Physics Letters B 790 (2019) 502–508
Contents lists available at ScienceDirect
Physics Letters B
www.elsevier.com/locate/physletb
Has the neutral double hypernucleus
4
n been observed?
Sebastian Bleser
a
, Michael Bölting
a
, Theodoros Gaitanos
b
, Josef Pochodzalla
a,c,∗
,
Falk Schupp
a
, Marcell Steinen
a
a
Helmholtz Institute Mainz, Johannes Gutenberg University, 55099 Mainz, Germany
b
Aristotle University of Thessaloniki, 54124 Thessaloníki, Greece
c
Institute for Nuclear Physics, Johannes Gutenberg University, 55099 Mainz, Germany
a r t i c l e i n f o a b s t r a c t
Article history:
Received
16 November 2018
Received
in revised form 9 January 2019
Accepted
25 January 2019
Available
online 30 January 2019
Editor:
V. Metag
Keywords:
Hypernuclei
Statistical
decay model
The BNL-AGS E906 experiment was the first fully electronic experiment to produce and study double
hypernuclei with large statistics. Two dominant structures were observed in the correlated π
−
–π
−
momentum matrix at (p
π−H
, p
π−L
) = (133, 114) MeV/c and at (114, 104) MeV/c. In this work we argue
that the interpretation of the structure at (133, 114) MeV/c in terms of
3
H+
4
H pairs is questionable. We
show, that neither a scenario where these single- hypernuclei are produced after capture of a stopped
−
by a
9
Be nucleus nor interactions of energetic
−
with
9
Be nuclei in the target material can produce
a sufficient amount of such twin pairs. We have therefore explored the conjecture of Avraham Gal that
decays of the
4
nmay be responsible for the observed structure. Indeed, the inclusion of
4
nwith a
two-body π
−
branching ratio of 50% in a statistical multifragmentation model allows to describe the
E906 data remarkably well. On the other hand, a bound
3
n nucleus would cause a striking structure in
the momentum correlation matrix which is clearly inconsistent with the observation of E906.
© 2019 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license
(http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP
3
.
1. Introduction
Recently, a candidate for a weakly unbound resonant tetraneu-
tron
was observed in the missing-mass spectrum measured in the
double-charge-exchange reaction
4
He(
8
He,
8
Be) at the Radioactive
Isotope Beam Factory of RIKEN [1]. Prior to this experiment, first
positive indications of such a nucleus were found in 2002 at GANIL
employing the breakup of
14
Be nuclei [2]. In the hypernuclear
sector, the HypHI Collaboration investigated peripheral
6
Li+
12
C in-
teractions
at GSI and found intriguing enhancements in the d+π
−
and t+π
−
invariant mass. These enhancements were interpreted as
weak decays of neutral
3
n hypernuclei [3].
From
the theoretical point of view, the tetraneutron is rather
controversial. Several theoretical models exclude the existence of a
bound or narrow resonant tetraneutron [4–8]. On the other side,
calculations of Lashko and Filippov [9], Shirokov et al. [10,11]as
well as Gandolfi et al. [12] support a slightly unbound tetraneutron
with a resonance energy in agreement with the RIKEN measure-
ment.
In the case of the neutral
3
n hypernucleus, the theoretical
*
Corresponding author at: Helmholtz Institute Mainz, Johannes Gutenberg Uni-
versity,
55099 Mainz, Germany.
E-mail
address: pochodza@uni-mainz.de (J. Pochodzalla).
URL: https://www
.hi-mainz.de (J. Pochodzalla).
position is clear: based on our present understanding of strange
nuclei, this nucleus should not be bound [13–17].
In
view of this challenging situation – experimentally as well
as theoretically – it is surely justified to explore the possibility
of other bound or resonant neutral baryonic systems as well. Of
particular interest are nuclear systems with two hyperons. The
onset of binding in light double -hypernuclei has a consider-
able
impact on our understanding of three-body forces in dense
baryonic matter. For charged double hypernuclei, the theoretical
situation is unclear for the A = 4
4
H nucleus [18–21], but bind-
ing
is expected to definitely set in for A = 5 double hypernuclei
[22–24]. Unfortunately, there is no consensus about the stability
with respect to either the n [25–27] nucleus or the
4
nnu-
cleus
[17,28,29].
In
this work we reconsider data taken by the AGS-E906 exper-
iment
which searched for double hypernuclei via their sequential
pionic decay [30]. Studying different production scenarios, we find
hints for a bound
4
nsystem.
2. The E906 puzzle
In 2001, the AGS-E885/E906 collaboration announced the first
‘mass production’ of about 30
4
Hevents based on ∼10
4
stopped
−
[30]. The -hypernuclei are identified through the sequential
weak decay via π
−
emission after a (K
−
, K
+
) reaction deposited
https://doi.org/10.1016/j.physletb.2019.01.047
0370-2693/
© 2019 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by
SCOAP
3
.