硝基甲烷振动能量弛豫的集体模型

用分子动力学方法结合Dlott等人提出的"门槛模"理论研究集体相互作用下硝基甲烷振动能量弛豫过程.其中振动冷却过程与实验符合的很好.在振动激发过程的分子动力学模拟中观测到与实验一致的基频频移现象.用分子动力学方法从微观上详细地描述出分子"门槛模"振动激发过程.研究表明,在高温高压作用下,集体作用效应对多原子振动激发具有不可忽视的作用,能量传递过程中除了基频的作用外,强烈的非线性相互作用引起的振动模泛频也携带有大量的振动能,这些泛频也对分子振动能量传递产生重要影响.

基于大功率LED的中子墙光刻度系统

光刻度系统是中子墙探测器系统的重要组成部分,用于中子墙前端电子学的刻度和探测器工作性能变化的监测．通过对基于发光二极管(LED)作为光源的中子墙光刻度系统方案开展了细致的测试研究,确定了基于快脉冲驱动的大功率蓝光LED(3W)的中子墙光刻度系统方案,对中子墙探测单元进行了初步刻度测试,刻度结果能很好地满足光刻度要求,表明对于快塑料闪烁体探测器该方案是一种较为理想的方案．

同位旋非对称核物质性质与扩展的BHF方法(Ⅴ)三体核力对质子和中子单粒子势的影响

在扩展的同位旋相关的Brueckner Hartree Fock理论框架内 ,研究了三体核力对同位旋非对称核物质中质子与中子的单粒子势及其同位旋依赖性的影响 .

Study of the LED based light calibration system for neutron wall detector

The light calibration system is one of the key components of Neutron Wall detector. It is used to calibrate the electronics and to monitor the long-term stability of the detector modules. With the detaile investigations, a calibration system with high-power LED (3W) driven by the fast pulses has been carried out. It is also tested together with the detector module of the Neutron Wall and the result of the preliminary calibration demonstrates that it fulfills the needs. It's a new design proposal to the light calibration system of the fast scintillator detector.

基于RIBLL束线开展超重核合成的可行性研究

超重元素合成研究是当今国际上核物理研究的热点领域之一，也是中国科学院近代物理研究所的一个重要研究方向。根据实际情况，我们确定了两步走的发展方案。针对第一步发展方案，我们对RIBLL放射性束流线进行了改造。具体做法就是在RIBLL入口的前段增加一个速度选择器，并将原束流传输线的前半段改造为充气谱仪。本论文详细论述了RIBLL改造所涉及到的硬件设计和建造以及改造后系统的各项性能测试。硬件部分主要包括反应靶室、转靶系统、速度选择器、充气及气压控制系统、焦平面的衰变探测器等。性能测试方面主要开展了以下工作：(1) 利用放射源对速度选择器的接收立体角和动量接收度进行了测试；(2) 测量了铀离子经不同厚度碳膜后的电荷态分布，并与经验公式计算进行了比较；(3) 利用已知截面的反应道和靶反冲核分别对系统的传输效率、充气谱仪的最佳气压值和重离子在氦气中的平衡电荷态进行了研究。基于以上测试的结果，论文对在改造后的RIBLL上开展超重核合成研究的可行性进行了讨论。结论是由于RIBLL的二极磁铁的分析能力太强，大大降低了系统的传输效率，因此该谱仪只可用于原子序数Z≤107的超重核合成研究和生成截面较高的短寿命滴线核的合成及性质研究，对于更高原子序数的超重核合成研究应该放到正在建造的SHANS谱议上进行

Calorimetric study on two biphenyl liquid crystals

The molar heat capacities of the two biphenyl liquid crystals, 3BmFF and 3BmFFXF3, with a purity of 99.7 mol% have been precisely measured by a fully automated precision adiabatic calorimeter in the temperature range between T = 80 and 350 K. Nematic phase-liquid phase transitions were found between T = 297 K and 300 K with a peak temperature of T-peak = (298.071 +/- 0.089) K for 3BmFF, and between T = 316 and 319 K with a peak temperature of T-peak = (315.543 +/- 0.043) K for 3BmFFXF3. The molar enthalpy (Delta(trs)H(m)) and entropy (Delta(trs)S(m)) corresponding to these phase transitions have been determined by means of the analysis of the heat capacity curves, which are (15.261 +/- 0.023) U mol(-1) and (51.202 +/- 0.076) J K-1 mol(-1) for 3BmFF, (31.624 +/- 0.066) kJ mol(-1) and (100.249 +/- 0.212) J K-1 mol(-1) for 3BmFFXF3, respectively. The real melting points (TI) and the ideal melting points (TO) with no impurities of the two compounds have been obtained from the fractional melting method to be (298.056 +/- 0.018) K and (298.165 +/- 0.038) K for 3BmFF, (315.585 +/- 0.043) K and (315.661 +/- 0.044) K for 3BmFFXF3, respectively. In addition, the transitions of these two biphenyl liquid crystals from nematic phase to liquid phase have further been investigated by differential scanning calorimeter (DSC) technique; the repeatability and reliability for these phase transitions were verified. (C) 2004 Elsevier B.V. All rights reserved.