Spectroscopy of $A=9$ hyperlithium by the $(e,e^{\prime}K^{+})$ reaction
T. Gogami, C. Chen, D. Kawama, P. Achenbach, A. Ahmidouch, I., Albayrak, D. Androic, A. Asaturyan, R. Asaturyan, O. Ates, P. Baturin, R., Badui, W. Boeglin, J. Bono, E. Brash, P. Carter, A. Chiba, E. Christy, S., Danagoulian, R. De Leo, D. Doi, M. Elaasar, R. Ent, Y. Fujii

TL;DR
This study used the $(e,e^{ extprime}K^{+})$ reaction at Jefferson Lab to perform missing mass spectroscopy on the neutron-rich hypernucleus $^{9}_{ m \Lambda}Li$, revealing its ground state energy and excited states, and comparing results with shell model predictions.
Contribution
First measurement of the energy levels of $^{9}_{ m \Lambda}Li$ using the $(e,e^{ extprime}K^{+})$ reaction, providing new data on hypernuclear structure and cluster configurations.
Findings
Ground state energy $B_{ m \\Lambda}^{ m g.s.}=8.84 \\pm 0.17^{\\rm stat.} \\pm 0.15^{\\rm sys.}~\text{MeV}
Observed excited states at $E_{\\Lambda}({\rm no.~2})=1.74 \\pm 0.27^{\\rm stat.} \\pm 0.11^{\\rm sys.}~\text{MeV}$ and $E_{\\Lambda}({\rm no.~3})=3.30 \\pm 0.24^{\\rm stat.} \\pm 0.11^{\\rm sys.}~\text{MeV}$
The $E_{\\Lambda}({\rm no.~3})$ state suggests a developed ${\rm ^{5}He}+t$ cluster structure.
Abstract
Missing mass spectroscopy with the reaction was performed at Jefferson Laboratory's Hall C for the neutron rich hypernucleus . The ground state energy was obtained to be by using shell model calculations of a cross section ratio and an energy separation of the spin doublet states ( and ). In addition, peaks that are considered to be states of [] and [] were observed at and , respectively. The is larger than shell model predictions by…
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