Bulletin of the American Physical Society
6th Joint Meeting of the APS Division of Nuclear Physics and the Physical Society of Japan
Sunday–Friday, November 26–December 1 2023; Hawaii, the Big Island
Session M01: Challenges in Understanding Exotic Hadrons
2:00 PM–5:00 PM,
Friday, December 1, 2023
Hilton Waikoloa Village
Room: Kona 4
Chair: Kiyoshi Tanida, Japan Atomic Energy Agency
Abstract: M01.00004 : Study of the Lambda(1405) resonance via kaon-induced reactions*
4:15 PM–5:00 PM
Presenter:
Hiroyuki Noumi
Author:
Hiroyuki Noumi
Collaboration:
J-PARC E31 collaboration
We measured πΣ invariant mass spectra below and above the KbarN mass threshold in the K-d -> NπΣ in order to study the KbarN interaction and the Λ(1405) resonance [1]. For this purpose, a negatively-charged kaon (K-) beam of 1 GeV/c was irradiated on a deuterium target at the K1.8BR beam line in the J-PARC Hadron Experimental Facility. In the experiment, a nucleon (N: neutron or proton) knocked out from a deuteron (d) by an incident K- was detected at a very forward angle, and four different final states of π+Σ-, π-Σ+, π0Σ0, and π-Σ0 were identefied by measuring the charged particles emitted around the target.
This reaction can be described by the following two-step process: (i) K-"N1"->KbarN and (ii) Kbar"N2"->πΣ, where "N1" and "N2" are nucleons bound in the deuteron.
Since the nucleon emitted at the forward angle carries away most of the collision energy in (i), the center-of-mass energy in (ii) can be lower, even below the KbarN mass threshold. Since the recoiled kaon is slow down below 250 MeV/c, one expects that the S-wave Kbar"N2"->πΣ scattering is dominant around the KbarN mass region. In order to separate the I=0 and 1 amplitudes in (ii), we demonstrate that an isospin relation of the cross sections between the four final πΣ states is satisfied as π0Σ0 = [π+Σ- + π-Σ+ - π-Σ0]/2.
The scattering amplitudes of step (i) has been well analyzed by Gopal et al. [2]. Employing their amplitudes in step (i), we could deduce the S-wave scattering amplitudes of step (ii): KbarN->KbarN as well as KbarN->πΣ in I = 0 in the framework of the KbarN-πΣ coupled channel by reproducing the πΣ spectrum of the I=0 channel. We find a resonance pole at 1417.7+6.0-7.4(fitting error)+1.1-1.0(systematic error) -i[26.9+6.0-7.9(fitting error)+1.7-2.0(systematic error)] MeV in the deduced KbarN->KbarN amplitude [3].
*The present work was supported by MEXT Grants-in-Aid of Innovative Area No. 21105003, No. 18H05402, and Grants-in-Aid of Scientific Research A No. 16H02188 and S No. 22H04940.
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