$(1405) mass distribution and width, depends quite sensitively on the $\bar{K}N-πΣ$ model of interaction. Hence accurate measurements of the $πΣ$ mass distribution have the potential to discriminate between possible mechanisms at work in the formation of the $Λ$(1405).

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Structure, formation and decay of $\bar{K}NN$ system by Faddeev-AGS calculations

The Faddeev AGS equations are solved for coupled-channels $\bar{K}NN-πΣ{N}$ system with quantum numbers $I=1/2$ and $S=0$. Using separable potentials for $\bar{K}N-πΣ$ interaction, we have calculated the transition probability for the $(Y_{K})_{I=0}+N\rightarrowπΣ{N}$ reaction. The possibility to observe the trace of $K^{-}pp$ quasi-bound state in the $πΣ{N}$ mass spectra was studied. Various types of chiral based and phenomenological potentials are used to describe the $\bar{K}N-πΣ$ interaction. It was shown that not only we can see the signature of the $K^{-}pp$ quasi-bound state in the mass spectra, but also, one can see the trace of branch points in the observables.

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Resonant formation of Lambda(1405) by stopped-K- absorption in deuteron

To solve the current debate on the position of the quasi-bound K^-p state, namely, "Lambda(1405) or Lambda*(1420)", we propose to measure the T_{21} = T_{Sigma-pi \leftarrow Kbar-N} Sigma-pi invariant-mass spectrum in stopped-K- absorption in deuteron, since the spectrum, reflecting the soft and hard deuteron momentum distribution, is expected to have a narrow quasi-free component with an upper edge of M = 1430 MeV/c^2, followed by a significant "high-momentum" tail toward the lower mass region, where a resonant formation of Lambda(1405) of any mass and width in a wide range is revealed. We introduce a "deviation" spectrum as defined by DEV = OBS (observed or calculated) / QF (non-resonant quasi-free), in which the resonant component can be seen as an isolated peak free from the QF shape.

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