The Synthesis of New Neutron-Rich Heavy Nuclei

Introduction

All known isotopes of the elements Fm through Og are neutron deficient relative to β-stability. While there is some dispute as to the next proton magic number beyond 82 (with proponents of Z = 114, 120, and 126) [1] there is little doubt that the next neutron magic number beyond N = 126 is N = 184. A clear-cut path to reach N = 184 is not evident although one is encouraged by recent efforts that have reached N = 177.

Two synthetic paths to making more neutron-rich super-heavy nuclei, the use of radioactive nuclear beams (RNBs) and the use of multi-nucleon transfer (MNT) reactions, seem to have emerged as the best approaches. The central issue for the use of RNBs for making new n-rich heavy nuclei is the available fluxes of n-rich projectiles [2, 3]. The central issue for the use of MNT reactions to make new neutron-rich heavy nuclei is to understand the MNT processes well enough to justify vigorous experimental efforts.

There have been several papers dealing with these issues. Loveland has treated the use of RNBs to synthesize new n-rich heavy nuclei [2, 3]. He concluded that RNBs are not useful for making the heaviest nuclei, but that there is a “window of opportunity” for making n-rich isotopes of elements 103–107 using FRIB. Wakhle et al. studied the reaction ^{39, 46}K + ¹⁸¹Ta [4] and concluded that Bh and Hs isotopes might be produced at rates ~0.1 atom/day at FRIB. Mun et al. [5] concluded that the radioactive beams of ^{66, 68, 70}Ni reacting with ²³⁸U do not provide any advantage in producing neutron-rich isotopes of Md due to low beam intensities and reduced complete fusion cross sections. Zhu et al. concluded that the use of the RNB ¹⁴⁴Xe [6] could lead to increased production cross sections for heavy n-rich nuclei although the issue of production rates was not addressed. Zhu et al. [7] did conclude that ¹⁴⁴Xe could be used to produce neutron-rich nuclei with Z < Z_target. This conclusion is based on estimating [8] that ¹⁴⁴Xe beam intensities at SPIRAL2 of >10⁸ p/s will be available. It was suggested that these ¹⁴⁴Xe beams would be most effective in producing nuclei near the neutron closed shell N = 126. Zhang et al. [9] concluded that ¹⁴⁵Xe + ²⁰⁸Pb reactions could be used to produce unknown isotopes of Pt (^209−212Pt) based upon similar estimates [8] of the intensities of ¹⁴⁵Xe beams at SPIRAL2. Li et al. [10] have pointed out the possibility of using ²²O in the ²²O + ²⁴⁴Pu reaction to make ^259−263No.

Most of the interest in making new n-rich heavy nuclei has centered on the use of MNT reactions with stable beams. In experiments at GSI and LBNL [11–16], several studies were made of the possibilities of using MNT reactions to make new heavy nuclei. [A review of these data is found in [17]]. Production of n-rich trans-target nuclides up to Fm and Md was observed with cross sections of ~0.1 μb. The basic problem was that the higher excitation energies that led to broader distributions of the trans-target nuclei caused the highly excited nuclei to fission, thereby restricting the use of these reactions to produce new n-rich heavy nuclei. Zagrebaev and Greiner [18–20] suggested that if MNT reactions were run near the barrier [~1.1V_b [21]] shell effects would be preserved and large transfers would occur. For the reaction of ²³⁸U with ²⁴⁸Cm at 1.1 V_b, they predicted a net transfer of 30 nucleons from ²³⁸U to ²⁴⁸Cm. The same calculational model when applied to the reaction of E_c.m. = 750 MeV ²³⁸U + ²⁴⁸Cm reproduced the previous measurements of Schadel et al. [14] and predicted the formation, at picobarn levels, of new n-rich isotopes of Sg.

RNBs

Why does one want to use RNBs for producing new n-rich heavy nuclei? Neutron-rich RNBs lead to the formation of more n-rich products. These n-rich heavy nuclei have longer half-lives enabling more detailed atomic physics and chemistry studies. In Figure 1 [taken from [24]] I show the dependence of the half-life (t_1/2) upon neutron number N for some typical even-even (e-e) heavy nuclei with 104 ≤ Z ≤ 120. One can see that the predicted half-lives increase logarithmatically with increasing neutron number showing maximum values for N = 184. The lowered fusion barrier found with n-rich RNB projectiles (compared to stable beams) allows the formation of evaporation residues (ERs) at lower excitation energies. Finally such n-rich reaction products will have higher survival probabilities.

FIGURE 1

Figure 1. The predicted [22, 23] half-lives of even-even heavy nuclei vs. their neutron number.

A simple example should suffice to demonstrate these effects. Consider the reaction of stable ³²S with ²⁰⁸Pb and radioactive ³⁸S with ²⁰⁸Pb. The nominal compound nuclei are ²⁴⁰Cf and ²⁴⁶Cf formed at excitation energies of 43.6 and 22.7 MeV, respectively (assuming the reactions are carried out at the interaction barriers of 149.4 and 133.3 MeV). The predicted ratio of the two evaporation residue production cross sections (σ₃₈/σ₃₂) is 8.2 × 10⁴, i.e., the radioactive beam reaction has an associated production cross section that is five orders of magnitude greater than the stable beam reaction. The product of the ²⁰⁸Pb(³²S, 4n) reaction, ²³⁶Cf, is estimated [23] to have a t_1/2 of 9.4 s, while the product of the ²⁰⁸Pb(³⁸S, 2n) reaction, ²⁴⁴Cf, is known to have t_1/2 = 19.4 m. The longer t_1/2 of the ²⁴⁴Cf can be important when one is studying the chemistry and atomic physics of these nuclei.

RNBs are used primarily in the synthesis of n-rich heavy nuclei using complete fusion reactions. For these reactions the cross section for producing a heavy evaporation residue can be written as a non-separable product of three factors, which express the capture cross section, σ_capture, the fusion probability, P_CN, and the survival probability, W_sur. This equation is

$\begin{array}{r}{\sigma }_{EVR}(E)={\displaystyle \sum _{l=0}^{\infty }}{\sigma }_{Capture}(E,l)P_{CN}(E,l)W_{sur}(E,l)\end{array}$

where σ_capture(E, |) is the capture cross section at center of mass energy E and spin l|. P_CN is the probability that the projectile-target system will evolve from the contact configuration to inside the fission saddle point to form a completely fused system. W_sur is the probability that the completely fused system will de-excite by neutron emission rather than fission.

Loveland [25] has evaluated the capture cross sections relevant for heavy element synthesis and finds that the capture cross sections are known to within a factor of two. There is a well-established formalism to calculate the survival probabilities, where the principal uncertainty is the values of the fission barrier heights used in these calculations. Loveland [25] concluded that W_sur is known within a factor 3. In the same paper, Loveland concluded that P_CN is known within an order of magnitude.

We can apply this knowledge about heavy element complete fusion cross sections to the problem of making new heavy nuclei with radioactive beams. The calculational framework is a brute force technique [2] in which one starts with the projected RNB intensities at various radioactive beam facilities and then considers all possible combinations of a radioactive projectile with a “stable” target nucleus. One varies the projectile energy and evaluates σ_EVR. Upon making a reasonable assumption about the target thickness (0.5 mg/cm²), one can evaluate the product yield in atoms/day.

Sources of information about possible radioactive beam intensities have to be carefully examined. The US FRIB project has a website¹ giving the current best estimates of the radioactive beams available at this facility. At this Projectile Fragmentation facility one has to be careful to distinguish between the fast fragmentation beams and the re-accelerated beams—which are the relevant beams for complete fusion reactions at near barrier energies. Older information about SPIRAL2 can be found [8]. RNB intensities at the ISAC2 facility are available². The US considered a “concept design” of a RNB facility, RIA, which had unrealistically high estimates of possible beam intensities. In a similar vein, the use of exotic target nuclei, like ²⁵⁰Cm needs to be carefully and critically evaluated.

Stable beams are available at intensities of ~3-6 x 10¹² p/s while radioactive beam intensities are substantially less (by 4 orders of magnitude or more). Consequently the heavy element production rates using radioactive beams are usually 3 orders of magnitude less than those achieved with stable beams. Radioactive beams are not a pathway to new superheavy elements (Z > 118).

Does this mean that RNBs are useless in synthesizing new n-rich heavy nuclei? No, there are “windows of opportunity” for making new n-rich isotopes of elements 104–107 [25]. These reactions generally involve high intensity light beams, like O, Ne, Mg, etc. reacting with n-rich heavy targets.

In making these estimates, one must be aware that new technical developments might result in new opportunities for the synthesis of new n-rich heavy nuclei.

What is the future of these efforts to use n-rich RNBs for heavy element synthesis? There are some efforts to develop the use of beams like ⁴⁶K at existing facilities like ReA3 to test how well our established formalisms predict the outcome of relevant complete fusion cross section measurements. Wakhle et al. [4] studied the near-barrier fusion of stable ³⁹K and radioactive ⁴⁶K with ¹⁸¹Ta. They found enhanced capture cross sections with the ⁴⁶K projectile compared to the stable ³⁹K. The authors took their results and extrapolated them to the ^{46, 47, 48}K + ²²⁶Ra and ²²⁷Ac reactions. Using current estimates of FRIB beam intensities¹, they predicted production rates of n-rich isotopes of Bh and Hs to be ~0.1 atoms/day. Future experiments with the ReA6 accelerator (where beams of RNBs at 6 A MeV might be available) may lead to “real” syntheses of n-rich heavy nuclei. Li et al. [10] have shown that the use of light RNBs like ²²O can lead to favorable situations for the synthesis of new n-rich isotopes of No.

MNT Reactions-General

As mentioned previously, MNT reactions are thought to be a pathway to new n-rich heavy nuclei with Z ≤ 118. The initial investigations of these reactions at GSI and LBNL [11–16] were not very promising, but recent calculations of Zagrebaev and Greiner [18–20] have invigorated research in this area. However, these reactions are difficult to study because of the low intensities of the heavy beams used in these reactions, the predicted low cross sections for these reactions (pb-nb) and the difficulty of detecting the most n-rich products, which are β-emitters. [A recent review article summarizes the situation [26]].

There have been several new initiatives involving MNT reactions to make n-rich nuclei. To begin with, there is a long-standing program to use MNT reactions to make nuclei for nuclear spectroscopy [27–32]. More recently there has been interest in using MNT reactions to make nuclei near the N = 126 neutron shell closure (to study r-process nucleosynthesis). This effort has culminated in a large project at the Argonne National Laboratory, the N = 126 factory. In the N = 126 factory, an intense beam (5 pmA) of 9 A MeV ¹³⁶Xe is used to bombard a rotating ¹⁹⁸Pt target. The recoiling reaction products are stopped in a gas catcher, mass separated and transferred to nuclear spectroscopy stations for further study. In addition to this project, there have been a number of studies focused on the yields of N = 126 products in MNT reactions [7, 20, 33–39] (Zhu, Personal communication). A central issue has emerged from these studies, i.e., what are the optimum strategies for making N = 126 isotones in MNT reactions? Should one focus on the grazing collisions where the transfer products are emitted at the grazing angle for reactions like ¹³⁶Xe + ¹⁹⁸Pt or should one look at near central collisions where the products are emitted near 0°? Experiments are underway to address this issue directly for the ¹³⁶Xe + ¹⁹⁸Pt reaction (Zhu, Personal communication). Zagrebaev and Greiner have clearly stated [20] that the relevant collisions for producing heavy n-rich transfer products are the near central (deep inelastic) collisions (DIC). Karpov and Saiko [37] reinforce this conclusion stating “At lower near-barrier energies, even central collisions lead to low excitation energies of primary products.” This suggestion to look for interesting transfer products at small angles has been reinforced by recent experiments at the velocity filter SHIP [34, 40] where transfer products from the ^{58, 64}Ni + ²⁰⁷Pb reaction were observed at angles of 0–2°. However, a recent radiochemical study [41] of the ⁴⁸Ca + ²⁴⁸Cm reaction at a beam energy of 10% above the Coulomb barrier showed the angular distributions of the Fm isotopes (ΔZ = +4) were peaked close to the laboratory grazing angle of 27°.

A process related to multi-nucleon transfer is the quasifission process, described in depth by Hinde et al. [42]. Quasifission bridges the gap between multi-nucleon transfer reactions where the colliding nuclei come into sufficiently close contact to exchange nucleons without altering their average mass and the fusion process where the reacting nuclei lose their identity by amalgamating into a compound nucleus. Quasifission processes occur over time scales of 1–10 zs [43] while MNT processes occur on a more rapid time scale.

MNT Reactions-Experiments

It is important that we test the various models for MNT reactions, to evaluate their utility in planning future experiments and to gain a correct understanding of how MNT reactions work. There are five competing models or theoretical approaches for describing MNT reactions, the GRAZING model [44–46], the di-nuclear systems model (DNS)³ [6, 7, 10, 38, 47–53], the Improved Quantum Molecular Dynamics model (ImQMD) [54–57], the Langevin approach of Zagrebaev and Greiner [18], and Karpov and Saito [37] and the time-dependent Hartree-Fock model (TDHF) [58, 59] and hybrids of these models.

We have focused our experimental efforts [35, 60, 61] on gross tests of these models where we measure the yields of various MNT products and compare our observations with model predictions. The systems we have studied are 5.46 A MeV ¹³⁶Xe + ²⁰⁸Pb, 6.67 A MeV ²⁰⁴Hg + ¹⁹⁸Pt, and 5.9 A MeV ¹³⁶Xe + ¹⁹⁸Pt. These studies have been done at projectile energies ranging from 1.06 to 1.16 V_B, consistent with the idea of preserving shell effects in these collisions.

Barrett et al. [35] reported the measurement of the yields of 235 PLFs and TLFs for the reaction of E_c.m. = 450 MeV ¹³⁶Xe + ²⁰⁸Pb. The experiment was done at the Gammasphere facility of the Argonne National Laboratory and utilized thick target measurements of product nuclides measured in beam and post-irradiation. This extensive data set (76 TLFs and 159 PLFs and fission fragments) of fragment yields for this reaction has served as a testing ground for models of multinucleon transfer reactions at near barrier energies.

Before doing that comparison, some general conclusions can be drawn from Barrett et al. [35] and other similar studies [33, 34, 62–65]. They are;

(a) The more n-rich the projectile, the more n-rich the TLFs are [35, 40, 62]

(b) The greater the projectile energy for a given reaction, the higher the yields of the n-rich transfer products [35, 65].

(c) N = 126 TLFs ranging from Tl to Ra (ΔZ = −1 to ΔZ = +6) are made in the 64Ni + 207, 208Pb reactions [40, 62]

Barrett et al. [35] found that a comparison of their measured PLF and TLF yields for the ¹³⁶Xe + ²⁰⁸Pb reaction with the predictions of the semi-classical GRAZING model³ showed that the GRAZING model predictions are adequate for describing then yields of near projectile and near target species, but they grossly underestimate (by orders of magnitude) the yields of all other products. GRAZING is not a model for large proton transfers. For the production of N = 126 nuclei, GRAZING overestimates the yields of the neutron deficient nuclei but grossly underestimates the yields of the products resulting from large proton transfers.

Zagrebaev and Greiner have suggested an alternate formalism [18–20, 36, 66] for predicting the yields of MNT reactions at near barrier energies (E _c.m. = 1.0–1.2 V_B). The predictions of Zagrebaev and Greiner when applied to the ¹³⁶Xe + ²⁰⁸Pb reaction correctly describe the magnitude and maxima of the observed [35] TLF transfer cross sections for a wide range of transfers (ΔZ = −8 to ΔZ = +2). For (ΔZ = +4), the measured TLF yields are four orders of magnitude higher than the predicted maxima.

An extension or generalization of the Langevin approach of Zagrebaev and Greiner [19, 20, 36, 66] to predicting the outcome of MNT reactions is found in the work of Karpov and Saiko [37]. These authors treat the reaction of ¹³⁶Xe + ²⁰⁹Bi [E_c.m. = 569,684.and 861 MeV [67–69]], the reaction of ¹³⁶Xe + ²⁰⁸Pb [E_c.m. = 450 [35], 526 and 617 MeV [65]], and the reaction of ¹³⁶Xe + ¹⁹⁸Pt [E_c.m. = 643 MeV [59]]. These authors conclude that the production yields of neutron-rich nuclei with N = 126 depend weakly on the incident energy (see discussion below, however, about the ¹³⁶Xe + ¹⁹⁸Pt reaction). As mentioned earlier, they calculate the angular distributions of the MNT products finding the distributions are peaked at the grazing angle for larger energies but are more forward peaked for near barrier collision energies. The calculated and measured total kinetic energy losses, angular and charge distributions are in reasonable agreement for the ¹³⁶Xe + ²⁰⁹Bi reaction. For the ¹³⁶Xe + ²⁰⁸Pb reaction at E_c.m. = 450 MeV, the Karpov and Saiko calculations are in better agreement with the data [35] for the neutron-deficient TLFs and PLFs but seriously overestimate the yields of the most n-rich products.

Three groups [6, 38, 50] use the DNS model to predict the yields of the MNT products in the ¹³⁶Xe + ²⁰⁸Pb reaction. In the work of [6], the yields of the proton pickup products (Tl, Hg, Au, and Pt) are reasonably well described, but the calculations of yields of the trans-target nuclei (Bi, Po, At, and Rn) underestimate the measured cross sections. In the work of [38], the proton pickup product yields are reasonably described with the exception of Au as are the yields of the trans-target nuclides Bi and Po but the yields of the larger transfers leading to the production of At and Rn are underestimated. In the work of Wen et al. [50], a hybrid of the GRAZING and DNS models is used to predict the yields of the MNT products from the ¹³⁶Xe + ²⁰⁸Pb reaction. The implication is that the small transfers are the result of grazing collisions while the larger transfers are the result of more central collisions.

The GRAZING, DNS, and ImQMD models were used by [48] to study the ¹³⁶Xe + ²⁰⁸Pb reaction. Excellent fits to the transfer product data for nuclides ranging from Pt (ΔZ = −4) to At (ΔZ = +3) although the predicted ImQMD distributions are broader than the observed distributions. In these multi-component fits the ImQMD model does the best job of reproducing the observations over a wide range of products.

Another class of models for studying MNT reactions are the time-dependent Hartree-Fock (TDHF) calculations [70–74]. TDHF calculations offer a fully microscopic description of the MNT processes with minimum assumptions on the dynamics. As such, they are free of many of the assumptions used in other models. TDHF theory is expected to be able to describe transfer mechanisms operating at various impact parameters in a unified way.

Sekizawa et al. [70–73] have studied the use of TDHF calculations to describe MNT reactions in a variety of systems. Comparison of the calculations with measured cross sections shows the TDHF calculations describe the cross sections for few nucleon transfers (|ΔZ| ≤ 2) adequately, but as the number of transferred nucleons increases, the agreement gets worse. These workers have shown the importance of including the effect of the de-excitation of the primary fragments by neutron evaporation and fission when comparing the calculations with the measurements. In this regard, when treating very heavy systems, it is important to use “after-burners” that are suitable for situations where most of the primary product nuclei fission [46] rather than generic approaches.

TDHF calculations were used by Simenel et al. to study MNT in the ²³²Th + ²⁵⁰Cf reaction at E_c.m. = 916 MeV. While the de-excitation of the primary MNT products was not considered, the authors were able to conclude that the primary TLFs were more n-rich than those seen in fusion-evaporation reactions.

MNT Reactions—N = 126

As discussed earlier, one of the exciting applications of MNT reactions is the synthesis of nuclei near the N = 126 shell closure. Watanabe et al. [59], in a seminal study, measured the yields of several PLFs formed in the 1085 MeV (8 A MeV) ¹³⁶Xe + ¹⁹⁸Pt reaction along with the TLFs Hg and Os. Neutron rich isotopes of Os were formed in collisions involving low total kinetic energy release, while higher total kinetic energy events resulted in the production of neutron deficient isotopes.

Desai et al. [74] extended this work by studying the reaction of 760 MeV (5.59 A MeV) ¹³⁶Xe + ¹⁹⁸Pt. At the lower beam energy, the yields of the n-rich TLFs decreased by an order of magnitude or more compared to the data of [59], clearly indicating the importance of using large beam energies in systems where fission decay of the MNT products is not very important.

MNT Reactions—Heavy Transfer Products

Another study that is more relevant to the synthesis of new n-rich heavy nuclides is the work of Welsh et al. [60]. These workers studied the formation of MNT products in the near-symmetric collision of 6.67 A MeV ²⁰⁴Hg + ¹⁹⁸Pt. The predictions of the GRAZING model, the DNS model and a hybrid GRAZING/DNS model were compared to the experimental data. The predicted cross sections were a factor of 10−10⁴ lower than the observed cross sections. The Improved Quantum Molecular Dynamics (ImQMD) model predictions were also compared to the measurements. The ImQMD predictions were closer to the data, but underestimated the measured yields by factors of 10–100, perhaps due to the lack of shell effects in the ImQMD simulations. This underestimation of the MNT yields is actually encouraging for attempts to synthesize very heavy MNT products.

Gotz et al. [41] were among the first groups in the modern era to experimentally test the ability to form very heavy MNT products. They studied, using radiochemical techniques, the reaction ⁴⁸Ca + ²⁴⁸Cm at E_lab = 262 MeV. They identified trans Cm nuclides by alpha spectroscopy and focused their efforts on understanding the kinematics of these reactions. For the Fm isotopes (the heaviest trans-target nuclei observed), the angular distributions peaked near the grazing angle, θ_gr = 27° and the kinetic energies were low (~80 MeV). This suggests such products are made in grazing collisions, not deep-inelastic collisions. The nuclides with Z < Z_target seem to be associated with (DIC) collisions where there is a low survival of the MNT products.

One fascinating set of studies of the synthesis of very heavy nuclei by MNT are the studies of Natowitz et al. [75–78] at Texas A&M. In a series of seminal papers from 2011 to 2018, these authors describe the possible formation of very heavy nuclei in MNT reactions. The initial publication of this group [75] described a study of the 7.5 A MeV ¹⁹⁷Au + ²³²Th reaction. Using the Big Sol spectrometer, the authors reported the formation of nuclei with Z ~ 100 and a production cross section of ~11 nb. The authors were cautious and expressed the need for further work to confirm this remarkable result (ΔZ = +10). Further details of this experiment were presented in Majka et al. [76] along with plans to use an “active” catcher setup for further studies [77]. Wuenschel et al. [78] reported the results of an investigation of the ²³⁸U + ²³²Th reaction at projectile energies of 6.1–7.5 A MeV. Using an active catcher system with yttrium aluminum perovskite (YAP) to detect transfer products from this reaction, the authors found several interesting events. (The incident beam was degraded from the entrance energy of 7.5 A MeV to below the Coulomb barrier (6.1 A MeV) in passing through the 11 mg/cm² Th target). Data was taken with the beam on and with the beam off following the detection of an interesting event. In Figure 2 [78], we see the results of a search for correlated decay pairs. The open circles show events with Z ≤ 101 and the filled triangles denote Z > 101 (ΔZ > 11). The systematics [79] of E_α vs. t_1/2 for e-e nuclei with Z = 98–122 is shown as a set of lines. If we restrict our attention to events in the angular range from 31° to 51°, the differential cross sections of Figure 3 result. (Groups 1–7 correspond to angular range of 31–51° with further sorting by half-life ranges, with Group 1 corresponding to the shortest half-lives and Group 7 the longest half-lives). The authors conclude that “new activities with Z as high as 116 are being produced in these reactions.” (This corresponds to ΔZ ~26!!). The quarter point angles for the TLFs range from 31 to 48°, consistent with the angular ranges plotted in Figure 3.

FIGURE 2

Figure 2. A plot of t_1/2 vs. E_α for coincident pairs of TLFs from the ²³⁸U + ²³²Th reaction from Wuenschel et al. [78]. Open circles denote Z ≤ 101 and filled triangles indicate Z ≥ 101. The lines and filled squares indicate the predictions of Agbemava et al. [79] for e-e nuclei with Z = 98–122.The solid diamonds indicate the experimental data.

FIGURE 3

Figure 3. A plot of the differential cross section of TLF events in the angular range from 31 to 51° for the reaction of ²³⁸U with ²³²Th. Groups 1-7 correspond to various half-life ranges with Group 1 corresponding to the shortest half-lives and Group 7 the longest half-lives.

The Future

What is the future of the effort to use MNT reactions to form very heavy neutron-rich nuclei? Part of the answer to this question is the determination of whether one should focus on events where the TLFs are formed near the grazing angle or whether the most interesting (high +ΔZ) events occur at angles near the beam axis (Zhu, Personal communication). Can we use existing vacuum separators like SHIP or the FMA to study these reactions (where detection of the products is restricted currently to small angles)?

The most n-rich heavy nuclei are β-emitters, posing a challenge to experimentalists to detect and identify these nuclei. The N = 126 factory project at the Argonne National Laboratory, described earlier, is one approach to this problem. However, if the interesting n-rich nuclei are formed at small angles with respect to the beam, this approach is problematic.

A stable beam facility that should play a role in future studies of heavy element synthesis reactions is the S³ project art GANIL. The GANIL facility, SPIRAL2, is expected to have very high intensity stable ion beams [8]. Two complementary detection systems, SIRIUS and REGLISS, are being developed to detect reaction products. SIRIUS is a highly segmented focal plane detector to detect the implantation and decay of reaction products [80]. REGLIS involves a gas cell for stopping the reaction products followed by resonant ionization of the stopped atoms [80].

One of the most developed schemes to study MNT reactions that produce very n-rich, β-emitting products is the KEK Isotope Separation System (KISS) [81–83]. This system is designed to study MNT reactions between heavy targets and heavy projectiles. The KISS consists of a dipole magnet and an argon gas-cell with laser resonant ionization. Isotope separation is achieved in two steps; laser resonant ionization to identify the Z of the reaction product followed by M/q separation in a magnetic field. First applications of this system are projected to study nuclei near the N = 126 shell.

While all these new developments in studying MNT reactions are exciting, one should not forget the use of “conventional” apparatus to study MNT reactions, especially those events produced at small angles with respect to the incident beam, the so-called “deep inelastic collisions.” The velocity filter SHIP has been employed in a number of these studies [34, 39–41].

Another “conventional” device to study MNT reactions is the PRISMA spectrometer at Legnaro, Italy. This spectrometer, when operated in coincidence with a time of flight arm, allows identification of the A, Z, and velocity of the PLFs and TLFs. This system has been used in several studies of MNT reactions.

Summary

What have we learned about and what is the future outlook for forming new very heavy n-rich nuclei? Using facilities like FRIB, SPIRAL2, and TRIUMF, it appears that there are reasonable opportunities to make new n-rich nuclei with Z = 103–108. The situation, with respect to MNT reactions, is less clear as we have several unanswered experimental questions. Assuming the cross sections are high enough and the facilities to study and identify the reaction products are developed, it may be that MNT reactions are the most promising for producing and studying these nuclei.

Data Availability

All datasets generated for this study are included in the manuscript and/or the supplementary files.

Author Contributions

The author confirms being the sole contributor of this work and has approved it for publication.

Funding

This work was supported in part by the U.S. National Science Foundation under award 1505043-PHY and the U. S. Department of Energy, Office of Science, Office of Nuclear Physics under award DE-SC0014380.

Conflict of Interest Statement

The author declares that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Footnotes

1. ^https://groups.nscl.msu.edu/frib/rates/fribrates.html

2. ^http://www.triumf.info/facility/research_fac/yield.php

3. ^http://www.to.infin.it/nanni/grazing

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