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1.
The pure nuclear spin alignments of 8Li and 8B were produced from the nuclear spin polarization applying the β-NMR method. The alignment correlation terms in the β-ray angular distribution were observed to test the G parity conservation in the nuclear β decay.  相似文献   

2.
The momentum dependences of the nuclear spin polarization P and alignment A of 13B(, T 1/2 = 17.36 ms) produced in the 100A MeV 15N + Be collisions have been measured by detecting β-ray asymmetry. Because both the P and A were significantly smaller than the prediction from a simple kinematical model, some relaxation mechanisms must be take into account. Comparing the signs of the observed alignment of 12B, the sign of the quadrupole coupling constant eqQ of 13B in TiO2 was determined to be positive.  相似文献   

3.
Asahi  K.  Ogawa  H.  Ueno  H.  Kobayashi  Y.  Sato  W.  Yoshimi  A.  Watanabe  H.  Kameda  D.  Miyoshi  H.  Sakai  K.  Imai  N.  Yoneda  K.  Watanabe  Y. X.  Fukuda  N.  Aoi  N.  Yoshida  A.  Kubo  T.  Ishihara  M. 《Hyperfine Interactions》2001,136(3-8):183-187
Magnetic dipole and electric quadrupole moments of nuclei in the light-mass neutron-rich region have been studied by taking advantage of spin-polarized radioactive nuclear beams that have been obtained from the projectile fragmentation reaction. Analyses of the results reveal a few interesting phenomena characteristic of nuclear structures in this region. In particular, we report in some detail the latest result on the magnetic moment of the 17C ground state. The distinctly small value of the g-factor obtained, |g(17C)|=0.5054±0.0025, clearly excludes a I π=1/2+ candidate for the spin-parity assignment of this marginally bound nucleus, providing a reasonable account of the non-halo nature reported in recent breakup reaction experiments. Finally, future plans at the upcoming radioactive beam facility presently under construction at RIKEN are briefly mentioned. This revised version was published online in September 2006 with corrections to the Cover Date.  相似文献   

4.
原子核阻止是核子–核子碰撞截面的可能探针   总被引:1,自引:1,他引:1  
利用同位旋相关的输运理论,研究了不同中子–质子比的碰撞系统在中能重离子碰撞过程中,原子核阻止的同位旋效应及其对束流能量和碰撞参数的依赖性.计算表明对于所研究的4个碰撞系统,在从费米能附近到大约150MeV/u的较宽入射能量范围内,近心碰撞的原子核阻止强烈地依赖于核子–核子碰撞截面的同位旋相关性,而对称势对它的影响并不明显.故原子核阻止是提取介质中核子–核子碰撞截面的灵敏探针.研究还表明动量相关势对原子核阻止的重要作用是不可忽略的.  相似文献   

5.
用修正的统计擦去模型计算了中能重离子碎裂反应产生的同位素分布的同位旋效应,发现随着(Zproj–Z)/Zproj的增大,碎裂反应的同位旋效应将逐渐减小直到消失.同时,研究表明碎裂反应的同位旋效应的消失主要是由擦去阶段的几何效应和随后的蒸发效应导致的.  相似文献   

6.
重离子碰撞中原子核阻止的同位旋效应   总被引:1,自引:0,他引:1  
利用含有3种对称势形式的同位旋相关的量子分子动力学,研究了中能重离子碰撞中原子核阻止的同位旋效应和随入射道条件的系统演化过程.计算结果表明,原子核阻止灵敏地依赖束流能量、碰撞参数、碰撞系统的质量和核子–核子碰撞截面的同位旋相关性,而3种对称势和碰撞系统的中质比对它的影响不很明显,但在大约费米能量以下能区,原子核阻止同时依赖于介质中核子–核子碰撞截面和对称势.故认为在费米能量以上能区直至150MeV/u,原子核阻止是提取介质中核子–核子碰撞截面的一个新的物理观测量.  相似文献   

7.
Matsuta  K.  Hashimoto  K.  Kudo  S.  Arimura  K.  Mihara  M.  Fukuda  M.  Minamisono  T. 《Hyperfine Interactions》2001,136(3-8):503-507
The line widths of the β-NMR spectra of the short-lived β emitters 8Li and 12N implanted in a single crystal of Al have been measured precisely for the first time as a function of crystal orientation. The NMR line widths were compared with the theoretical van Vleck values of the dipolar broadening. As a result, it was found that 8Li mainly sits in substitutional sites, while 12N sits in tetrahedral interstitial sites, in Al. This revised version was published online in September 2006 with corrections to the Cover Date.  相似文献   

8.
讨论了重离子辐照生物中核碎裂效应,给出与此相关的核碎裂研究现状和进展。The effect of nuclear fragmentation discussed. The status and perspectives of this data. in the topic interactions of heavy ions with biological are presented based On calculations and molecules is experimental.  相似文献   

9.
Matsuta  K.  Sasaki  M.  Tsubota  T.  Kaminaka  S.  Hashimoto  K.  Kudo  S.  Ogura  M.  Arimura  K.  Mihara  M.  Fukuda  M.  Akai  H.  Minamisono  T. 《Hyperfine Interactions》2001,136(3-8):379-384
The hyperfine interactions of 8Li implanted in single crystal Fe have been studied using the β-NMR technique. One kind of hyperfine field B hf was found. Since no dipolar field was observed, 8Li nuclei are suggested to sit in substitutional sites. The B hf and the spin-lattice relaxation time T 1 were observed as functions of temperature. The experimental B hf and T 1 were compared with the theoretical predictions from the first principles KKR-band-structure calculations. While predicted B hf for the substitutional site is consistent with the experiment, predicted T 1 cannot reproduce the experiment well. This revised version was published online in September 2006 with corrections to the Cover Date.  相似文献   

10.
相对论重离子碰撞的拓扑荷作用破坏作用平面两侧不同手征性的夸克数目的平衡,从而引起P和CP破坏特征。本工作主要分析RHIC和LHC能区的手征电荷分离作用,分析手征电荷分离随碰撞中心度、碰撞能量和核屏蔽等依赖关系。并未发现手征电荷分离效应与碰撞能量大小有非常紧密的依赖关系,但发现核屏蔽效应对手征电荷分离有重要的影响,与不考虑屏蔽效应相比,考虑屏蔽效应会使手征分离效应明显压低,由于屏蔽效应出现,使得a++a--)的分布与a+-a-+)分布并不对称。并且还发现手征分离效应主要发生在碰撞参量较大的周边碰撞,越接近中心碰撞,手征分离效应几乎可以忽略。The topological charge interactions in relativistic heavy ion collisions cause quark chirality imbalance, resulting in charge separation under the strong magnetic field and local P and CP violation. In this paper, the chiral charge separation at RHIC and LHC energies is systematically analyzed as functions of the collision centrality, the collision energy and the nuclear shielding factor. It is found that there is not a very close dependence of the chiral charge separation effect on the collision energies, but that has an important dependence on nuclear shielding factor. Compared with the non-shielding effect, the shielding effect can reduce the chiral separation effect obviously. Due to the shielding effect, the distribution of a++(a--) and the distribution of a+-(a-+) are asymmetric. One also finds that chiral separation effect, which is almost negligible when more close to the central collision, occurs mainly in the peripheral collision for larger impact parameter.  相似文献   

11.
Mihara  M.  Hashimoto  K.  Arimura  K.  Kudo  S.  Akutsu  K.  Minamisono  K.  Miyake  T.  Fukuda  M.  Matsuta  K.  Minamisono  T. 《Hyperfine Interactions》2001,136(3-8):339-343
The hyperfine interactions of short-lived β-emitter 12B implanted into a CaB6 crystal have been studied by means of the β-NMR technique. An electric quadrupole splitting has been observed at room temperature from which an electric field gradient of q=−(1.34±0.05)×1021 V/m2 was determined. From the present result, it was found that the 12B nuclei are mainly implanted in the substitutional boron site. This revised version was published online in September 2006 with corrections to the Cover Date.  相似文献   

12.
Izumikawa  T.  Matsuta  K.  Tanigaki  M.  Miyake  T.  Sato  K.  Fukuda  M.  Zhu  S. Y.  Minamisono  T. 《Hyperfine Interactions》2001,136(3-8):599-605
Using β-NMR with 12B nuclei the temperature dependence of the lattice locations of boron implanted in Si is studied. At low temperature almost 100% of the implanted B is in either substitutional site or nonsubstitutional site. Above 260 K, the nonsubstitutional B rapidly becomes undetectable and disappears at a temperature higher than 325 K due to the fast spin-lattice relaxation. Above 450 K, the fraction of substitutional B increases to 100%. These experimental results are consistently explained by the thermal atomic jump and the dissociation of the defect associated with the nonsubstitutional B. This revised version was published online in September 2006 with corrections to the Cover Date.  相似文献   

13.
Gruskova  A.  Lipka  J.  Papanova  M.  Kevicka  D.  Gonzalez  A.  Mendoza  G.  Toth  I.  Slama  J. 《Hyperfine Interactions》2004,159(1-4):187-191
The β-NMR of short-lived β-emitter in a rutile TiO2 single crystal has been measured as functions of temperature and external magnetic field. Atomic motion induced spin lattice relaxation was observed for two known sites, O substitutional and interstitial sites. The data were analyzed in terms of the thermal atomic jump, which suggests that the motion of defects around the substitutional 12N atom for O, and of the interstitial 12N atom are attributed to the spin lattice relaxation. The electric field gradients have shown temperature dependence for both sites, which is probably due to the thermal expansion of rutile.  相似文献   

14.
高能重离子碰撞中末态粒子的极角分布   总被引:1,自引:0,他引:1  
在反应平面内不同极角方向为z轴的质心坐标系中,分析了末态粒子方向角分布的非对称性,建立了一种确定集合侧向流流角的方法.在以流方向为z轴的质心坐标系中研究了Bevalac流光室1.2AGeV Ar+KCl、1.2AGeV Ne+NaF和2.1AGeV Ne+NaF三种反应中末态粒子的极角分布,对末态粒子非对称发射部分所占的比例及其在流方向的集中程度做出了定量的估计.  相似文献   

15.
基于实验测量并结合模型分析,讨论了中能区重离子周边碰撞过程中出射的类弹碎片(PLF)的中质比(N/Z)与靶核N/Z相关现象的产生原因.  相似文献   

16.
利用同位旋相关的量子分子动力学模型,对中能重离子碰撞过程中多重碎裂对于同位旋自由度和动量相关作用的依赖性进行了研究.结果表明:在相对较高能区,碎片的平均多重性敏感地依赖于介质中核子–核子碰撞截面的同位旋效应,但很弱地依赖于对称势;动量相关作用增强了中等质量碎片多重性对于核子–核子碰撞截面的同位旋依赖的敏感性.中等质量碎片的平均多重性可用作提取介质中同位旋相关的核子–核子碰撞截面的探针.  相似文献   

17.
摘要: 对清华大学在束γ谱实验组近年来在A=135缺中子核区N=79的同中异位素 135Ba, 137Ce和 139Nd的高自旋态实验研究进行了介绍。 实验是在中国原子能科学研究院HI 13串列加速器上用在束γ的实验技术、 分别通过重离子核反应 130Te(9Be, 4n), 124Sn(18O, 5n), 128Te(16O, 5n)进行的。 实验结果扩展了这3个核的高自旋态能级纲图。 研究表明, 这3个核的低自旋态结构均起源于 νh-111/2空穴与其偶偶核芯的耦合。 用粒子 转子模型对其结构进行了计算, 得到这3个核的形变参量γ值均稍大于30°, 为偏向于扁椭的三轴形变, 从而可看出Ba, Ce和Nd 3个同位素链在低自旋态下由长椭边到扁椭边的形状转变都发生在中子数N=77—79之间。 对于中等自旋态下一些能级的组态进行了指定与系统学比较。 在高自旋态下, 在 137Ce中发现一条γ≈-60°的扁椭形变带, 在 139Nd中则发现3条这样的扁椭形变带, 对这些扁椭形变带的起源及结构特性进行了讨论。 The progress of research on the high spin states at N=79 isotopes 135Ba, 137Ce and 139Nd in A=135 neutron deficient region by the research group of Tsinghua University has been reviewed. The experiments were carried out by using in beam γ ray spectroscopy technology and heavy ion nuclear reactions 130Te(9Be, 4n), 124Sn(18O, 5n) and 128Te(16O, 5n) at China Institute of Atomic Energy (CIAE). The high spin level schemes of these nuclei have been expanded. The results indicate that the lower spin states of these nuclei originated from νh-111/2 hole state coupling with the neighboring even even nucleus cores. All the deformation parameters γ values of these three isotones are larger than 30°, which indicates that they have triaxial deformation with oblate side. The prolate oblate transition in Ba, Ce and Nd isotopic chains indeed happens between N=77 and N=79. Through systematical comparison with the neighboring isotones, the configurations for some middle spin state levels have been assigned. At the high spin states, one oblate band in 137Ce and three ones in 139Nd with γ≈ -60° were discovered. The origination and structural character of these oblate bands have been discussed.  相似文献   

18.
Mekata  M.  Kikuchi  H.  Watanabe  I.  Nagamine  K.  Itoh  S.  Mamiya  H.  Kojima  K. M. 《Hyperfine Interactions》2001,136(3-8):263-268
The magnetic ordering process of Ising spins on diluted square lattice was studied by muon spin relaxation using model compounds Rb2Co c Mg1−c F4. Muon relaxation shows an anomaly at a remarkably higher temperature T N μSR than the transition temperature determined by neutron Bragg scattering T N ND near the percolation threshold for square lattice (c p=0.593). The difference between the two temperatures amounts to 50% of T N ND just above c p. The field cooling effect of DC magnetic susceptibility is appreciable below T N ND while the temperature of the anomaly in AC susceptibility approaches to T N μSR as the frequency is increased. It was concluded that there is a crossover from two-dimensional ordering at T N μSR to three-dimensional ordering at T N ND but the two-dimensional order between T N μSR and T N ND has slow fluctuations due to the fractal structure with a plenty of weak links. This revised version was published online in September 2006 with corrections to the Cover Date.  相似文献   

19.
By studying the quadrupolar interaction of 12B in silicon–germanium mixed crystals with the β-NMR method, the boron–germanium pair was identified and the saturation amplitudes for boron in differently composed crystals were measured. The relative saturation amplitudes agree with statistical predictions. At low temperatures boron is preferentially implanted into stable interstitial sites. These sites are converted into substitutional sites by diffusion processes which take advantage of reorientation jumps.  相似文献   

20.
Matsuta  K.  Miyake  T.  Minamisono  K.  Mihara  M.  Fukuda  M.  Sato  K.  Zhu  S. Y.  Minamisono  T. 《Hyperfine Interactions》2001,136(3-8):189-194
Hyperfine interactions of 12,14N in BN(hexagonal) crystal were studied by detecting β-NQR(12N) and FT-NMR(14N). A β-NMR of 16N (I π=2,T 1/2=7.13 s) in MgO crystal was detected to determine the magnetic moment of 16N to be |μ(16N:2)|=(1.986±0.001)μN. Also, the β-NQR of 12,16N in TiO2 crystal were detected to determine |Q(16N:2)|=(17.9±1.7) mb. An abnormally small effective charge for neutrons is required to account for |Q(16N:2)|. This revised version was published online in September 2006 with corrections to the Cover Date.  相似文献   

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