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1.
The magnetic dipole moment of114Sb has been measured using on-line nuclear orientation (OLNO) at the UNISOR Nuclear Orientation Facility (UNISOR/NOF). The value was determined to be 1.72 (8) nuclear magnetons. The observed anisotropy of the 1299 keV transition was fitted as a function of temperature making allowance for incomplete thermalization of the114Sb nuclei prior to decay. The relaxation constant, Ck, is discussed, as is the ground state structure of114Sb.  相似文献   

2.
The performance of two external plastic scintillator detectors has been tested in an off-line mode using a source of106RuFe at UNISOR/NOF. The measurement of beta asymmetries at various temperatures has resulted in the reproduction of the previously-determined magnetic dipole moment for the 1+ ground state of106Rh and in addition the conclusion that the sign of this moment is positive.  相似文献   

3.
The184Au→184Pt decay, studied on-line with the UNISOR facility at HHIRF, is discussed. Gamma-ray and conversion-electron spectroscopy of184Pt as well as on-line nuclear orientation measurements of184Au were done. A new low-lying level scheme of184Pt is proposed. Two coexisting bands with different deformations and their respective γ-vibrational bands are established. Internal conversion coefficients for interband transitions between states with the same spin are extracted from the spectroscopy measurements. The relative E0 contents of the transitions are determined by combining internal conversion coefficients with E2/M1 mixing ratios deduced from gamma-ray anisotropies measured from oriented nuclei.  相似文献   

4.
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6.
The design of a simple and inexpensive3He insert for the existing ac susceptometer is described. The system uses a home built mutual inductance bridge for the ac susceptibility measurements from 0·4 K to 300 K. Simple and inexpensive design with the top loading facility are the main features of this set up. The insert can also be used as a continuously3He operating refrigerator down to 0·5 K.  相似文献   

7.
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   

8.
The Daresbury On-Line Isotope Separator (DOLIS) has recently been commissioned, in conjunction with the Nuclear Structure Facility (NSF) 20 MV tandem accelerator, and a3He-4He dilution refrigerator. First experiments are concentrating on a study of the decay of the neutron deficient iodine isotopes, extracted from a FEBIAD ion source and implanted at 60 keV into an iron host at 15 mK. As well as measuring iodine magnetic moments, the role of proton excitations across the Z=50 shell gap is being investigated in the even-even tellurium daughter nuclei. An on-line laser facility is also being developed, and first measurements have been made for unstable samarium isotopes  相似文献   

9.
Various isotopomers of the mercury hydride radical (HgH) have been generated in a microwave discharge and trapped in neon and argon matrices at 4 K for electron spin resonance (ESR) investigations. Both the dipolar (Adip) and isotropic (Aiso) components of the nuclear hyperfine interactions have been directly measured for 199Hg, 201Hg, H and D. Electronic structure information for HgH in its X2Σ ground state obtained from the hyperfine data is compared with theoretical results from several different computational methods. The hyperfine interactions in HgH are unusually large with Aiso(199Hg) = 6859(3), Adip(199Hg) = 446(3), Aiso(H) = 730(2) and Adip(H) = 0(2) MHz. A standard analysis of the hyperfine interactions demonstrates the need for a more in-depth theoretical treatment of HgH that should include relativistic effects. An interesting shift in spin density is observed when deuterium replaces hydrogen in HgH. The decreased spin density on deuterium, which was demonstrated in earlier studies, can now be more fully investigated since these new measurements confirm an associated increase in spin density on mercury  相似文献   

10.
Neutron rich205Hg (T 1/2=5.2 min) was produced and on-line mass separated at the ISOLDE facility at CERN. The polarization achieved by optical pumping via the atomic line (6s 21 S 0?6s6p 3 P 1,λ=2 537Å) was monitored by theβ decay asymmetry. Hyperfine structure and isotopic shift of the205Hg absorption line was determined by Zeeman scanning. In addition a magnetic resonance was performed on the polarized205Hg nuclei in the atomic ground state. The results are: \(I(^{205} Hg) = \tfrac{1}{2}\) (confirmed);μ I (205Hg)=0.5915 (1)μ N (uncorrected for diamagnetism); isotopic shiftδv204/205=v(205Hg)-v(204Hg)=?1.8 (1) GHz.μ I and IS are discussed briefly in the frame of current literature.  相似文献   

11.
Isotope shifts of the neutron-deficient thallium isotopes were measured on-line at the UNISOR mass separator. Spectroscopy was carried out using collinear fast beam laser spectroscopy in neutral thallium. The changes of the mean square charge radii were derived from the measurements. The changes in charge radii of the I=7 isotopes, including the newly measured188Tl, are compared to the results in mercury and lead.  相似文献   

12.
With the availability of modern isotope separator on-line systems it has become possible to make broad and systematic studies of low-energy low-spin nuclear structure. A vital ingredient in such a program is unique spin-parity assignments to all low-lying levels. A most desirable complement to spin-parity information is detailed spectroscopic information. Obtaining such information far from stability is difficult because of low activity production. Nuclear orientation provides a means for obtaining spin assignments usingsingles measurements. This is less demanding on source intensities than - angular correlation coincidence measurements. Further, nuclear orientation can provide information on magnetic moments and on multipole mixing ratios. A number of structural problems are discussed: the need for unique spin assignments in systematics schemes; the need to distinguish between E2+E0 and M1 transitions; the importance of measuring E2-M1 mixing ratios; and the value of magnetic moment information. Particular emphasis is placed on the desirability of obtaining such information in the neutron-deficient Pt, Au, Hg, Tl, Pb and Bi isotopes, based upon the experimental program at the UNISOR facility.Work supported in part by U.S.Dept. of Energy, Contract No. DE-AS05-80ER10599.  相似文献   

13.
POLAREX (POLARization of EXotic nuclei) is a new facility for the study of nuclear magnetic moments and decay modes of exotic nuclei using the established On-Line Nuclear Orientation (OLNO) method. A radioactive beam of interest is implanted into a ferromagnetic host foil held at a temperature of order 10mK in a 3He - 4He dilution refrigerator. The foil is magnetized by an applied magnetic field and the nuclear spins become polarized through the internal hyperfine field. The angular distribution of decay products from the polarized sample is measured. Accurate values of nuclear moment are obtained by NMR. The new facility will have access to neutron-rich nuclides produced at the ALTO facility (Linear Accelerator at Orsay Tandem) by fission induced by electrons from the linear electron accelerator. Basic concepts and initial tests are outlined.  相似文献   

14.
A large electric hyperfine alignment of 197Au nuclei has been observed by Mössbauer absorption measurements of the 77.3 keV γ-transition of 197Au in diamagnetic KAu(CN)2. the measurements were extended down to 36 mK by employing a 3He/4He dilution refrigerator. The nuclear spin-lattice relaxation time was estimated from the time dependence of the asymmetry in Mössbauer spectra. It is shown that the spectra of oriented specimen can be used for determination of the recoilless factor of the absorber.  相似文献   

15.
A new version of integrated target-ion source unit (ionising target) has been developed for the on-line production of radioactive single-charged ions. The target is able to withstand temperatures up to 2500 °C and acts also as an ion source of the surface and laser ionisation. Off-line and on-line experiments with the ionising target, housing tantalum foils as a target material, have been carried out at the IRIS (Investigation of Radioactive Isotopes on Synchrocyclotron) facility. The off-line surface ionisation efficiency measured for stable atoms of Li, Rb and Cs was correspondingly 6% , 40% and 55% at the target temperature of 2000 °C and 3-10% for atoms of rare-earth elements Sm, Eu, Tm and Yb at a temperature of 2200 °C. The off-line measured values of the ionisation efficiency for stable Gd and Eu atoms by the laser beam ionisation inside the target were 1% and 7%, respectively. The radioactive beam intensities of neutron-deficient rare-earth nuclides from Eu to Lu produced by the integrated target-ion source unit have been measured at a temperature of 2500 °C. The results of the integrated target-ion source unit use for on-line laser resonance ionisation spectroscopy study of neutron-deficient Gd isotopes have been also presented.  相似文献   

16.
Recently, two experiments were concluded in Hall A at Jefferson Lab which utilized a newly assembled, solid, polarized hydrogen target. The primary components of the target are a new, high cooling power 4He evaporation refrigerator, and a re-purposed, superconducting split-coil magnet. It has been used to polarize protons in irradiated NH3 at a temperature of 1 K and at fields of 2.5 and 5.0 tesla. Maximum polarizations of 55% and 95% were obtained at those fields, respectively. To satisfy the requirements of both experiments, the magnet had to be routinely rotated between angles of 0°, 6°, and 90° with respect to the incident electron beam.  相似文献   

17.
The Holifield Radioactive Ion Beam Facility is described. Utilizing the isotope separator on-line technique, this new user facility is coming on-line at the end of 1996. A new experimental endstation centered around the Recoil Mass Spectrometer is also described. Recent data taken on 74Rb and 75Rb is also presented.  相似文献   

18.
Theα decay of mass-separated188Pb and180,182Hg has been studied at the GSI on-line mass separator. Alpha singles spectra as well asα-X-t andα-e-t coincidence events were collected. Fine structure in theα decay of188Pb was measured for the first time, feeding the 21 + and 02 + states in184Hg. Theα decay of180,182Hg feeds low-lying states in176?178Pt. One of these states could be identified as a 0+ state. The deexcitation pattern could be established. As a by-product an alpha-decay scheme of180Au towards levels in176Ir is given.  相似文献   

19.
Reorientation effect and multiple Coulomb excitation measurements have been performed for198, 200, 202, 1204Hg. By measuring particle spectra after Coulomb excitation of an enriched198Hg target with4He and16O beams, a positive quadrupole moment of Q2 = 0.66±0.18 eb (for negative interference) or Q2=0.80±0.18 eb (for positive interference) andB(E2,0→2)=0.991±0.006 e2b2 were obtained. All otherB(E2) values and quadrupole moments were determined relative to these numbers from preciseγ-ray yields obtained from Coulomb excitation of a frozennatHg target with4He and16O projectiles. Oblate shapes of all Hg isotopes were found. The data have been interpreted in terms of triaxial rotation and anharmonic vibrations.  相似文献   

20.
The methods of time-resolved and time-integral on-line nuclear orientation have been applied to study short lived nuclei with the NICOLE facility (Nuclear Implantation into Cold On-Line Equipment) at ISOLDE-3 in CERN using beams of182–186Hg. The half-lives in these decay chains are of the order of seconds and therefore comparable to the spin-lattice relaxation times of the nuclei in iron. As the relaxation rate depends strongly on the g-factor, g-factors of nuclei in the decay chains can be deduced from the observation of the time evolution of γ-ray anisotropy. Using this technique the existence of an isomer in184Au has been found and the g-factors of184Au,184mAu and182Au have been determined. Accurate half-lives have been extracted from the data. Time-integral nuclear orientation has been observed for short lived as well as longer lived isotopes of the Hg decay chains. From these measurements, after proper correction for incomplete relaxation, the magnetic moments of183mPt,183Ir and182Ir have been derived. The applicability of the time-resolved nuclear orientation technique for nuclei far from stability and its possible limitations is discussed.  相似文献   

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