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20条相似文献,搜索用时 15 毫秒
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A. N. Andreyev N. Bijnens T. Enqvist M. Huyse P. Kuusiniemi M. Leino W. H. Trzaska J. Uusitalo P. Van Duppen 《Zeitschrift für Physik A Hadrons and Nuclei》1997,358(1):63-68
The neutron-deficient 190Po and 189Bi isotopes have been produced in the 2n respectively p2n channels of the 48Ti +144 Sm reaction. Cross sections for different reaction channels are given. For 190Po, improved values of α-energy Eα = 7550(15) keV and half-life T1/2 = 1.9 ?0.4 +0.6 ms were measured. By using correlated α-decay chains an α-branching ratio of 0.50(25) was deduced for 186Pb. The reduced α-width systematic is extended for both of these isotopes, confirming a persistence of the saturation towards the lighter Po isotopes and the absence of any anomalies for the neutron-deficient Pb isotopes. For 189Bi improved values of Eα = 7300(15) keV and T1/2 = 4.8(5) ms were measured. 相似文献
3.
A.P. Byrne A.M. Baxter G.D. Dracoulis S.M. Mullins T. Kibédi T.R. McGoram K. Helariutta J.F.C. Cocks P. Jones R. Julin S. Juutinen H. Kankaanpää H. Kettunen P. Kuusiniemi M. Leino M. Muikku P. Nieminen P. Rahkila A. Savelius 《The European Physical Journal A - Hadrons and Nuclei》2000,7(1):41-44
Lifetime measurements of states in nuclei with A=187 and 188 have been performed, using reactions between 155Gd and 36Ar and following the transport of evaporation residues to the focal plane of a gas-filled recoil separator. In a separate
experiment using the 159Tb(32S, 4n) reaction the γ-decay of isomeric levels in 187Tl has been studied using delayed γ-γ coincidence measurements. From observation of their subsequent γ decay, the mean lifetimes
were measured to be 1000 ± 55 ns and 1600 ± 100 ns. Although it was not possible to characterize the isomers completely, they
are proposed as candidates for one-proton, two-neutron excitations. In the course of this study, the decay of an isomer in
188Pb was also observed and its lifetime was measured as 1150 ± 30 ns, and limits of 20–600 ns were placed on the meanlife of
an isomer conjectured in 187Pb.
Received: 20 August 1999 相似文献
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报道了利用兰州重离子研究装置提供的26Mg重离子束流轰击243Am靶产生和鉴别已知超重核素266Bh的实验结果。利用转轮收集探测装置依靠母子核遗传关系通过观测Bh同位素与其子核Db和Lr之间的α-α关联事件来鉴别266Bh。实验中观测到266Bh的α能量为(9.03 ± 0.08)MeV, 与日本理化学研究所在合成113号元素中第一个衰变链中观测到266Bh的α能量为9.07 MeV相近。 266Bh的半衰期为0.66+0.59-0.26 s, 从实验得到的Qα也符合Z=107的Qα随中子数变化的系统性。The isotope of 266Bh was produced and identified definitely in bombardments of 243Am target with 162 MeV 26Mg ions at HIRFL. Identification was made by observation of correlated α particle decays between the Bh isotopes and their Db and Lr daughters using a rotating wheel system. The measured α energy for 266Bh is (9.03±0.08) MeV, and this value close to the 9.07 MeV for 266Bh observed in the first chain of element 113 at RIKEN. The half life of 266Bh is 0.66+0.59 -0.26 s. The Qα value derived from this experiment fits well into the general trend in a “Qα N systematics” for the isotopes with Z = 107. 相似文献
6.
K. Hardt Y. K. Agarwal C. Günther M. Guttormsen R. Kroth J. Recht F. A. Beck T. Byrski J. C. Merdinger A. Nourredine D. C. Radford J. P. Vivien C. Bourgeois 《Zeitschrift für Physik A Hadrons and Nuclei》1983,312(3):251-256
High-Spin states in188Hg have been investigated using the168Er(24Mg,4n) reaction. The rotation aligned vi 13 2/2 band, which intersects the weakly oblate ground state band atI≈10, is observed up toI π =20+ with an isomeric 12+ level with T1/2=134(15)ns. The coexisting strongly deformed band, built on the 825 keV 0+ level, is observed up to the 14+ state. The systematics of the vi 13 2/2 rotation aligned bands is discussed. 相似文献
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H. De Witte A. N. Andreyev S. Dean S. Franchoo M. Huyse O. Ivanov U. Köster W. Kurcewicz J. Kurpeta A. Plochocki K. Van de Vel J. Van de Walle P. Van Duppen 《The European Physical Journal A - Hadrons and Nuclei》2005,23(2):243-247
A new measurement of the 200Fr -decay half-life, with improved accuracy compared to previous measurements, has been carried out at the Isolde-CERN on-line mass separator. A half-life of 49(4) ms has been obtained, which is substantially different from earlier literature values. For the 196At daughter decay, a half-life of 389(54) ms and an branching ratio b = 94(5)% were measured. In addition, the half-lives of 201, 203, 205Fr and 197,199At are reported. 相似文献
9.
P. Hornshj 《Nuclear Physics A》1974,230(3):380-392
The use of mass-separated samples of neutron-deficient francium isotopes, produced at the ISOLDE on-line mass-separator facility at the CERN 600 MeV synchro-cyclotron, has permitted precise determinations through genetic relationships of /(EC+β+) branching ratios for a range of light francium and astatine isotopes. The experiments verify previous mass assignments and provide improved values for the half-lives. The systematics of -widths and of β-strength functions is surveyed. 相似文献
10.
H. Sergolle P. Aguer G. Bastin R. Kroth J. P. Thibaud K. Hardt T. Lönnroth F. Beck J. C. Merdinger 《Zeitschrift für Physik A Hadrons and Nuclei》1983,313(4):289-292
Using the reaction175Lu(19F, 6n) theg-factor of the188Hg isomeric state (J π=12+,T 1/2=135 ns) has been measured with the TDPAD method. The experimental value g=?0.168(10) supports the interpretation of an almost pure (vi13/2)?2 configuration for this isomer. 相似文献
11.
H. Kettunen T. Enqvist T. Grahn P.T. Greenlees P. Jones R. Julin S. Juutinen A. Keenan P. Kuusiniemi M. Leino A.-P. Leppänen P. Nieminen J. Pakarinen P. Rahkila J. Uusitalo 《The European Physical Journal A - Hadrons and Nuclei》2003,17(4):537-558
Detailed alpha-decay studies have been performed for the neutron-deficient isotopes 191At and 193At. The nuclei were produced in fusion-evaporation reactions of 54Fe and 56Fe ions with a 141Pr target. The fusion products were separated in-flight using a gas-filled recoil separator and implanted into a position-sensitive silicon detector. The isotopes were identified using position, time and energy correlations between the implants and subsequent alpha-decays. Three alpha-decaying states were identified for 193At and two for 191At. The spin and parity of the initial states in the astatine isotopes were deduced based on unhindered alpha-decays to states in the bismuth daughter nuclei. In both astatine isotopes the 1/2+ intruder state was determined to be the ground state and a 7/2- state to be the first-excited state. In 193At the alpha-decay of the 13/2+ state was observed in coincidence with a previously known gamma-ray transition from the 13/2+ state in the corresponding daughter nucleus 189Bi. In 187Bi and 189Bi low-lying 7/2- states were observed for the first time via alpha-decay of the mother nuclei.Received: 16 December 2002, Revised: 26 March 2003, Published online: 4 August 2003PACS:
23.60.+e Alpha decay - 27.80.+w
- 23.20.Lv
transitions and level energies - 21.10.Dr Binding energies and masses 相似文献
12.
巯基棉富集-氢化物原子荧光法测定地下水中超痕量铅、汞 总被引:8,自引:0,他引:8
本文对巯基棉同时富集铅,汞的条件及洗脱条件,氢化物-原子荧光法测定铅、汞的条件及干扰元素进行探讨,并拟定了测定地下水中超痕量铅、汞的灵敏、可靠的分析方法,实验结果表明,此方法的各项指标均满足地下水分析要求。 相似文献
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用ICP-AES同时测定工业硫酸样品中的铁、砷、铅、汞.方法加标回收率为97%-110%,11次测定的RSD(n=11)小于2.4%.方法操作方便,分析速度快,结果准确. 相似文献
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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19.
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电感耦合等离子体原子发射光谱法测定化妆品中砷、铅、汞 总被引:14,自引:1,他引:14
本文采用五氧化二钒作催化剂,HNO3-H2SO4消解法对化妆品前处理后,用电感耦合等离子体发射光谱仪同时测定砷,铅,汞,方法简便,快速,回收率在95%-103.5%之间,相对标准偏差不大于3%。 相似文献
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