First Observation of Ground State Dineutron Decay: Be16

Phys. Rev. Lett. 108, 102501
Level and decay scheme for neutron-rich isotopes of beryllium. The solid lines correspond to experimental data from 17, 15, and the present Letter, while the dashed lines represent shell model calculations in the spsdpf model space using the WBP interaction [18].Level and decay scheme for neutron-rich isotopes of beryllium. The solid lines correspond to experimental data from 17, 15, and the present Letter, while the dashed lines represent shell model calculations in the spsdpf model space using the WBP i... Show more

Exotic types of radioactivity have been proposed and searched for with great interest for decades. The simultaneous two-proton decay was proposed by Goldansky [1] for nuclei with an even number of protons beyond the dripline. This 2p decay can proceed either through a simultaneous three-body breakup or through the emission of a diproton system which then breaks up into two protons later in the decay. Two-proton radioactivity was observed for the first time in 2002 [2,3]. Although some evidence for the observation of a diproton has been reported (e.g., [4,5], and most recently in [6]), no clear cases are presently known [7]. Blank and Ploszajczak state in their review, “All experiments performed up to now seem to indicate that the sequential decay prevails, as long as intermediate states for 1p emission are energetically accessible.” In addition, the identification of diproton clusters is difficult, since, even if they could be present inside the nucleus, they may not survive as they penetrate the Coulomb barrier.

In analogy to the proton dripline, dineutron emission could be possible beyond the neutron dripline. The absence of the Coulomb barrier would make the identification easier, as the correlation of the dineutron cluster would be better conserved during the decay. Hansen and Jonson first suggested the presence of a dineutron in the two-neutron halo nucleus Li11 [8]. Charge radii measurements in He8 and He6 indicated that the two halo neutrons in He6 are preferentially located together on one side of the He4 core [9].

Previous measurements of multiple neutron emissions in β-delayed two- and three-neutron radioactivity [10,11] did not measure any neutron correlations, and the decays most likely proceed sequentially via intermediate states, similar to the proton emitters. An ideal case for searching for dineutron decay is an unbound nucleus for which the single-neutron emission is greatly suppressed. This is the case for nuclei beyond the neutron dripline where a nucleus is bound with respect to single-neutron emission but unbound with respect to two-neutron emission. Two such nuclei, H5 and He10 [12,13], have been studied, and some evidence for a dineutron component has been observed in He10 [13]. In both cases, the intermediate unbound systems ( H4 and H9e) have broad resonances which can extend below the single-neutron emission threshold, thus favoring the sequential decay.

A nucleus predicted to be bound with respect to one-neutron emission but unbound with respect to two-neutron emission is Be16. It was shown to be unbound in a recent Ar40 fragmentation experiment [14]; however, nothing else is known about Be16. Shell model calculations [15] predict the one- and two-neutron separation energies to be +1.8MeV and -0.9MeV, respectively. Mass extrapolations from the Atomic Mass Evaluation 2003 [16] assign corresponding values of +0.2(7)MeV and -1.6(5)MeV. The intermediate system, Be15, was found to be unbound by more than 1.54 MeV in our previous work [15], in agreement with shell model calculations. Knowing the location of the intermediate system, even as a lower limit, is important for characterizing the 2n-unbound Be16. The level and decay schemes for neutron-rich beryllium isotopes are shown in Fig. 1. Sequential two-neutron emission from Be16 is expected to be suppressed, since the ground state of Be15 is a narrow resonance at a significantly higher energy. This makes Be16 an ideal candidate for the search of dineutron decay. In the present Letter, we report on the first observation of this exotic decay in Be16.

A single-proton knockout reaction from a B17 beam was used to populate Be16. Knockout reactions have been shown to be a powerful tool for studying the structure of exotic nuclei at these energies [19]. Knowing the configuration of the initial beam-nucleus ground state, as well as that of the final state, can help with understanding the observed decay. In the case of a two-neutron decay, the energy and structure of the intermediate system is also important. In this case, the beam nucleus B17 is known to have a significant mixing of the ν(2s1/2) and ν(1d5/2) configurations [20–22], which provides evidence for a two-neutron halo structure. Be16 is therefore expected to be populated with a similar neutron configuration. The picture is similar for the final nucleus Be14, with a known two-neutron halo structure; however, it is more complicated due to the fact that its ground state probably has components from the coupling of s, p, and d neutrons, with not only a Be12(0+) core but also with an excited Be12(2+) core [23,24]. Be14 has no bound excited states, and therefore any Be14 events observed in our experiment correspond to its ground state. The goal of the experiment was to populate the 0+ ground state of Be16 and reconstruct its decay into Be14 and two neutrons.

The experiment was performed at the National Superconducting Cyclotron Laboratory, at Michigan State University. A 120MeV/u Ne22 primary beam impinged on a 2938mg/cm2 Be target to produce the secondary B17 beam at 53MeV/u. The B17 beam was selected through the A1900 fragment separator [25] with the use of a 1050mg/cm2 Al achromatic degrader at its intermediate focal plane. The average total secondary beam intensity was 250 pps, of which 75% corresponded to the isotope of interest, B17. The other main beam component was C19, together with some additional light fragments that were produced in the Al degrader. The different components of the beam were separated by time of flight. Less than 0.1% contamination from the C19 beam component was present in the B17 beam gate.

(a) Three-body decay energy from the reconstruction of Be14+n+n. (b),(c) Two-body decay energy of Be14+n, where (b) corresponds to the highest decay energy and (c) to the lowest. (d) Two-body relative energy of the two neutrons. (e) Opening angle θnn between the two neutrons in the center-of-mass frame of Be16. (f) Opening angle (θBe14n1) between the Be14 fragment and the first neutron in the center-of-mass frame of Be16. In all figures, the experimental data are shown in black triangles, the sequential emission in dotted lines, the three-body decay in dashed lines, and the dineutron decay in solid lines.(a) Three-body decay energy from the reconstruction of Be14+n+n. (b),(c) Two-body decay energy of Be14+n, where (b) corresponds to the highest decay energy and (c) to the lowest. (d) Two-body relative energy of the two neutrons. (e) Opening angle θn−... Show more

The Be16 nucleus of interest was populated via a one-proton knockout reaction from the B17 beam interacting with a 470mg/cm2 beryllium target. The unbound Be16 was reconstructed from the products of its decay, Be14 and two neutrons. The charged fragment was bent 43° by the Sweeper dipole magnet [26] and was detected in a suite of position- and energy-sensitive detectors. The neutrons were detected by the Modular Neutron Array (MoNA) [14], located 7.9 m downstream from the target location, centered on the beam axis.

For the reconstruction of the Be16 decay, we identified events where Be14 was in coincidence with two neutrons in MoNA. In order to remove cross talk events (events where a single neutron interacts twice in MoNA) and enhance the two-neutron signature, the 144 plastic scintillator bars were arranged in four separate walls, all centered along the beam axis. Each wall was 160 cm in height (16 detector bars). Three walls were 20 cm thick (2 layers of detectors, with 100 cm space between walls), while the last wall was 30 cm thick (3 layers of detectors, placed with 80 cm space to the previous wall). This geometry allowed for larger distances between the neutron interactions and improved the resolution for measuring the velocity between interaction points. The selection of two-neutron events was done by including the following conditions in the analysis [27]: A cut was applied for selecting events where the distance between the first and second hit had to be larger than 50 cm. A second cut required the time difference between the first and second hits in the detector to be shorter than the time it would take a beam-velocity neutron to travel between their respective interaction points.

The effectiveness of the cuts was tested using reactions where only one neutron was expected in the data. This was done with events from the single-proton knockout reaction from the C19 component of the secondary beam. This reaction populates B18, which decays by single-neutron emission to B17 [28]. The number of single-neutron events from the B18 decay that survived the 2n conditions was 3.2(2)% of the total events. Based on this calculation and assuming a similar cross section for the population of Be15 and Be16 from B17 [29,30], we estimate that there is less than a 10% contribution of single-neutron events from Be15Be14+n in our 2n selection. It should also be noted that the contribution of 1n events from the Be15 breakup counted as 2n events will add to the decay energy spectrum in the region above 3 MeV because the single neutron that is being counted twice corresponds to a decay above 1.5 MeV.

Figure 2 shows the experimental results (black triangles) compared to three different decay models produced in Monte Carlo simulations. The simulation package included the geometry and resolution of all detectors involved in the experiment, the map of the magnetic field, and the reaction and decay mechanisms. The neutron interactions in MoNA were simulated in GEANT4 [31] using the physics class MENATE_R [32], which was found to provide excellent agreement with the experimental observables. The three decay models used in the simulations which are presented in Fig. 2 were the following. (1) Represented by dotted lines is a sequential emission of the two neutrons assuming that the decay proceeds through a broad state in the intermediate system Be15 [33]. A decay through the 3/2+ and 5/2+ states has to be a d wave, and, because they are much higher in energy than the Be16 ground state, this type of sequential decay is not possible. The only possible contribution from a sequential decay is through the high-lying 1/2+ state in Be15. This state could correspond to a broad s wave, which can extend lower in energy than Be16 and allow for a sequential decay. (2) Represented by dashed lines is a simultaneous emission of the two neutrons via a three-body breakup where the initial state breaks up into a Be14 and two neutrons [34]. This breakup model represents the extreme limit of a three-body decay and includes no interactions between the three particles. (3) Represented by solid lines is a dineutron decay. In this case, the two neutrons are emitted together and the dineutron breaks up immediately after its emission. The dineutron breakup is modeled using an s-wave line shape [35] based on its known scattering length of -18.7±0.7fm [36] and pairing energy of 0.87 MeV [37]. In all three cases, the initial state was simulated as a Breit-Wigner line shape.

As shown in Fig. 2, the (a) three-body and (b),(c) individual two-body decay energy spectra are not sensitive to the decay mode. All three decay modes could fit the experimental data satisfactorily. However, the sequential and three-body breakup modes of decay deviate significantly from the data for the two-neutron correlation parameters. This can be seen in Fig. 2(d), which shows the relative energy of the two neutrons, as well as in Fig. 2(e), which presents the opening angle between the two neutrons in the Be16 center-of-mass frame. In particular, in the latter figure, the up-bend of the data at small opening angles ( cosθn-n1) can only be reproduced by the dineutron decay mode. We also looked for correlations between the two neutrons and the Be14 fragment. Figure 2(f) shows the angle between Be14 and the first of the two neutrons [ cos(θBe14-n1)]. Once again, the dineutron decay fits the experimental data much better than the other decay modes. These comparisons show clearly that the dominant contribution in the decay of Be16 is through the emission of a dineutron. Apart from the decay mechanism, the only free parameters in our simulation were the location and width of the initial state. We performed a χ2 minimization analysis, and the best fit to the experimental data corresponded to a two-neutron separation energy for Be16 of 1.35(10) MeV with a width of 0.8-0.2+0.1MeV.

Shell model calculations were performed in the s-p-sd-pf model space with the WBP Hamiltonian [18] using the code NuShell [38]. The results of the calculations are shown in Fig. 1. The calculated two-neutron separation energy for Be16 is 0.9 MeV, in reasonable agreement with the experimental result at 1.35(10) MeV and within the uncertainty of the calculations (330 keV). The ground state of Be16 is expected to be populated from a B17 beam via the removal of a p3/2 proton with a spectroscopic factor, C2S=0.4. The two-nucleon transfer amplitudes (TNAs) for Be16 to Be14 obtained with WBP are 0.90, 0.33, and 0.34 for (d5/2)2, (d3/2)2, and (s1/2)2, respectively. Following the formalism used for diproton decay [39], the dineutron spectroscopic factor is S=(16/14)4(0.461)2=0.36, where all three of the TNAs contribute. The full three-body phase space for two-proton decay has been calculated by Grigorenko et al. [40,41] for pure shell model configurations. When rates from these full three-body calculations are combined with the shell model TNA values, good agreement for the experimental decay width of Zn54 was obtained [42], but the observed angular correlations are not yet fully understood. Three-body calculations for two-neutron decay with constraints to the expected shell model wave functions remain to be carried out.

Because of the absence of an angular momentum barrier, the dominant component is expected to be the s wave. However, a three-body virtual state can be presented as a relatively sharp resonance in contrast to the two-body virtual state [43]. In this case, the initial state can have a measurable width, despite its s-wave character. The shape of the initial state is most probably not the same as a standard resonance. Because of the experimental resolutions, our results are not sensitive to small changes in the shape of the decay, and, for this reason, a Breit-Wigner line shape was used in our analysis.

In summary, we report on the first observation of the dineutron decay in the unbound nucleus Be16. Be16 was populated via a single-proton knockout reaction from B17. The Be16 decay was reconstructed event-by-event from the decay products Be14+n+n. The present observation of a dineutron decay confirms the models that predict dineutron clusters inside neutron-rich nuclei. The dineutron decay reported in the present Letter is indicative of such a structure in the original nucleus B17, a known two-neutron halo.


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About the Authors

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Image of A. Volya

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