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Physics Research International
Volume 2011 (2011), Article ID 128429, 12 pages
http://dx.doi.org/10.1155/2011/128429
Review Article

Neutron Production in Thick Targets Irradiated with High-Energy Ions

1Institute of Nuclear Science, School of Physics, University of Sydney, Sydney, NSW 2006, Australia
2Physics Department, Aristotle University, 54124 Thessaloniki, Greece
3Joint Institute for Nuclear Research, 141980 Dubna, Russia
4Fachbereich Chemie, Philipps Universität, 35032 Marburg, Germany
5Institut für Materialwissenschaften, Technische Universität Darmstadt, 64287 Darmstadt, Germany
6Forschungszentrum Jülich GmbH, 52425 Jülich, Germany
7Dr. Westmeier GmbH, 35085 Ebsdorfergrund, Germany

Received 18 April 2011; Accepted 12 July 2011

Academic Editor: Ali Hussain Reshak

Copyright © 2011 S. R. Hashemi-Nezhad et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

The neutron production in thick targets irradiated with 1 GeV protons was studied experimentally, and results are well understood with model calculations, including MCNPX 2.7a. However, one observes very large neutron production rates in the interaction of 44 GeV 12C onto thick Cu-, Pb-, and U-targets beyond calculated rates. The experimental spallation product yield curve in a 20 cm thick Cu target irradiated with 72 GeV 40Ar also cannot be reproduced by several model codes, including MCNPX 2.7a. This may be due to secondary fragments produced in high energy ( GeV) heavy-ion interactions which destroy target nuclei more effectively than primary ions. These observed experimental facts constitute “unresolved problems” from a fundamental point of view. It may have an impact on radiation protection issues for future heavy-ion accelerators.

1. Introduction

Recent investigations on the interaction of relativistic ions (called primaries in this paper) above a total energy  GeV in thick heavy-element targets show unexpected phenomena in the spallation yield distributions, as well as surprisingly intense neutron emission. These unexpected phenomena constitute “unresolved problems” as described in [1, 2].(1) Spallation mass-yield curves in any thin target are completely understood with conventional reaction models like “limiting fragmentation” and “factorisation” [1, 2]. However, the spallation mass-yield curves in thick targets which are also produced by secondary fragments, generated in the interaction of primaries with target nuclei, are incompatible with these concepts of “limiting fragmentation” and “factorisation.” Secondary fragments, in the following called secondaries, seem to release more neutrons when they interact than primaries.(2)The neutron emission from thick targets irradiated with ions having  GeV is rather intense, in particular for 44 GeV 12C and 72 GeV 40Ar onto thick Cu- and Pb-targets. These phenomena need further investigation.

Experimental results published for thick targets irradiated with relativistic ions are scarce and sometimes contradictory. In the experiment on “neutron yields from 1 GeV/nucleon 238U ion beams on Fe target” by Yordanov et al. [3], the neutron spectra above 50 MeV were studied. The authors could fit their experimental data with well-known models and stated (quote) that “after a first beam-target collision the projectile residue may subsequently undergo the same type of reactions as just mentioned” (i.e., in agreement with well-accepted standard models). The results reported in [1, 2] show evidence that secondary fragments excite target nuclei stronger than primary ions, thus producing more neutrons than expected from calculation. Findings from [13] are not in contradiction as will be shown [4]. It seems that as if unresolved problems arise only after an energetic limit that is barely approached in the 1 GeV/u 238U + Fe experiment. This may become an important issue for high intensity, high energy heavy-ion accelerators presently under construction. One essential aspect of this construction is the consideration of all aspects of radiation protection for the operation of these machines with respect to(i)workers in the laboratories,(ii)materials close to the beam line and target areas,(iii) and—not the least—the surrounding environment.

The aim of this paper is to concentrate on the experimentally known facts which may serve as benchmarks for any radiation protection model. Two major topics will be considered.(1)The neutron emission from thick targets irradiated with ions in the energy range of 1 GeV ≤ ≤ 44 GeV at the JINR in Dubna (Russia) and its influence on radiation protection.(2)The experimental spallation mass-yields produced in a 20 cm thick Cu target in the irradiation with 72 GeV 40Ar at the LBNL in Berkeley (USA). Calculations with modern code MCNPX 2.7a [5] are compared with experiments demonstrating that secondaries interact with target nuclei stronger than primaries. The corresponding neutron emission in the irradiation was measured to be large, however, quantitative results have not been published.

A key question in all investigations is the determination of the total number of neutrons produced in a thick target by a single ion with a well-defined primary energy. A target is considered as being thick when a large fraction of secondary particles induce additional interactions within this target.

2. Radiation Protection Studies at JINR, Dubna, Russia

2.1. Direct Neutron Measurements from a Thick Pb Target at the Synchrophasotron Accelerator

In an early experiment, a very consistent measurement of the numbers of neutrons emitted from a thick Pb target ( cm and  cm) was carried out in irradiations with a large variety of ions available at the Synchrophasotron at the JINR in Dubna (Russia) by Vasil'kov et al. [11]. The essential experimental results are presented in Table 1(a), together with calculations in Table 1(b). One observes for proton irradiations at kinetic energies  GeV and  GeV a consistent and well-understood behaviour. The number of neutrons per GeV decreases slightly with increasing energy. However, one observes an unexpected result for heavy ions up to mass 12: The experimental values at 3.7 AGeV are up to 50% larger than results from model calculations. One should remember that individual neutrons were determined by counting in an LSC unit.

tab1
Table 1: The direct measurement of neutron production in THICK Pb-targets irradiated at the Synchrophasotron [11].

A recent publication by Yurevich et al. [12] reports on the direct measurements of the total number of neutrons emitted from lead targets of various configurations in proton irradiations in the energy range (1 GeV < < 3.7 GeV). The authors used various experimental techniques, including TOF and Pb(,xn), to obtain the total number of emitted neutrons. They also investigated the same thick Pb target as the one employed in [11]. The observed neutron numbers per proton for the same target as shown in Table 1(a) are () at 1 GeV and () at 3.7 GeV, which is in fair agreement with the results from [11].

2.2. Radiation Protection and Indirect Measurements of Neutrons Produced by (1.0–1.5) GeV Protons at the Nuclotron Accelerator

A recent publication [6] from experiments at the Nuclotron accelerator in JINR describes measurements of the neutron dose from 1 GeV protons around two thick Pb target assemblies, called “Gamma-2” and “Energy plus Transmutation” (). The neutron dose measurements were carried out close to the targets and in addition behind a 1.0 m thick concrete shielding wall of the experimental set-ups as shown in Figure 1.

fig1
Figure 1: The spallation sources used in JINR in Dubna, Russia: (a) “Gamma-2” target, (b) “Energy plus Transmutation” () assembly. The term “Uz blanket” stands for the uranium blanket surrounding the Pb target. (c) This diagram illustrates the positions of the spallation sources, the concrete shielding wall, and the locations of the SSNTDs (solid state nuclear track detectors) that serve to determine the neutron ambient dose equivalent. Distances can be estimated from the thickness of the concrete wall which is 1.00 m (Figure taken from [6]).

The target system “Gamma-2” (for details see Figure 2 and Section 2.3 below) had been used earlier in the same experimental location of the Laboratory for high energy (JINR, Dubna) for heavy ion irradiations using the Synchrophasotron accelerator. Thus, one can compare the results from the present-day neutron dose experiments with earlier irradiations with relativistic heavy ions a decade ago using the same “Gamma-2” target.

fig2
Figure 2: The GAMMA-2 target (Since 2007, GAMMA-2 has been an IAEA benchmark target for transmutation studies, see text and [710]). (a) Positions for uranium sensors, (b) positions of lanthanum sensors, (c) positions of various SSNTD sensors.

The Pb core in the “Energy plus Transmutation” () target has a diameter of 8.4 cm and a length of 45 cm, and it is surrounded by a blanket of 206.4 kg natural uranium plus also a massive neutron shield. A detailed description can be found in [6, 1315].

The neutron dose measurements were carried out with solid state nuclear track detectors (SSNTD’s) by Fragopoulou et al. [6]. Their experimental techniques allow to obtain separate results for(i) low-energy neutrons with  eV,(ii)epithermal neutrons with 1 eV < < 10 keV, and(iii) intermediate-fast neutrons with 0.3 MeV < < 3 MeV.

The actual neutron ambient dose equivalent in units of Sievert (Sv) was calculated using experimental conversion factors. The results are shown in Table 2:

tab2
Table 2: Experimental neutron ambient dose equivalent from the irradiation of a Pb target in “Gamma-2” and “Energy plus Transmutation” () with 1013 protons and a comparison with model calculations [6].

The agreement between experiment and calculation is fine within uncertainties for these two target systems and in this energy range. The calculation for the “Gamma-2” target gave 15 neutrons per 1.0 GeV proton which is smaller than the corresponding number in Table 1(a) as the Pb target in Gamma-2 was smaller than Vassil'kov’s target.

A further detailed analysis of the fission rate inside the massive uranium blanket for the () system has been carried out in [15]. The authors used Monte Carlo code MCNPX 2.6C and showed that the experimental fission rates are only about ()% larger than the calculated ones.

2.2.1. Neutron Dose in the Vincinity of the Target

The intermediate-fast neutron dose around the () target with its massive uranium blanket around a thick lead target is larger than around “Gamma-2”, however, the thermal-epithermal neutron dose is larger at “Gamma-2”, due to the paraffin moderator around this target (see Table 2).

2.2.2. Neutron Dose behind 1 m of Concrete

The “Gamma-2” target produced a considerable thermal neutron dose behind the concrete wall. The irradiation lasted 11 hours with a total fluence of 1013 protons of 1 GeV on target, corresponding to an average of  protons/sec. The experimental neutron ambient dose equivalent behind the concrete wall was 37 μSv/h [6], which is too much to be tolerated by humans. The ICRP 66 (International Commission on Radiological Protection, Recommendation No. 66) recommends that for a position outside the concrete shielding of accelerators in “controlled areas,” a dose should not exceed 10 μSv/h. Therefore, the Health Physics Department of JINR requested the scientists to stay at least 50 m away from the experimental area during irradiation. For irradiations of the () target, similar rules applied, but the radiation level outside the experimental area was considerably smaller due to the additional neutron shield provisions around the Pb/U target.

Further experiments measuring the neutron dose equivalent under well-defined conditions during the irradiation with heavy ions onto thick targets are necessary with relativistic ions like 2H, 4He, and 12C. Such irradiations had been carried out a decade ago using the “Gamma-2” target at the Synchrophasotron, however, without any quantitative measurements of the neutron ambient neutron dose equivalent outside the concrete shielding. In this paper, a “postfactum” estimate of the corresponding neutron ambient dose equivalent outside the concrete shielding is presented.

2.3. Neutron Emission from the “Gamma-2” Target Irradiated with Protons at the Nuclotron and Heavy Ions (2H, 4He, and 12C) at the Synchrophasotron

The comparison of the neutron emission from the “Gamma-2” target irradiated with heavy ions at the Synchrophasotron accelerator and with protons at the Nuclotron accelerator will allow the inter-calibration of experimental results from both accelerators. Figure 2 shows the detailed lay-out of the “Gamma-2” target. It consists of a metallic core of either 20 Cu or 20 Pb disks (1 cm thick, 8 cm diameter) and it is surrounded by a 6 cm thick paraffin moderator. The moderator contains grooves for plastic vials containing 1 g of La or U for radiochemical studies.

The “Gamma-2” target allows two-parameter experiments: (1)In the irradiation with relativistic ions onto the metallic core, all kinds of spallation products are produced inside the metallic disks. These spallation products can be determined with standard radiochemical techniques after the irradiation. (2)Spallation neutrons are simultaneously produced, which enter the paraffin. These neutrons are partially moderated, with many neutrons even reaching the thermal regime. All neutrons induce () and other reactions in various sensors. Details are given in [1, 2, 710], only a short description will be given here. Using the lanthanum sensor, which is mono-isotopic stable , one can study the neutron capture reaction From the -ray emission rate of a production rate, called “breeding rate” , can be calculated which is defined as In a similar manner, one can measure from the study of the reaction . For this comparative analysis, results measured for proton interactions at the Nuclotron in Table 3 and for heavy ion interactions at the Synchrophasotron in Table 4 using the same “Gamma-2” Pb target are shown.

tab3
Table 3: -values on the “Gamma-2” Pb target, irradiated with protons at the Nuclotron [9] and compared with different model calculations.
tab4
Table 4: Neutron fluences measured as on “Gamma-2” target in irradiations with 2H, 4He, and 12C at the Synchrophasotron [7].

Table 3 allows the following conclusions:(i)The recent experimental values of ratios obtained for (1.0–3.7) GeV proton irradiation are in fine agreement with model calculations. Details of the distribution on top of the “Gamma-2” Pb target with MCNPX 2.7a calculations for 1.0 GeV and 2.0 GeV protons reveal good agreement between experiment and calculation [16].(ii)The ratios between (3.7 GeV/1.0 GeV) and (2.0 GeV/1.0 GeV) agree with model calculations.

During the last decade of the operation of the Synchrophasotron until about the year of 2000, extended irradiations of “Gamma-2” targets with 2H-, 4He-, and 12C-beams in the range of total energies from 3 GeV up to 44 GeV were carried out [7, 8] where the metallic target core was copper or lead. Radiochemical sensors, such as stable lanthanum (see (1)) and natural uranium were irradiated and and values were obtained. Results of irradiations with 2H-, 4He-, and 12C-ions onto “Gamma-2” targets at the Synchrophasotron are shown in Figures 3 and 4.

fig3
Figure 3: Breeding rates and in irradiations with relativistic 2H, 4He, and 12C onto a Pb core in “Gamma-2”. Results are given for 5 sensors on top of the paraffin moderator [7].
fig4
Figure 4: Breeding rates and in the irradiation with 2H and 12C onto a Cu core in the centre of “Gamma-2”. -values are averages from 5 sensors. (This figure is taken from [7]).

The resulting distributions for 2H-, 4He-, and 18 GeV 12C-irradiations are surprisingly similar, irrespective of the projectile element and energy. In the 44 GeV 12C irradiation, however, one observes a drastic increase in the production of 140La and 239Np.

Similar results are observed in experiments using a Cu-core in “Gamma-2.” The results are shown in Figure 4, where the average -value for the investigation in five La- or U-sensors on top of the moderator is given [7]. Again, for 44 GeV 12C irradiations, one observes a strong increase in -value, whereas at lower total bombarding energies, -values are grouping around significantly lower values.

Neutron induced interactions were studied by this collaboration over a wide energy range: Wang et al. [17] studied the integral neutron energy spectra emitted from “Gamma-2” with the nuclear emulsion technique. They measured secondary neutrons with energies up to 1 GeV. Their results are complementary to the work of Yordanov et al. [3], who studied high energy neutron spectra behind 20 cm thick iron targets with counter techniques.

A summary of -values, originating from the capture of low-energy neutrons, measured in 2H, 4He, and 12C ion irradiations is given in Table 4. The experimental ratios of -values at (3.7 AGeV/1.5 AGeV) are(i)() for 2H and 4He induced reactions, and(ii)() for 12C irradiations, which is significantly higher.

The large -value for 44 GeV irradiations is again an indication of something different, already observed in [1, 2] and termed there as “unresolved problem.” A similar observation was found earlier by Brandt [18]. In the irradiation of a large Pb block with 3.7 AGeV ions from the Synchrophasotron, fine agreement between experiment and calculations for proton, deuteron, and alpha irradiations was observed. In the irradiation with 44 GeV 12C, however, (atoms per carbon ion per gram of Np) was measured, which is about twice as large as calculated by Tolstov and rather similar to our result shown in Figure 3.

All evidences demonstrate that one needs additional experiments to study the neutron production in thick targets using heavy ions at high energies. In these future experiments, one may be confronted with nontrivial radiation protection problems. 1 GeV protons on the “Gamma-2” Pb-target lead to a large neutron dose behind the concrete shielding; therefore, one might expect much more severe radiation protection problems in irradiations with 44 GeV 12C beams.

If assuming that(i)one uses the same experimental setup as shown in Figure 1, and(ii)the “neutron ambient dose” behind the concrete shielding increases linearly with -values that were measured on “Gamma-2” with Pb core at the Synchrophasotron,

then one obtains estimated neutron ambient doses as given in Table 5.

tab5
Table 5: Estimated neutron ambient doses (for  ions/s) in irradiations with 44 GeV 12C, as based on recent experiments with 1 GeV protons onto a “Gamma-2” Pb target. The calculated neutron production rate in neutrons per ion is taken as the basis for calculation of the last column.

The measured ambient neutron dose (μSv/h) and the experimental transmutation rate in the interaction of (1 GeV + Pb target) yielding a ratio [(μSv/h)/(/ion)] = 2.3 ± 0.3 are in agreement with recent calculations. For irradiation with 44 GeV 12C onto a thick Gamma-2 target core, however, one estimates an average which is much larger and statistically significantly different from 2.3. This is a further indication that one may observe for large beam energies onto thick targets significantly higher than calculated neutron numbers. The neutron ambient doses behind the concrete shielding exceed significantly the radiation protection allowance for humans to stay near this area during the experiment. A further clarification of this problem can only be obtained with more experiments. Such experiments are needed to understand the underlying physics more accurately, as well as to supply more adequate radiation protection shielding data for thick-target irradiations.

3. Thick Target Studies at LBNL, Berkeley, California

Thick-target experiments at Lawrence Berkeley National Laboratory (LBNL) started around 1980 with the irradiation of two Cu disks in contact, with each disk having a thickness of 1 cm and a diameter of 8 cm. The aim of such studies was the investigation of possible differences in nuclear interactions of relativistic secondary fragments in comparison with the relativistic primary ions as reviewed in [1, 2] and presented in Figures 5 and 6.

fig5
Figure 5: The original “two Cu disk experiments” in Berkeley showing the first evidence for unresolved problems [1, 2] in irradiations with 72 GeV 40Ar at the Bevalac accelerator (LBNL) after 1980. The original “two Cu disks” experiments were carried out from 1980 with relativistic 40Ar-ions at the Bevalac in Berkeley. (a) Schematic representation of the target set-up using two Cu disks and a surrounding guard ring around the second disk. Two configurations were irradiated: (i) (top): 0 cm distance between the disks (), (ii) (bottom): 20 cm distance between the disks (). (b) Autoradiographic negative picture of a Cu disk after an irradiation with 72 GeV 40Ar showing the well-focussed Ar beam in the centre. (c) Schematic representation of 3 different reaction paths. The path Ar-3 is of particular importance for the study of effects due to secondary fragments.
128429.fig.006
Figure 6: The original “two Cu disk experiments” in Berkeley showing the first evidence for unresolved problems [1, 2] in irradiations with 72 GeV 40Ar at the Bevalac accelerator (LBNL) after 1980. ratios for reaction products measured in interactions of 72 GeV 40Ar with two Cu disks are defined as: (activity of nuclide downstream/activity of nuclide upstream). The distance between the two Cu disks is  cm for and  cm for . These ratios can be determined very accurately.

The ratio of nuclear interactions induced by primaries to those induced by secondaries is larger in the first Cu disk than in the second Cu disk. The study of experimental yield ratios of individual spallation products in the second Cu disk as compared with the first Cu disk reveals evidence for a different behaviour of secondary fragments as compared with the primary ions.

The ratio is defined for two Cu disks in contact ( cm), where activities are decay-corrected to the end of bombardment.

Figure 5 shows the experimental setup and the results are shown in Figure 6. Our focus will be on the results. Due to considerable production of relativistic secondaries, one observes for all spallation products . It is interesting to note two surprising features in Figure 6:(i) for 24Na is . This value is considerably larger, by at least 25%, than all values based on various theoretical model calculations as has been discussed by Aleklett et al. [19] and in detail in [1, 2]: the production of 24Na by secondaries is larger than that by primaries.(ii)One observes for product masses above a decrease in with increasing mass . All theoretical interpretations have failed to describe this phenomenon.

The comparison of experimental results (see Figure 6) with the calculated distribution using the MCNPX 2.7a code is shown in Figure 7 and reveals surprising results.

128429.fig.007
Figure 7: Comparison of the experimental and theoretical distributions in the interaction of 72 GeV 40Ar with two Cu disks.

Some details of this comparison shall be emphasized(i)For mass (7Be) and for masses the agreement is good.(ii)The experimental production rate of the isotope 24Na (as well as 22Na and 28Mg) is significantly larger than models calculate. (Region 1 around ).(iii)Above   experimental decreases with rising whereas an increase in with rising is theoretically predicted. (Region 2 above ).

The results for Region 1 could correlate with the result seen in Region 2. One finds an excess of experimental cross section in Region 1 whereas one misses cross-section in the second Cu disk just below the target mass in Region 2.

It may be useful to carry out further experiments to learn more about these phenomena from additional experimental approaches:(i)One should measure for many nuclides close to the target mass but also for 60Co, 61Co, 62Zn, and 64Cu in order to compare with Cumming et al.’s [20] data where production rates for these isotopes in thin Cu targets irradiated with 80 GeV 40Ar were determined.(ii)Additionally, one should carry out neutron counting experiments using thick Cu targets having thicknesses 2 cm ≤ ≤ 20 cm irradiated with 72 GeV 40Ar ions.

The experimental distribution shown in Figure 6 is compared with the theoretical calculation using the MCNPX 2.7a code in Figure 8. The congruence between the theoretical fit and the experiment is remarkable. One observes only a slight experimental deficiency around masses and a slight experimental excess for 24Na.

128429.fig.008
Figure 8: Comparison of the experimental distribution and the MCNPX 2.7a calculation.

The last issue of this paper is concerned with the radiochemical aspects in the study of a 20 cm thick Cu target (i.e., 20 Cu disks of 1 cm thickness in contact) irradiated with 72 GeV 40Ar. In this irradiation at LBNL, a very strong neutron dose was registered even outside the experimental area of the Bevalac accelerator. However, quantitative neutron data about this event have never been released.

The 20 cm thick Cu target was designed as a two-parameter experiment:(i)The determination of neutron production was in principle possible, however, no results of neutron measurements were ever published, as mentioned several times.(ii)Nuclear reactions inside the Cu disks were actually studied, that is, spallation product yields in several 1 cm Cu disks were determined, yielding information about nuclear interactions of relativistic ions inside the entire thick Cu target.

Both sets of information (neutron production rates plus spallation yields) are needed for a complete understanding of the reaction mechanism.

Some detailed experimental yield ratios for two typical spallation nuclides (24Na and 57Ni) in several Cu disks (number = ) as compared with the first Cu disk (number = 1) will be discussed. The nuclide 24Na was chosen as representative for “Region 1” and 57Ni as representative for “Region 2.” The experimental yield ratios are compared with their calculated ratio using MCNPX 2.7a in Figure 7. Two nuclides appear to be of particular importance:(i)The key isotope 24Na (Region 1) is produced in the downstream 1 cm thick Cu disks () definitely in larger yield than calculated by computer codes, including MCNPX 2.7a. (ii)The isotope 57Ni (Region 2 with ) is produced in the downstream 1 cm thick Cu disks () with about the same yield as calculated by MCNPX 2.7a.

The following Figures 9 and 10 present the respective ratios for -values, where is the number of the Cu disk within the 20 cm Cu stack. The experimental ratios are compared with model calculations, experimental data tables are given in [21].(i)24Na is produced more abundantly than calculated in every disk, just as in the “2 cm Cu disk” experiment.(ii)57Ni is produced a little less abundantly in this experiment as compared with calculation. This deficiency is observed in all Cu disks in the 20 cm Cu target.

128429.fig.009
Figure 9: Comparison of the experimental yields in the 20 cm Cu stack with theoretical values from the computer code MCNPX 2.7a. is the activity ratio of  24Na in Cu disk number “” as compared with the first disk.
128429.fig.0010
Figure 10: Comparison of the experimental yields in the 20 cm Cu stack with theoretical values from the computer code MCNPX 2.7a. is the activity ratio of 57Ni in Cu disk number “” as compared with the first disk.

Repeating the argumentation presented for Figure 7, one can correlate the behaviour of 24Na with the behaviour of 57Ni. One finds an excess in experimental cross section for 24Na in all Cu disks as compared with calculation, and one misses experimental cross section in all Cu disks for 57Ni. This is continuing evidence for discrepancies that requests further experiments to measure product yields and additionally also the neutron production per ion in the reaction of 72 GeV 40Ar with a thick Cu target (or similar).

Another question to be asked is: what amount of “enhanced neutron production” can one expect in the reaction (20 cm Cu + 72 GeV 40Ar) as compared with the well-investigated reaction (20 cm Cu + 44 GeV 12C)? There exists only one indirect measure for the “enhanced nuclear destruction” ability of secondary fragments in thick copper targets, which is the measurement of in “two Cu disk experiments” (Figures 5 and 6) for a large variety of projectile ions using several accelerators around the world. The result of such investigation is presented in Figure 11. It was shown in [1, 2] that there is a smooth relation between and the energy of the ion when the experimental values are plotted with respect to the total ion energy , irrespective of the ion. Some of those experimental ratios for 24Na production are(i)1.5 GeV 1H onto two Cu disks yield ;(ii)44 GeV 12C onto two Cu disks yield ;(iii)72 GeV 40Ar onto two Cu disks yield .

128429.fig.0011
Figure 11: The ratio as a function of total kinetic energy. The calculated “theoretical” line from [1, 2] is given for comparison.

The increase in for 72 GeV 40Ar as compared with 44 GeV 12C may yield stronger increase in the “enhanced neutron production”—but only an experiment can give the answer. This answer is needed to understand neutron multiplicities in thick targets and to provide proper radiation protection for any new construction of high intensity, high energy heavy-ion accelerators.

Recent calculations using the MCNPX code indicate that the simulated mass yields are model dependent. Conclusions presented here on the 72 GeV Ar + Cu results (Figures 710) are based on the current results of calculations. A detailed analysis of the MC-calculated mass yields in heavy-ion interactions using all available physics models in the MCNPX code and comparison with the experimental data from the literature is in progress and will be presented in another publication.

4. Conclusions

Neutron ambient dose equivalents have been measured in the irradiation of a 20 cm thick Pb target with 1 GeV protons close to the target and at larger distances in the experimental hall. Experiments and calculations based on DCM/CEM code agree within uncertainties. Based on experiments where breeding rates were measured with 1 GeV protons and 44 GeV 12C under similar conditions, one can estimate the neutron ambient dose equivalent during irradiations with 44 GeV 12C onto thick Pb and Cu targets close to the target and in the experimental hall. The estimated neutron ambient dose equivalents are on the order of 1000 μSv/h at about 5 meters distance and behind 1 meter thick concrete shielding for the irradiation parameters given. Such large doses require that humans stay away a considerable distance from the experimental area, maybe more than 50 m. One may observe in these heavy ion irradiations of thick targets some physical phenomena constituting a radiation protection problem connected to the “unresolved problems” as described in [1, 2].

Detailed calculations carried out with the MCNPX 2.7a code have shown that radiochemical spallation yield distributions in thick Cu targets irradiated with 72 GeV 40Ar cannot be reproduced by calculations. Secondary fragments destroy Cu nuclei stronger than primary 72 GeV 40Ar ions, thus confirming observations reported in [1, 2]. The neutron ambient dose equivalent in the irradiation of 20 cm thick Cu targets with 72 GeV 40Ar is experimentally known to be large, but data have never been published. Such published data would be useful for two reasons: (i)to design the radiation protection shielding for heavy ion accelerators producing high energy heavy ions with large intensities, and(ii)to learn more about the physical reason connected with these “unresolved problems.”

Acknowledgments

The authors wish to thank the operators of the Nuclotron accelerator in the LHEP for their continuous efforts to provide first class and stable beams. Considerable part of the work was made in the framework of an International Collaboration (GAMMA-2, Energy plus Transmutation) experimenting at the Nuclotron accelerator in JINR (Dubna, Russia).

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