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October 14, 2024 to November 15, 2024
YITP
Asia/Tokyo timezone

Higher partial waves in femtoscopy

Oct 21, 2024, 3:30 PM
1h
Panasonic Auditorium, Yukawa Hall (YITP)

Panasonic Auditorium, Yukawa Hall

YITP

1st and 2nd weeks (Hadron structure and interactions) Seminar (1,2 week)

Speaker

Koichi Murase (Tokyo Metropolitan University)

Description

Recently, femtoscopy in high-energy heavy-ion collisions has been gathering attention as a new approach to hadron-hadron interaction, and two-particle momentum correlation is widely measured in experiments [1]. Existing studies have mainly assumed the s-wave interaction, where the contributions from p-wave and d-wave have been neglected for simplicity. However, the correlation function gets contributions from all higher partial waves in general. The effect becomes particularly significant in the presence of resonances of higher partial waves. For example, a peak observed in the $K$-$p$ correlation [2] is attributed to the d-wave resonance $\Lambda(1520)$.

In this talk, we discuss the effect of higher partial waves on the correlation function based on the Koonin-Pratt formula, which gives the correlation function as an integral of the two-particle source $S(\mathbf{r})$ and the relative wave function $\phi^{(-)}_\mathbf{q}(\mathbf{r})$. We first consider the partial-wave expansion of the correlation function under the spherical source, where the correlation is shown to be the sum of the contributions from each wave. We also attempt an extension of the Lednicky–Lyuboshits (LL) formula [3] for the s-wave interaction. Assuming a short interaction range, a Gaussian source, and the effective range expansion of the s-wave scattering amplitude $f_0$, the LL formula gives a parametrized form of the correlation function in terms of the scattering length $a_0$ and the effective range $r_0$. Using similar assumptions, we obtain a generalized LL formula for the higher partial waves. In this procedure, we give an insight into the structure of the LL formula and discuss a relation to the optical theorem. We also check the applicability of the generalized LL formula using typical potentials such as the potential well.

[1] S. Cho et al. [ExHIC], Prog. Part. Nucl. Phys. 95, 279-322 (2017).
[2] S. Acharya et al. [ALICE], Phys. Rev. Lett. 124, no.9, 092301 (2020).
[3] R. Lednicky and V. L. Lyuboshits, Yad. Fiz. 35, 1316-1330 (1981).

Primary author

Koichi Murase (Tokyo Metropolitan University)

Co-author

Tetsuo Hyodo (Tokyo Metropolitan University)

Presentation materials