首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 46 毫秒
1.
Fast neutrons produced in 44 and 22 GeV 12C+Cu interactions have been recorded and analysed with a CR-39 detector stack. The irradiation of the CR-39 stack to fast neutrons was carried out at the accelerator Synchrophasotron, Joint Institute for Nuclear Research, Dubna, Russia. Areal and volume densities of tracks induced by fast neutrons in the CR-39 at different positions and for different etching time have been measured. The neutron production ratio of 44 GeV to 22 GeV 12C+Cu interactions has been obtained, which is 2.17 ± 0.30 by areal track density, or 2. 12±0.33 by step etch technique, or 2.03±0.34 by volume track density measurement. These results confirm that the production rate at 44 GeV 12C+Cu interactions is more than theoretical estimation.  相似文献   

2.
Summary A stack consisting of CR-39(DOP) detector with 2.6 cm Al target was exposed to a238U beam of energy 0.927 GeV/n from LBL BEVALAC to study the large-fragmentation phenomena during U+Al interaction. The diameter distribution of the etch pits formed in the plastic detectors for the first three projectile fragments of chargeZ F≥89 yields the partial cross-section data which is comparable to the data obtained from the cone length distribution. The present result on the partial cross-section is significantly higher than those expected from the abrasion-ablation model of Wilson, Townsed and Badavi (1987). The authors of this paper have agreed not to receive the proofs for correction.  相似文献   

3.
We present the results of an experimental work aimed at improving the performances of the CR-39® (Registered Trademark of PPG Industries Inc.) nuclear track detector for neutron dosimetry applications. The work was done in collaboration with the Intercast Europe S.p.A., producer of CR-39 for commercial and scientific applications. We compare the CR-39 made with different additives concentrations and different polymerization processes. We evaluate the response of the CR-39 to fast neutrons from three sources: 241Am---Be, 252Cf and 238Pu---Li. Particular attention was paid to background fluctuations that limit the lower detectable dose.  相似文献   

4.
Measurements have been carried out on neutron yields and spatial distributions in U/Pb, Pb and Hg thick targets and the surrounding paraffin moderators bombarded by 0.533 and 1.0 GeV protons. CR-39 detectors were deployed on the surfaces of targets and moderators to record the neutrons produced in the targets. The measurements show that:

Article Outline

1. Introduction
2. Experiments
3. Results
3.1. Neutron yield of Hg target
3.2. Neutron distributions along targets
3.3. Energy of secondary neutrons
4. Conclusions
Acknowledgements
References

1. Introduction

The study of accelerator-driven subcritical nuclear reactor has attracted the attention of nuclear physicists and engineers in the world. The main aim of the facility to be built is to generate electricity, dispose long-life radioactive wastes and find a way not to produce or produce much less radioactive wastes. One of the key components of this type of new facility is a particle accelerator, from which high energy particles, most possibly protons, impinge on a target in which high intensity of secondary neutrons are produced. These neutrons then initiate operation of a subcritical nuclear reactor. In the central part of the core of the reactor is the target. The optimization of neutron parameters in the target and the surrounding moderating materials is very important for successful operation of the reactor. This work aims to determine neutron yield, spatial distribution and energy characteristics in the target region of the accelerator. This paper reports the new results obtained by proton bombardments on U/Pb, Pb and Hg targets.

2. Experiments

The experiments were carried out at the Synchrophasotron accelerator in the Joint Institute for Nuclear Research (JINR), Dubna, Russia. The beams of protons with 0.533 or 1.0 GeV from the accelerator impinge on a target U/Pb, Pb or Hg. The size of the Pb target was 8 cm in diameter and 20 cm in length (thickness). The U/Pb target was composed of a U column in the central part and a Pb sleeve (cylinder) on the column. The size of the U column was 3.6 cm in diameter and 20 cm in length. The outer diameter of the sleeve was 8 cm and the length was 20 cm. The inner diameter of the sleeve was just in contact with the outer surface of the U column. The size of Hg target was the same as the Pb target. Outside the U/Pb, Pb, or Hg target there was a cylindrical paraffin moderator with a thickness of 6 cm and length of 31 cm. Intensive secondary neutrons were produced in the U/Pb, Pb or Hg target on irradiation with protons. The neutrons were recorded with CR-39 detector strips of 20 cm in length and 1 cm in width, which were placed in the gap between the target U/Pb, Pb, or Hg and the paraffin moderator (here, we call inner CR-39 detector) as well as on the outer surface of the paraffin moderator (we call outer CR-39 detector). The length of the CR-39 strips was the same as the targets and the starting point (X=0) of the CR-39 detector was just the starting point of the targets at the upper stream end for the incident beams. The ending point (X=20 cm) of the CR-39 detectors was just the ending point of the targets at downstream for the beam. The secondary neutrons from the targets produce recoil nuclei C, O and H and other charged reaction products in the CR-39 detectors whose composition is [C12H18O7]n. The recoil nuclei and other products create tracks in the CR-39. The numbers of 0.533 GeV protons impinged on Pb and U/Pb targets were 1.52×1013 and 1.502×1013, respectively. The numbers of 1.0 GeV protons impinged on Pb, U/Pb and Hg targets were 1.91×1013, 2.03×1013 and 2.236×1013, respectively. After irradiation with secondary neutrons in each run of the experiments, the CR-39 detectors were etched in 6.5 N NaOH solution at 70°C for 45 min to develop the tracks in the detectors. The tracks at certain positions (X=0,5,10,15 and 20 cm) in each CR-39 detector were counted with track image analyzer.

3. Results

3.1. Neutron yield of Hg target

The areal track densities (ρT) were measured at different positions (X) along the CR-39 detectors on the surfaces of the U/Pb and Hg targets and the moderator for 1.0 GeV p bombardments. Track yield (Y) from a single proton is defined to be the ratio of ρT to the number of the incident protons. The track yields in the outer CR-39 detectors are shown in Fig. 1. The track yield ratio R of U/Pb to Hg targets from the above outer CR-39 detectors are shown in Fig. 2. The average value of the ratios at different places (X) is 2.00±0.11. Similar measurements with inner CR-39 detectors on the surfaces of U/Pb and Hg targets were also carried out. The track yield ratio from the inner CR-39 is 2.11±0.33, which is in agreement with the value of the outer CR-39. The final result of the track yield ratio of U/Pb to Hg target is 2.01±0.10. If we suppose that the energy spectra of neutrons from different targets and different energies of protons at different detector positions are similar and their differences would not produce a great influence on track formation in CR-39 detectors, then the track densities in the CR-39 detectors are proportional to the fluences of the secondary neutrons at the place. The track yield is approximately proportional to the neutron yield in the corresponding place. This supposition is approximately true for 44 and 18 GeV 12C+Cu interactions (Bisplinghoff et al., 1995) and further evidence is shown in this paper in the following paragraph 3.3. From Fig. 1 and Fig. 2 we can see that the neutron yield in Hg target is less than in U/Pb target. Only about half of secondary neutrons are produced in Hg target compared with U/Pb target. Similar measurements were also performed with outer CR-39 detectors for Pb and Hg targets. The track yield ratio of Pb to Hg target is 1.76±0.33 at 1.0 GeV of protons. It means that Hg target produces lesser neutrons than even a Pb target. Hg target is less preferable in order to be used as a target in the reactor from the point of view to get more secondary neutrons.  相似文献   

5.
Summary A search has been made on the charge-changing partial cross-sections by using 0.927 GeV/n238U ion from LBL BEVALAC projected at an angle 30° on27Al target and CR-39 (DOP) was used as analyser. The irradiated plastic sheets were duly etched for one hour in 6.25N NaOH solution and about 1680 cone lengths at both the surfaces of the CR-39 (DOP) sheets were optically measured. The cone length distribution exhibits the existence of U fragments in the charge range 84≤Z≤91 and the estimated partial cross-sections range from 60 to 400 mb. The present data are in accord with the fit to the extrapolated data of Binnset al.  相似文献   

6.
通过CR-39 核径迹探测器对471 AMeV 56Fe 和400 AMeV 20Ne 诱发Al,C 和CH2 靶反应的弹核碎裂反应截面及出射角度进行了测量,并利用改进的量子分子动力学(ImQMD) 模型和描述统计衰变的GEMINI 模型对实验结果进行了分析和讨论。实验结果表明,总反应截面与弹核的能量无关,但随着靶核质量的增加而增加。这与其他的实验结果以及Bradt-Peters 的半经验理论公式所得结果一致。理论计算和实验测量结果中,分截面出现了明显的奇偶效应。理论计算结果表明,奇偶效应主要产生于受激碎块的衰变过程,其中对效应起着重要作用,而且,主要形成于擦边碰撞的反应中且多来自于同位旋为TZ = 0; ±0:5 的弹核碎块的贡献。产生碎块的同位素分布与弹核的种类有关,与入射能量和靶核的种类没有太大依赖性,其较小的偏转角大部分来自于擦边碰撞产生的较重的类弹碎块的贡献。We have measured the fragmentation cross sections and the emission angles for 471 AMeV 56Fe and 400AMeV 20Ne on Al, C and CH2 targets using CR-39 plastic nuclear track detector. The total charge changing cross sections agree well with other previous experimental results at different energies and the theoretical prediction of Bradt-Peters semiempirical formula, which are pproximately independent of the beam energy but increase with the increase of the target mass. The experimental results are compared with the prediction of the improved quantum molecular dynamical model (ImQMD) together with the GEMINI model. The odd-even effect of the partial cross sections observed in experiments is well produced. It is found that such effect is mainly formed in the grazing collisions and comes from the fragments with TZ = 0; ±0:5. The shape of the isotopic distribution is independent on the target mass and the incident energy but the projectile mass and charge, and the small angular distribution of all fragments comes from the heavier projectile-like fragments which produced in the peripheral collision.  相似文献   

7.
《Radiation measurements》1997,28(1-6):455-462
Using CR-39 plastic track detectors the range values of 16O ions at two different energies (initially in the beam line, 39.97 MeV/n and 69.98 MeV/n) were measured after escaping the beam pipe and found to be (3050 ± 40) μm and (8210 ± 90) μm, respectively. The longitudinal and projected angular spread of oxygen ions of an initial energy of 69.98 MeV/n in the region of the Bragg peak was derived from the measured geometrical parameters of tracks. Based on a calibration curve (etch rate ratio vs total linear energy transfer in CR-39) and the measured track length distribution at the range end of oxygen ions, the complete depth dose profile of a 67.7 MeV/n 16O beam in CR-39 (plateau, extended Bragg peak and residual ionization caused by projectile like fragments) was obtained.  相似文献   

8.
Six stacks of nuclear track detectors were exposed in December 1994 to 207Pb82+ ions of 158 A GeV at the CERN-SPS. Each stack was made of CR39 sheets placed after a target. The CR39 was manufactured by the Intercast Europe Co. of Parma (Italy). The exposures were carried out at normal incidence to an average density of 400 ions/cm2. The main purpose of the exposures was the calibration of the CR39 nuclear track detector used in a large area detector to search for magnetic monopoles (experiment MACRO at the Gran Sasso Laboratory). We compare the response of CR39 of different production batches in different etching conditions. The results indicate no relevant aging effect for the CR39 made more than 5 years ago. The first result of a “long period” investigation of possible fading effects for the CR39 is also presented.  相似文献   

9.
A measurement of the double-differential cross-section for the production of charged pions in proton–tantalum collisions emitted at large angles from the incoming beam direction is presented. The data were taken in 2002 with the HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 GeV/c to 12 GeV/c hitting a tantalum target with a thickness of 5% of a nuclear interaction length. The angular and momentum range covered by the experiment (100 MeV/c ≤p< 800 MeV/c and 0.35 rad ≤θ< 2.15 rad) is of particular importance for the design of a neutrino factory. The produced particles were detected using a small-radius cylindrical time projection chamber (TPC) placed in a solenoidal magnet. Track recognition, momentum determination and particle identification were all performed based on the measurements made with the TPC. An elaborate system of detectors in the beam line ensured the identification of the incident particles. Results are shown for the double-differential cross-sections d2σ/dpdθ at four incident proton beam momenta (3 GeV/c, 5 GeV/c, 8 GeV/c and 12 GeV/c). In addition, the pion yields within the acceptance of typical neutrino factory designs are shown as a function of beam momentum. The measurement of these yields within a single experiment eliminates most systematic errors in the comparison between rates at different beam momenta and between positive and negative pion production. PACS 13.75.Cs; 13.85.Ni  相似文献   

10.
Considering the magnetic field response of the QGP medium,we perform a systematical study of the chiral magnetic effect(CME),and make a comparison with the experimental results for the background-subtracted correlator H at the energies of the RHIC Beam Energy Scan(BES)and the LHC energy.The CME signals from our computations show a centrality trend and beam energy dependence that are qualitatively consistent with the experimental measurements of the charge dependent correlations.The time evolution of the chiral electromagnetic current at the RHIC and LHC energies is systematically studied.The dependence of the time-integrated current signal on the beam energy√s with different centralities is investigated.Our phenomenological analysis shows that the time-integrated electromagnetic current is maximal near the collision energy√s≈39 GeV.The qualitative trend of the induced electromagnetic current is in agreement with the CME experimental results at the RHIC and LHC energies.  相似文献   

11.
The Gamma-3 assembly is located at the Joint Institute for Nuclear Research, Dubna, Russia. It consists of a cylindrical lead target (ø = 8 cm, L = 58.8 cm) surrounded by reactor grade graphite (110 × 110 × 60 cm). The target was irradiated with a beam of 1.6 GeV deuterons from the Nuclotron accelerator and CR-39 track detectors coupled to LR-115 2B film were used to measure the slow neutron distribution on the surface of the graphite. The detection efficiency of the CR-39 in the CR-39/LR-115 2B system was measured using a custom made calibration setup and found to be (1.12 ± 0.05) × 10−3 and (6.1 ± 1.2) × 10−4 tracks per neutron, for thermal and epithermal neutrons respectively, under the etching and counting procedures described in this work. The irradiation of the Gamma-3 was also simulated using MCNPX 2.7 Monte Carlo code and good agreement between the experimental and calculated track densities was found. This serves as a good validation for the computational models used to simulate spallation neutron production, transport and moderation.  相似文献   

12.
Summary Final results of the experiment for the estimation of charge abundances using plastic emulsion chamber consisting of CR-39 (HCB) and Fuji ET-7B nuclear-emulsion sheet, launched from Alice Springs for 32 hours at an atmospheric depth of 9.8 g cm−2 is presented. The latest long hour etching technique was used for track detection in plastics. The estimated reduced etch rate distribution presented was based on 2968 measured track diameter data in CR-39 (HCB) stacks. The observed charge spectrum from the reduced etch rate distribution was duly corrected for the top of the atmosphere by adopting the conventional formulation for cosmic-ray propagation along with the latest modified partial cross-sections for A-A collisions after Tsaoet al. The average value of the observed energy of the 77 very heavy primaries was estimated from the opening angle measurements of alpha fragments in Fuji ET-7B nuclear emulsion and was found to be 5.01 GeV/n which comes out to be 8.2 GeV/n, when corrected for the top of the atmosphere due to propagation in the residual atmospheric depth. The measured integral fluxes for NeMgSi and Fe groups above 4 GeV/n have been compared with the global data surveyed by Ichimuraet al. Our results on element/Si and element/Fe have been compared with the HEAO-3-C2 data after Englemannet al. Using SSLB model, the source abundance is derived from the observed result and that was compared with the results of Juliusson,et al., Lezniak and Webber and Garcia-Munozet al.  相似文献   

13.
We present a measurement of the longitudinal spin asymmetry A(||) in photoproduction of pairs of hadrons with high transverse momentum p(T). Data were accumulated by the HERMES experiment using a 27.5 GeV polarized positron beam and a polarized hydrogen target internal to the HERA storage ring. For h(+)h(-) pairs with p(h(1))(T)>1.5 GeV/c and p(h(2))(T)>1.0 GeV/c, the measured asymmetry is A(||) = -0. 28+/-0.12(stat)+/-0.02(syst). This negative value is in contrast to the positive asymmetries typically measured in deep inelastic scattering from protons, and is interpreted to arise from a positive gluon polarization.  相似文献   

14.
The depth-dependent bulk etch rate has been examined for the gamma-irradiated CR-39 at doses ranging from 20 to 100 kGy. The thickness of the damaged region in gamma-irradiated CR-39 plastics, in which the bulk etch rate was significantly enhanced, was found to be limited in the thin layer near the surface and decreases with increasing the dose-rate, while it barely depend on the total dose. This indicates that it is possible to apply CR-39 plastics as high dose gamma-dosimeter by assessing both the bulk etch rate in the damaged region and its thickness in principle.  相似文献   

15.
Experiments have been carried out to study the ‘heavy fragments’ emitted at wide angles in the interaction of 3.65 A GeV 16O ions with a thick Cu target, using a stack of CR-39 track detectors. Diametric distribution in a stack registering 16O-beam halo are compared with diameters observed in a stack placed downstream at an angle of 25°. There is a strong indication that the heavy fragments are scattered at large angles.  相似文献   

16.
Within the framework of the study of the behaviour of relativistic particles formed in the interaction of 65 GeV 19F-ions and a 1 cm thick Cu target, the wide angle emission of heavy fragments has been studied using CR-39 (INTERCAST) as a detector.  相似文献   

17.
Summary A detailed study on the relative abundances of very heavy elements of cosmic rays with charges 10≤Z≤28 in the interstellar medium has been estimated from the results obtained from the balloon-borne passive-detector experiments flown for 32 hours from Alice Springs. The recovered CR-39 (HCB) detectors were etched for 96 hours in 7.5N NaOH solution at 80°C. About 2126 elliptic etch pit cones were scanned from the 250 cm2 area of the track detector and the chemical abundances of elements with charges 10≤Z≤28 above 2 GeV/n have been estimated. We have adopted the charge-changing cross-sections calculated from the abrasion/ablation model after Norbury and duly fitted in the slab model to account for the loss of intensity due to nuclear fragmentation in the upper atmosphere. The predicted source composition is comparable with the derived result of Lezniak and Webber. Our result on (Sc−Cr)/Fe flux ratio at 6.52 GeV/n energy is in accord with the results derived from the leaky-box model.  相似文献   

18.
A technique based on the optical density (D) measurement of the etched track is useful for charged particles spectroscopy using SSNTD. It was shown that the stopping power of alpha particles in CR-39 is proportional to D. We measured the optical density and derived an expression to estimate the range of alpha particles in CR-39 detector as a function of the bulk etching rate and etching time. The relation between the etching time, track parameters (depth, radius) and D for different alpha particles energy and etching conditions were studied. A relation describing D as a function of track size is proposed.  相似文献   

19.
We have measured the total and partial charge-changing cross-sections (Z=5) after the passage of a 110 MeV/u 12C beam through an assembly consisting of CR-39 thin detectors and paraffin targets. These experimental cross-sections were compared to the predictions of known models. It was found that the measured total cross-sections agree with the model calculations to within about 8% or even less, while, depending on a model, discrepancies of up to a factor 1.2 higher and up to a factor 2.7 lower values of cross-sections for the production of fragment with Z=5 were observed.  相似文献   

20.
A non-contact and simple interferometric technique has been used to measure the refractive index variation of gamma irradiated CR-39 polymer samples. Six samples of thickness (750 μm) and dimensions of 1.5 × 3 cm2, have been irradiated with gamma radiation doses in the range from zero to 600 kGy. It is observed that the refractive index increases by increasing the dose and reaches its maximum value at 40 kGy dose, and then starts to decrease again. This means that the gamma radiation deformation in the CR-39 polymer is a chain scission effect. This interferometric technique could make a contribution to recombination and degradation mechanisms on CR-39 polymer.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号