25–30 May 2025
Daejeon Convention Center (DCC)
Asia/Seoul timezone

Measurement of Hyper-Hydrogen Lambda-Binding Energy via Decay Pion Spectroscopy

29 May 2025, 17:20
15m
Room 5: 1F #102 (DCC)

Room 5: 1F #102

DCC

Contributed Oral Presentation Hadrons in Nuclei Parallel Session

Speaker

Ryoko Kino (Tohoku University)

Description

The hypertriton ($^3_\Lambda$Η) is the lightest Lambda-hypernucleus, consisting of one proton, a neutron, and a Lambda. This simplest Lambda hypernucleus has been an essential benchmark for hypernuclear physics. However, the primary properties, mass and lifetime, still have systematic experimental uncertainties. The Lambda-binding energy ($B_\Lambda$) is reported to be $130\pm50$ keV based on emulsion data summarized by Jurič $et$ $al$.[1]. The shallow binding energy suggests a hypertriton lifetime similar to a free Lambda particle ($\tau_\Lambda = 263$ ps)[2]. The recent heavy ion collision experiments have generated considerable interest. After 2010, the STAR and ALICE collaborations have reported a $20-30$% shorter lifetime than $\tau_\Lambda$[3,4]. Furthermore, there are still significant discrepancies in the $B_\Lambda$ values reported by these two groups, differing by a factor of four[5,6]. Accurate and independent measurement of these values is crucial for understanding the hypertriton’s lifetime and mass simultaneously, making this one of the hot topics in hypernuclear physics the ‘Hypertriton puzzle.’
In October 2022, we conducted decay pion spectroscopy experiments on s-shell hypernuclei at the Mainz Microtron MAMI in Germany. The method was established, and the mass of $^4_\Lambda$H was successfully measured with an accuracy of approximately 80 keV in 2016[7].
To enhance the yield of hypertriton and reduce background events, we selected a 4.5 cm long and 0.75 mm wide Lithium target aligned along the beam direction to increase luminosity[8]. Additionally, a new beam energy measurement technique[9] was introduced to reduce the systematic error of hypernuclear mass to $10-20$ keV.
In this session, I will present this experimental method and provide a new result from the latest analysis.

[1] M. Jurič et al, Nucl. Phys. B 52, 1 (1973) 1-30.
[2] H. Kamada et al., PRC 57, 4 (1998)
[3] STAR collaboration, Science 328 (2010) 58
[4] J. Adam et al., Phys.Lett. B 754 (2016) 360-372
[5] S. Acharya et al., PRL 131(2023), 102302
[6] STAR collaboration, Nature Phys. 16 (2020) 4, 409-412
[7] F. Shultz et al., NPA 954, 149 (2016)
[8] P. Eckert et al., EPJ Web Conf. 271, 01006 (2022)
[9] P. Klag et al., NIM A 910 (2018) 147–156

Primary author

Ryoko Kino (Tohoku University)

Co-authors

Patrick Achenbach (Thomas Jefferson National Accelerator Facility) Pascal Klag (Johannes Gutenberg University Mainz) Satoshi Nue Nakamura (The University of Tokyo, Tohoku University) Sho Nagao (The University of Tokyo) Kotaro Nishi (The University of Tokyo) Josef Pochodzalla (Johannes Gutenberg University Mainz, GSI, Helmholtz Institute Mainz) Tianhao Shao (Fudan University) for the A1 hypernuclear collaboration .

Presentation materials