近代物理研究所超重核研究现状及计划

简单描述了超重核合成的历史与国际现状， 详细地介绍了近代物理研究所已经开展的研究工作及取得的成果， 并对近代物理研究所未来在超重核研究方面的研究计划进行了介绍。 The history and the international status of the super heavy nuclei synthesis are briefly described. The related research work carried out at the Institute of Modern Physics (IMP) has been reviewed. The prospect of the super heavy nuclei research at IMP has been introduced.     

超重核研究谱仪的RFQ冷却聚束器RFQ1L

介绍了超重核研究谱仪中RFQ冷却聚束器RFQ1L的结构和运用SIMION程序对离子的冷却、聚束、引出和撇气过程的模拟情况。 模拟显示: 通过仔细选择工作点就完全可以把经过充气反冲质量分离器分离后的低品质束流转化为斑点小、发射度小和能量单一的高品质束流, 为紧接其后的磁铁和激光高效率分析提供条件。The structure and the simulation results about the cooling,bunching,extraction and skimming of the RFQ cooler and buncher RFQ1L, which is an important part of the being built super heavy nuclide research spectrometer, have been introduced. It shows that, by careful choice of its working point, we can obtain an ion beam with small beam spot, small emittance and mono energy, which can satisfy the requirements of the successive analyses by dipole and laser with high efficiencies.     

LPT的RF分相偏置电路的研制

为了对兰州彭宁离子阱LPT内的离子运动进行偶极和四极共振激发,采用变压器原理,设计制作了两套分相器:一套工作频率为200 k Hz～4 MHz,适用于四极激发模式;另一套工作频率为1700～1750 Hz,适用于偶极激发模式。详细测试了它们在空载和负载情况下的幅频曲线与相频曲线。测试结果表明:RF分相偏置电路的输出幅度与相位均达到了设计要求。     

合成和研究滴线区新核素β延发质子先驱核121Ce

利用³²S束轰击⁹²Mo靶,熔合蒸发3n反应合成了¹²¹Ce.藉助于具有γ(X)-p-t符合测量的氦喷嘴反冲快速带传输系统进行分离和鉴别.实验定出¹²¹)Ce的半衰期为(1.1±0.1)s,观测到了¹²¹Ce的延发质子谱并近似估计了延发质子分支比为(1.0±0.5)%.     

兰州彭宁阱核心电极的最优电压幅值计算

彭宁阱是用于直接测量原子核质量的精确设备。为了保证彭宁阱的测量精度,需在阱中心产生精准的四极静电场,而四极静电场是通过对彭宁阱的核心电极施加合适的电压产生的。采用公式推导法和最小二乘法两种方法计算得到了LPT核心电极需加电压幅值。对于公式推导法,电压值完全从理论出发,经公式推导后计算得到;最小二乘法的出发点是使取样偏差的平方和最小,且通过仿真模拟考虑了电极的实际几何形状。由这两种方法得到的非四极项系数C4 和C6,可用于估算因偏离理想四极电场所产生的实验误差。虽然这两种方法的出发点不同,但都可以在阱中心产生需要的四极电场。Penning trap mass spectrometry is one of the direct methods and maybe the most accurate tool for atomic mass measurements. The quadrupole electric eld produced in the trap should be very accurate in order to ensure the precision of measurements. The optimal amplitudes for the key electrodes of the Lanzhou Penning Trap(LPT) have been calculated by two methods|formula derivation and least-squares tting. For formula derivation method, the optimal values are based on the theory and deduced from the formulas. Least-squares tting method is to minimize the quadratic sum of sampling deviations, where the actual geometry of the electrodes has been considered by the simulation. The obtained C4 and C6 values can be used to estimate the experimental error produced by the deviation from the ideal quadrupole electric eld. The expected quadrupole electric led could be gotten by both methods.     

奇奇核174Re的转动带

利用重离子熔合蒸发反应¹⁵⁹Tb(²⁰Ne,5n)¹⁷⁴Re,并通过激发函数、KX－γ和γ–γ符合测量,研究了¹⁷⁴Re核的高自旋态.鉴别并指定了¹⁷⁴Re核的一个基于л1/2^－[541]⊙v1/2^－[521]准粒子组态上的双退耦带.还发现了两个分别具有半退耦特征和强耦合特征的转动带,定性地讨论了它们的粒子组态.     

206At的[πh1/2νi-113/2]10-同质异能态研究

利用能量为60-80MeV的12C束流,通过197Au(12C,3n) 206 At反应研究了206At核的高自旋能级结构. 用7台BGO(AC)HPGe探测器和一台用于探测低能γ射线的平面型HPGe探测器进行了γ射线的激发函数、γ-γ-t符合及γ射线的角分布测量. 基于这些测量,首次建立了包括25条γ跃迁的206At高自旋能级纲图. 确定了一个半寿命为(908±400)ns、自旋和宇称为10-的同质异能态. 基于较重的双奇核 208,210At能级结构的系统性,对206At的10-同质异能态进行了讨论.     

Reeb定理在2维情形的推广与完善

本文利用极函数存在定理性得到下面两个定理:定理1、紧致连通可定向的2维C~∞一微分流形M与一带上g(≥0)个柄的球面Tg同胚的充要条件为存在一临界点最少的Morse函数f:M→R,其临界点个数为2+2g。定理2、一紧致连通2维C~∞一微分流形M的Euler示性数为X(M)的充要条件为存在一临界     

~(206)At的[лh_(1/2)vi_(13/2)~(-1)]10~-同质异能态研究(英文)

利用能量为６０－８０ＭｅＶ的~(１２)Ｃ束流,通过~１９７Ａｎ（~(１２)Ｃ,３ｎ）~２０６Ａｔ反应研究了~２０６Ａｔ核的高自旋能级结构．用７台ＢＧＯ（ＡＣ）ＨＰＧｅ探测器和一台用于探测低能γ射线的平面型ＨＰＧｅ探测器进行了γ射线的激发函数、γ－γ－ｔ符合及γ射线的角分布测量．基于这些测量,首次建立了包括２５条γ跃迁的~２０６Ａｔ高自旋能级纲图．确定了一个半寿命为（９０８±４００）ｎｓ、自旋和宇称为１０的同质异能态．基于较重的双奇核~(２０８,２１０ )Ａｔ能级结构的系统性,对~(２０６)Ａｔ的１０~－同质异能态进行了讨论．     

A simulation study of a dual-plate in-room PET system for dose verification in carbon ion therapy

During carbon ion therapy,lots of positron emitters such as11C,15O,10C are generated in irradiated tissues by nuclear reactions,and can be used to track the carbon beam in the tissue by a positron emission tomography(PET)scanner.In this study,an dual-plate in-room PET scanner has been designed and evaluated based on the GATE simulation platform to monitor patient dose in carbon ion therapy.The dual-plate PET is designed to avoid interference with the carbon beamline and with patient positioning.Its performance was compared with that of four-head and full-ring PET scanners.The dual-plate,four-head and full-ring PET scanners consisted of 30,60,60detector modules,respectively,with a 36 cm distance between directly opposite detector modules for dose deposition measurements.Each detector module consisted of a 24×24 array of 2 mm×2 mm×18 mm LYSO pixels coupled to a Hamamatsu H8500 PMT.To estimate the production yield of positron emitters,a 10 cm×15 cm×15 cm cuboid PMMA phantom was irradiated with 172,200,250 MeV/u12C beams.3D images of the activity distribution measured by the three types of scanner are produced by an iterative reconstruction algorithm.By comparing the longitudinal profile of positron emitters along the carbon beam path,it is indicated that use of the dual-plate PET scanner is feasible for monitoring the dose distribution in carbon ion therapy.