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1.
The results of an experimental work aimed at improving the performance of the CR-39 nuclear track detector for neutron dosimetry applications are reported. A set of CR-39 plastic detectors was exposed to 252Cf neutron source, which has the emission rate of 0.68 × 108 s−1, and neutron dose equivalent rate 1 m apart from the source is equal to 3.8 mrem/h. The detection of fast neutrons performed with CR-39 detector foils, subsequent chemical etching and evaluation of the etched tracks by an automatic track counting system was studied. It is found that the track density increases with the increase of neutron dose and etching time. The track density in the detector is directly proportional to the neutron fluence producing the recoil tracks, provided the track density is in the countable range. This fact plays an important role in determining the equivalent dose in the field of neutron dosimetry. These results are compared with previous work. It is found that our results are in good agreement with their investigations.   相似文献   

2.
A review was given for our recent studies on the latent tracks in CR-39 nuclear track detector. The radial size of track core has been determined through UV spectral measurements combined to the model of track overlapping and by AFM observations of slightly etched detectors. The track core radius was found to be about a few nano-meters and almost proportional to the cubic root of stopping power. As a control study, the etching properties of CR-39, irradiated by low-LET radiation, has been examined. The observed depth dependence and dose-rate dependence of the bulk etch rate of the irradiated CR-39 were explained that the damage formation process was governed by the reaction between the radiation induced radicals and the oxygen supplied from the air. This indicated that latent tracks in CR-39 are produced through local radiation induced oxidation process along the ion paths. Studies on vibration spectra, near-IR, FT-IR and Raman spectra, of CR-39 have also been carried out to estimate the chemical structure of the latent tracks. The creation of OH group in irradiated CR-39 has been confirmed.  相似文献   

3.
Neutron detection with a stack of two detector foils of CR-39 (intercast) was studied. A comparison between the experimental results (exposure to 14.8 MeV neutrons) and the results of a computer simulation was performed. Emphasis was given to the detection of particles—products of the break-up reaction of the 12C nucleus—and to heavier recoil nuclei. The detectors were chemically etched and analysed with an automatic counting system. All detector surfaces were analysed, and the coincidence tracks produced by the same particles on detector surfaces in contact were determined. These tracks facilitate characterization of the type and energy of the recoil nuclei. Further separation was made on the basis of the distribution of size and darkness of the tracks.  相似文献   

4.
We have exposed stacks of CR-39 plastic nuclear track detectors inside the MIR space craft during the EUROMIR95 space mission for almost 6 months. Over this long period a large number of tracks of high LET events was accumulated in the detector foils. The etching and measuring conditions for this experiment were optimized to detect tracks of stopping iron nuclei. We found 185 stopping iron nuclei inside the stack and identified their trajectories through the material of the experiment. Based on the energy-range relation the energy at the surface of the stack was determined. These particles allow the determination of the low energy part of the spectrum of iron nuclei behind shielding material inside the MIR station.  相似文献   

5.
Systematic measurements of swelling of CR-39 nuclear track detector (NTD) due to irradiation with fission fragments and alpha particles over a wide range of fluences from 252Cf are presented here. Precisely designed and optimized exposure and chemical etching experiments were employed to unfold the structure of radiation induced surface damage. Delays in the startup of the chemical etching of latent tracks in low radiation fluence detectors are measured and are found to contain important information about structure of the surface damage. Simple atomic scale pictures of radiation induced surface damage and its chemical etching are developed using measurements of radiation induced swelling of CR-39 detectors and nuclear track parameters. The computer code SRIM2010 was utilized for the calculations of basic features of latent tracks of fission fragments and alpha particles in CR-39. Another computer code TRACK_VISION was used to compute parameters of etched tracks. Computations and experimental findings in the paper coherently compose a realistic picture of radiation damage.  相似文献   

6.
CR-39 nuclear track detectors have been used as an efficient radon monitoring system. Exposing these detectors to radon would result in tracks where ever particles hit the surface of the detector. Natural radioactivity of alpha particles (radon concentration) is measured based on the count of these tracks on CR-39 detector. Counting these tracks by eye is not an easy task especially when the density of the tracks is high. Automated tracks counting systems are attractive solution for this problem. However, as the density of tracks increases the accuracy of these methods deteriorates. This is due to the fact that overlapped tracks are counted as one track during the segmentation process resulting in an underestimation of the real count of the tracks. This work proposes a new image processing based automated approach for tracks counting. This new automated approach solves the problem of counting overlapping tracks by approximating their number and then adjusting the final count of tracks by compensating for those uncounted tracks. The experimental results show that the proposed approach reduces the counting percentage error from 5.64% to 2.54% by solving the counting problem of the overlapped tracks.  相似文献   

7.
Track etch rate characteristics of CR-39 plastic detector exposed to 28Si ions of 670 MeV energy have been investigated. Experimental results were obtained in terms of frequency distribution of the track diameter, track density and bulk etching rate. A dependence of the mean track diameter on energy was found. The application of the radiation effect of heavy ions on CR-39 in the field of radiation detection and dosimetry are discussed. Results indicated that it is possible to produce etchable tracks of 28Si in this energy range in CR-39. We also report the etching characteristics of these tracks in the CR-39 detector.  相似文献   

8.
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   

9.
Stacks of CR-39 plastic nuclear track detectors were mounted inside the MIR spacecraft during the EUROMIR95 space mission for a period of 6 months. This long exposure time resulted in a large number of tracks of HZE-particles in the detector foils. All trajectories of stopping iron nuclei could be reconstructed by optimizing the etching conditions so that an automatic track measurement using image analysis techniques was possible. We found 185 stopping iron nuclei and used the énergy-range relation to calculate their energies at the stack surface. The measured spectrum of iron nuclei inside the MIR station is compared to results of model predictions considering the effect of the solar modulation for the mission period, the geomagnetic shielding effect for the MIR orbit and the shielding by material of the spacecraft walls and its instrumentation.  相似文献   

10.
翟鹏济 《物理》2000,29(7):397-400,392
介绍了一种核径迹探测器CR-39塑料的特性,这种探测器对逞电粒子非常灵敏,它还具有稳定、透明等特点,可记录p、a粒子,裂变碎片和其他带电粒子,它是现有固体核径迹探测器中能量沉积密度探测阈最低的材料,介绍了CR-39对带电粒子的响应,给出了各种带电粒子的vT对限定能量损失(REL)的响应曲线,利用CR-39与转换屏的组合还可测定能量范围广的中子能谱,可作为方便的个人中子剂量计,介绍了CR-39在研究  相似文献   

11.
The ray tracing method was applied to study etched tracks from α-particles in CR-39 solid-state nuclear track detectors. The transmission mode of a microscope operation was simulated. A track was considered as a set of small triangular elements, and the brightness of all elements was calculated systematically through the entire track to create the final image. Preliminary results are given for α-particle tracks in the CR-39 detector for initial energies of 4 and 4.5 MeV, and incident angles of 40 and 90°, respectively. Total reflection, as well as the slope of a surface element in the track wall, were identified as the main factors that affect the brightness of that element. At this stage, comparisons with experimental results can be made in terms of the average grey levels for the entire tracks.  相似文献   

12.
The effects of storage temperatures on the track registration of CR-39 as a solid state nuclear track detectors have been investigated. The results show that the storage CR-39 detectors cause partial or complete removal of tracks depending on storaged time and temperatures. The bulk activation energy for CR-39 has been found to be 0.883 eV.  相似文献   

13.
A better understanding of the background of CR-39 detectors   总被引:1,自引:0,他引:1  
The background of CR-39 detectors varies from batch to batch, from foil to foil in the same batch, from one side to another of the same foil and within the same foil surface. In spite of many efforts made in the past, little success has been achieved in producing detectors with a consistently low background. For this reason, new investigations have been undertaken with the specific scope in mind to improve the background of these detectors. The key strategy of these studies was to investigate whether the background tracks originate from the detector surface or from detector bulk, if not from both. From these systematic investigations it was possible to demonstrate that most of the background is due to defects present on the detector surface. For this reason, the simplest way to reduce the background is to carry out a heavy pre-etching prior to the use of the CR-39 detector. This procedure has been successfully exploited not only to increase the signal-to-noise ratio of CR-39-based radon dosimeters but also to carry out different radon measurements with the same CR-39 foil.  相似文献   

14.
In this paper, we study the thermal annealing of proton tracks of 4 and 6 MeV at temperatures ranging from 150 to 240°C in CR-39 polymer detectors. A special experimental set-up for irradiating the detectors was arranged to obtain adequate proton beams from the Cyclotron CV-28 at IPEN/SP, Brazil. We report experimental data on track densities, track diameters, and activation energies based on current annealing models for the annealing of proton tracks in the energy range investigated. A value of (0.20±0.02)eV was determined as the mean activation energy of the annealing process in CR-39 detectors.  相似文献   

15.
Two techniques have been developed to investigate the characteristic of the sensitivity of CR-39 (polyallyldiglycol carbonate) track detector using Am---Be neutron source. The firstis to measure volume track density created by fast neutrons in CR-39 detectors. The second is to measure areal asymptotic track density on the surface of CR-39 sheets. Two types of CR-39—SY-2 CR-39 made in China and another made in USA were calibrated using the techniques. It shows that the two types of CR-39 detectors have nearly the same sensitivity to detect fast neutrons. The techniques developed in this work can be applied to calibration of other track detectors.  相似文献   

16.
Space radiation dosimetry measurements have been made on board the Space Shuttle STS-65 in the Second International Microgravity Laboratory (IML-2). In these measurements, three kinds of detectors were used; one is a newly developed active detector telescope called “Real-time Radiation Monitoring Device (RRMD)” utilizing silicon semi-conductor detectors and others are conventional detectors of thermoluminescence dosimeters (TLDs) and CR-39 plastic track detectors. Using the RRMD detector, the first attempt of real-time monitoring of space radiation has been achieved successfully for a continuous period of 251.3 h, giving the temporal variations of LET distribution, particle count rates, and rates of absorbed dose and dose equivalent. The RRMD results indicate that a clear enhancement of the number of trapped particles is seen at the South Atlantic Anomaly (SAA) without clear enhancement of dose equivalent, while some daily periodic enhancements of dose equivalent due to high LET particles are seen at the lower geomagnetic cutoff regions for galactic cosmic ray particles (GCRs). Therefore, the main contribution to dose equivalent is seen to be due to GCRs in this low altitude mission (300 km). Also, the dose equivalent rates obtained by TLDs and CR-39 ranged from 146.9 to 165.2 μSv/day and the average quality factors from 1.45 to 1.57 depending on the locations and directions of detectors inside the Space-lab at this highly protected orbit for space radiation with a small inclination (28.5°) and a low altitude (300 km). The LET distributions obtained by two different detectors, RRMD and CR-39, are in good agreement in the region of 15–200 keV/mm and difference of these distributions in the regions of LET < 15 keV/mm and LET > 200 keV/mm can be explained by considering characteristics of CR-39 etched track formation especially for the low LET tracks.  相似文献   

17.
《Radiation measurements》2007,42(8):1332-1334
The elastic scattering of light nuclei, especially hydrogen, is widely used for detection of fast neutrons. Fast neutrons have a few interactions in solid state nuclear track detectors (SSNTDs), such as CR-39. It has been shown that to increase the efficiency of detector, a radiator layer, e.g. polyethylene may be used. In this work, the optimum thickness of the radiator layer has been determined. Some different thicknesses of aluminium layers have been used as discriminators for which the efficiency of detector to Am–Be neutron source has been calculated. A program FTRAC has been developed for the calculation of the detection efficiency. This software determines the specifications of recoil protons (using PTRAC card of MCNP code) and also the kinematics of interactions. Transport of recoil protons has been carried out using SRIM Monte Carlo code. A good agreement have been shown between measurement and simulation results.  相似文献   

18.
To measure the energy spectra of low energy ions inside the International Space Station (ISS) we will expose three stacks of CR-39 plastic nuclear track detectors aligned to the three coordinate axes of the space station. The energies of cosmic ray nuclei at the stack surfaces can be determined by reconstructing the trajectories of ions stopping inside the detector material and by measuring their ranges. To measure only HZE (high charge Z and energy E) ions with charges of Z6 stopping in our experiment a special batch of CR-39 detectors with low sensitivity will be used. This detector material has been already tested by an exposure to carbon ions at the GSI accelerator in Darmstadt, Germany.  相似文献   

19.
CR-39 plastic nuclear track detector is used to measure the fraction of alpha-particle tracks due to radon daughters activities plated-out on the internal walls of a cylindrical-shaped plastic can. Radium chloride solution is used as a radon source, the exposure time is ranged from 4 hours to 3 days. To assess the percentage of plate-out effect on CR-39 nuclear track detector, two different methods were used. In one experiment, a few circular parallel pairs of CR-39 sheets were hanged in the can device. In the other experiment, the estimation of the plate-out effect has been performed, after exposure to the radon source, by detecting tracks with a second unexposed sheet placed in close contact to the exposed wall and detectors. In the two methods, it was found that the chemically etched tracks related to plated-out activities contribute about 50% of the measured alpha-particles tracks.

Der CR-39 Plast-Kernspurdetektor wurde zur Messung des Anteils an Spuren von Alphateilchen verwendet, die sich von den Radon-Tochterprodukten ergeben und auf den Innenwänden eines zylindrisch gestalteten Plastbehälters abgeschieden haben. Als Radonquelle wurde eine Radiumchlorid-Lösung verwendet und die Expositionszeiten lagen zwischen 4 Stunden und 3 Tagen. Um den Anteil des Abscheidungseffektes in einem CR-39 Spurdetektor zu bestimmen, wurden zwei unterschiedliche Methoden angewendet. In dent einen Versuch wurden einige zylindrische Parallelpaare von CR-39 Folien in den Behälter gehängt. In dent anderen Versuch wurde der Abscheidungseffekt in der Weise ermittelt, daβ nach der Exposition auf die Radonquelle mit einer zweiten nichtexponierten Folie die Spuren bestimmt wurden. Die nichtexponierte Folie war dabei in einem engen Kontakt zur exponierten Wand und den Detektoren. Durch beide Methoden wurde gefunden, daβ die chemiseh geätzten Spuren, die auf die Abscheidimgsaktivitäten züruckgeführt werden können, einen ungefahren Anteil von 50% an den gemessenen Alphateilchenspuren ausmachen.  相似文献   

20.
In this paper, cellular automata are used to detect the nuclear tracks in the track images captured from the surface of CR-39 detectors. Parameters of the automaton as the states, neighborhood, rules and quality parameters are defined optimally for the track image data set under analysis. The presented method is a supervised computational algorithm which comprises a rule definition phase as the learning procedure. Parameter optimization is also performed to adapt the algorithm to the data set used.  相似文献   

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