排序方式: 共有22条查询结果,搜索用时 207 毫秒
1.
The Langevin equation is used to simulate the fission process of ^112Sn ^112Sn and ^116Sn ^116Sn. The mass distribution of the fission fragments are given by assuming the process of symmetric fission or asymmetric fission with the Gaussian probability sampling. The isoscaling behaviour has been observed from the analysis of fission fragments of both the reactions, and the isoscaling parameter α seems to be sensitive to the width of fission probability and the beam energy. 相似文献
2.
The Δ-scaling method has been applied to ultra-relativistic p p,C C and Pb Pb collision data simulated using a high-energy Monte Carlo package,LUCIAE 3.0.The Δ-scaling is found to be valid for some physical variables,such as charged particle multiplicity,strange particle multiplicity and number of binary nucleon-nucleon-nucleon collisions from these simulated nucleus-nucleus collisions over an extended energy ranging from E1ab=20 to 200A GeV.In addition we derive the information entropy from the multiplicity distribution as a function of beam energy for these collisions. 相似文献
3.
4.
Investigation of Exotic Structure of the Largely Deformed Nucleus ^23A1 in the Relativistic-Mean-Field Model 下载免费PDF全文
A candidate for proton halo nucleus ^23A1 is investigated based on the constrained calculations in the framework of the de[ormed relativistic mean tield (RMF) model with the NL075 parameter set. It is shown by the constrained calculations that the ground state of ^23A1 has a large deformation that corresponds to the prolate shape. With that large deformation, the non-constrained RMF calculation predicts that there appears an inversion between the 2s1/2 [211] and ld5/2 [202] shells. The valence proton of ^23A] is weakly bound and occupies 2s1/2 [211] and ld5/2 [202] with the weights of 56% and 29%, respectively. The calculated RMS radius for matter is in agreement with the experimental one. It is also predicted that the difference between the proton RMS radius and the neutron one is very large, This suggests that there exists a proton hMo in ^23Al. 相似文献
5.
用非线性相对论平均场对两对镜像核13N-13C 和15N-15O进行了研究. 发现无论在基态还是激发态, 用两套参数所得的结合能都跟实验值很接近. 计算结果显示13N的第一激发态(2s1/2)和第三激发态(1d5/2)各存在一个非束缚的质子晕, 而13C的第三激发态(1d5/2)存在一个弱束缚的中子皮. 另外研究表明, 在另一对镜像核15N-15O的第二激发态(2s1/2)和第一激发态(2s1/2)分别存在一个中子晕和质子皮. Properties of two pairs of mirror nuclei 13N-13C and15N-15O are investigated by using the nonlinear relativistic mean field theory. It is found that all the calculated binding energies with two different parameter sets are very close to the experimental ones for both the ground states and the excited states. The calculations show that the first excited state (2s1/2) and the third excited state (1d5/2) in 13N are both unbound resonances with proton halo structure, whereas the third excited state (1d5/2) in 13C is weakly bound with a neutron skin. It is also predicted that there has a proton halo in the second excited state (2s1/2) of 15N as well as a neutron skin in the first excited state (2s1/2) of 15O. 相似文献
6.
7.
A New Possible Probe for Investigating the Exotic Structure of Neutron-Rich Nuclei by Using the Hanbury-Brown-Twiss Method 下载免费PDF全文
Hanbury-Brown-Twiss (HBT) results of the nucleon-nucleon correlation function have been presented for the nuclear reactions with neutron-rich projectiles using an event-generator, i.e. the isospin-dependent quantum molecular dynamics model. A good agreement of our calculation for the two-halo-neutron correlation function of 相似文献
8.
人胰岛淀粉样蛋白(hIAPP)与Ⅱ型糖尿病(T2DM)密切相关,被认为是导致胰岛β细胞凋亡的致病因素之一,研究发现环境因素(如金属离子、pH值和温度等)对hIAPP的聚集过程有很大影响。本文采用多种生物物理的实验方法,研究了二价铜离子对hIAPP及其片段聚集的影响。原子力显微镜(AFM)和硫代黄素T(ThT)荧光的测量表明,铜离子能够明显地抑制hIAPP(11~28)聚集成纤维,其抑制程度随铜离子浓度的增加而明显加剧。显微傅里叶变换红外光谱(Micro-FTIR)的结果表明,铜离子能够抑制hIAPP多肽中α螺旋结构向β折叠的转变。另外,氨基酸定点突变实验结果表明,hIAPP(11~28)中的组氨酸(His18)可能对多肽的聚集行为和金属铜离子的相互作用起到了决定性的影响。 相似文献
9.
利用淀粉样蛋白纤维为生物模板合成了尺寸均匀且分散性较好的金属钯纳米颗粒.原子力显微镜的测试表明,钯纳米颗粒的平均粒径大小为(12.8±0.5)nm.利用X射线光电子能谱对钯纳米颗粒/胰岛素进行化学组分表征,最后将钯纳米颗粒/胰岛素催化剂应用于Suzuki交叉偶联催化反应以及过氧化氢的检测.实验结果表明,生物模板制备的钯纳米颗粒催化剂具有高效的催化性能,可用于多种铃木交叉偶联反应,并能很好地检测低浓度的过氧化氢溶液. 相似文献
10.