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
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共查询到18条相似文献,搜索用时 15 毫秒
1.
We report on the cw-laser fabrication of sharp-edged holes and grooves in organic-dye-sensitized photoresists for g-line or i-line by manipulating its intensity and scanning rate. The laser fabrication is performed to locally control the reaction time constant of the photoresist. By scanning a tightly focused laser focal spot inside the transparent photoresist, various micron/submicron meter structures have been produced based on the reaction time constant depending on the beam intensity. The proposed method is considered to be a cost-effective technique for high-aspect-ratio holes and grooves fabrication. 相似文献
2.
S. -L. Guo L. Li Q. -B. Shen Y. -Q. Shi R. Brandt P. Vater J. S. Wan W. Ensinger B. A. Kulakov M. I. Krivopustov A. N. Sosnin V. Bradnova 《Radiation measurements》2001,34(1-6):301-304
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: Full-size image Article Outline
1. IntroductionThe 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. ExperimentsThe 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. Results3.1. Neutron yield of Hg targetThe 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3.
Study of initial shock wave in exhausted flow field by use of a Laser Moire Deflectometry instrument
The initial show wave is a non-stationary phenomenon in the initial stage of an exhausted flow field. Its movement characteristic and development process cannot be mastered accurately with the use of contact-type measurement methods, such as pressure and velocity measurements. An experimental study of the shock wave field by use of a Laser Moire Deflectometry instrument is introduced in this paper. The instrument has a large caliber, high sensitivity and high precision. A serial photograph of shock wave field is also presented. The formation mechanism and development trend of the initial shock wave can be drawn from analysis of flow field display photographs. 相似文献
4.
Mollenauer LF Mamyshev PV Gripp J Neubelt MJ Mamysheva N Grüner-Nielsen L Veng T 《Optics letters》2000,25(10):704-706
By combining a special dispersion map that has nearly constant path-average dispersion, a hybrid amplification scheme involving backward-pumped Raman gain, and sliding-frequency guiding filters, we have demonstrated massive wavelength-division multiplexing at 10 Gbits/s per channel, error free (bit-error rate, =1x10(-9) for all channels), without the use of forward error correction, over greater than 9000 km, using dispersion-managed solitons. The number of channels (27) was limited only by a temporary lack of amplifier power and gain flatness. Terabit capacities are to be expected in the near future. 相似文献
5.
K. B. Gikal Yu. G. Teterev M. V. Zdorovets I. A. Ivanov M. V. Koloberdin S. G. Kozin 《Physics of Particles and Nuclei Letters》2016,13(2):198-203
The yields of neutrons produced in thick LiF, Be, C, Al, Al2O3, and Cu targets irradiated by Li, C, and N ions with energies below 1.75 MeV/nucleon are measured on the DC-60 cyclotron at the Institute of Nuclear Physics, Astana Branch, Kazakhstan. The experimental angular distributions of the neutron yields from the targets are measured and an empirical equation to describe the distributions is proposed. The measured neutron yields are compared with the figures calculated by the LISE++ program. The measured and predicted neutron yields in the reactions coincide to within a factor of 2. 相似文献
6.
We show how replacement of a modest fraction of the usual fiber-based dispersion compensation with a periodic-group-delay dispersion-compensating module can result in a drastic reduction in collision-induced timing jitter in dense wavelength-division multiplexing with dispersion-managed solitons. The principal mechanism here is a correspondingly large reduction in the net path over which a pair of colliding pulses interact. 相似文献
7.
M. Temporal S. Atzeni D. Batani M. Koenig 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2000,12(3):509-511
The impedance mismatch effect in a two-layer (low density plastic foam, and solid aluminum, respectively) plane target compressed
by a laser driven shock wave is considered. In such targets the ablative pressure generated by absorption of laser light in
the foam layer is amplified when crossing the foam-aluminum interface. In this paper an analytical model is developed to evaluate
the shock pressure in the aluminum layer as a function of the density and thickness of the foam layer and of the laser parameters.
The model is in good agreement with previously published experimental results [A. Benuzzi et al., Phys. Plasmas 5, 2827 (1998)].
Received 20 January 2000 and Received in final form 16 May 2000 相似文献
8.
Experimental observation of ionization and shock fronts in foam targets driven by thermal radiation 下载免费PDF全文
The behaviours of ionization and shock propagation in
radiatively heated material is crucial for the understanding of
indirect drive inertial confinement fusion as well as some
astrophysics phenomena. In this work, radiation field with a peak
temperature of up to 155 eV was generated in a gold cavity heated by
four laser beams on the SG-II laser system and was used to irradiate
a plastic foam cylinder at one end. The radiatively ablated foam
cylinder was then backlighted side-on by x-ray from a
laser-irradiated Ti disk. By observing the transmission decrease due
to the shock compression of the foam cylinder, the trajectories of shock
front were measured, and from the onset of the intense thermal
emission from the side of the cylinder, the propagations of
the ionization front were also observed on the same shot. The
experimental measurements were compared to predictions of the
radiation hydrodynamics code Multi-1D and reasonable agreements were
found. 相似文献
9.
A. A. Andreev S. Yu. Gus’kov D. V. Il’in A. A. Levkovskii V. B. Rozanov V. E. Sherman O. B. Vygovskii 《Journal of Experimental and Theoretical Physics》2003,96(4):695-703
One-dimensional numerical calculations were performed to study the dependence of conditions for initiating thermonuclear combustion and of the target gain of direct-ignition inertial fusion targets ignited by a short radiation pulse on the initial temperature of a preliminarily compressed fuel and the initial heat energy distribution between plasma electrons and ions in the ignition region (igniter). The igniter parameters at which an effective thermonuclear target explosion with a G ~ 103 target gain occurred were shown to substantially depend on the initial temperature of the major fuel fraction and the initial heat energy distribution between igniter electrons and ions. The heat energy of the igniter passed a minimum as the size of the igniter decreased. The dependences of these minimum energies on the temperature of the major fuel fraction at various initial energy distributions between igniter electrons and ions were determined. An increase in the temperature of the major fuel fraction was shown to decrease the target gain. 相似文献
10.
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12.
We demonstrate the generation of high-energy picosecond pulses directly from a thin-disk laser oscillator by employing a self-imaging active multipass geometry. Stable single-pulse operation has been obtained with an average output power in excess of 50 W, excluding a cw background of 8%, at a repetition rate of 3.8 MHz. Self-starting passive mode locking was accomplished using a semiconductor saturable absorber mirror. The maximum pulse energy was 13.4 microJ at a pulse duration of 1.36 ps with a time-bandwidth product of 0.34. Single-pass external frequency doubling with a conversion efficiency of 60% yielded >28 W of average power at 515 nm. 相似文献
13.
We investigate the extreme-ultraviolet (EUV) emission from targets that contain tin as an impurity and the advantages of using these targets for ion debris mitigation by use of a magnetic field. The EUV spectral features were characterized by a transmission grating spectrograph. The in-band EUV emission energy was measured with a calorimeter of absolute calibration. The ion flux coming from the plume was measured with a Faraday cup. Our studies indicate that 0.5% Sn density is necessary to obtain a conversion efficiency very close to that of full-density Sn. The use of Sn-doped low-Z targets provides a narrower unresolved transition array and facilitates better control of energetic ions in the presence of a moderate magnetic field of 0.64 T. 相似文献
14.
Kulcsar G AlMawlawi D Budnik FW Herman PR Moskovits M Zhao L Marjoribanks RS 《Physical review letters》2000,84(22):5149-5152
We describe the optical, radiative, and laser-plasma physics of a new type of nanostructured surface especially promising as a very high absorption target for high-peak-power subpicosecond laser-matter interaction. This oriented-nanowire material, irradiated by 1 ps pulses at intensities up to 10(17) W cm(-2), produces picosecond soft x-ray pulses 50x more efficiently than do solid targets. We compare this to "smoke" or metallic clusters, and solid nanogroove-grating surfaces; the "metal-velvet" targets combine the high yield of smoke targets with the brief emission of grating surfaces. 相似文献
15.
S. E. Chigrinov K. K. Gudima A. I. Kievitskaya V. A. Petlitsky 《Hyperfine Interactions》1993,77(1):149-159
In this paper, we present a model of calculation with respect to the interactions of high-energy nuclei with matter. Based
on this model, we obtain results on energy and angular spectra of the n- and π−-particles produced in collisions of deuterium and tritium nuclei at energiesT
d=1 GeV/nucleon with light targets such as Li, Be. We have also estimated the production yields of neutrons and π−-mesons in targets of various radii, as well as mean energies of these these particles. Summarizing, we find that the lithium
target of radiusR=10−12 cm for which the energy cost επ to produce one π−-meson is estimated as 6.7 GeV/π for a d-beam and 5.3 GeV/π for a t-beam is the most preferred pion-production target. 相似文献
16.
Fluctuations of the fission neutron multiplicity and prompt γ-ray energy have been measured for resonance neutron induced fission of 239Pu below 110 eV. An observed anticorrelation between fluctuations of these two parameters is attributed to the role of the (n, γf) reaction. 相似文献
17.
Calcium ions are laser cooled in a Paul trap by use of a grating-stabilized UV laser diode. Unusual quantum jumps or fluctuations in the fluorescence signal are observed without application of any shelving lasers. It has become clear that such phenomena can be ascribed to shelving transitions induced by background 393-nm spontaneous photons emitted from the laser medium. Shelving transitions are suppressed by use of an interference filter, and the ions are successfully cooled to crystallization temperature with sufficient reproducibility. 相似文献
18.
用数值模拟的方法,给出了一种适合以纳秒级的高功率钕玻璃激光系统为抽运源的光学参量啁啾脉冲放大(OPCPA)系统的最优化设计.该系统主要由一级LBO预放大器和一级LBO主放大器组成.数值模拟结果表明该系统能够把纳焦级能量的飞秒脉冲放大到焦级,从而产生几十个太瓦(1012W)的脉冲输出.这一结果为进一步利用OPCPA技术放大飞秒脉冲产生拍瓦(1015W)的超短超强激光脉冲输出奠定了基础,从而为强场科学研究提供崭新的技术手段. 相似文献
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