HL—1装置中心热区电子热传导初步分析

在电流及温度分布满足“不变性”原理的基础上,本文分析了等离子体中心热区的能量平衡,求出了电子热传导系数,根据实验数据拟合出HL-1装置电子热传导系数的定标关系为X_e=6.8(n_(eq1))~(-1.2)。此关系与其他托卡马克装置的结果类似。     

全硅MCM-41担载的加氢脱硫催化剂的TPR研究

用TRP技术研究了以全硅MCM-41(Si-MCM-41)和HNO3交换的全硅MCM-41(H-MCM-41)为载体制备的Ni-Mo、Co-Mo和Ni-W加氢脱硫(HDS)催化剂的还原性能，并以0．8(wt)％二苯并噻吩(DBT)的十氢萘溶液为模型化合物，在高压固定床反应器上考察了上述催化剂的加氢脱硫(HDS)反应性能。结果表明，Si-MCM-41经稀HNO3交换后，所担载的Ni-Mo和Ni-W催化剂还原性能、HDS活性和加氢活性有显著变化，但对Co-Mo催化剂影响不大。这说明在Ni-Mo／H-MCM-41和Ni-W／H-MCM-41中可能存在氢溢流现象，DBT的HDS活性与载体表面酸性和氢溢流有关。     

Photoredox‐Catalyzed Isomerization of Highly Substituted Allylic Alcohols by C−H Bond Activation

Photoredox‐catalyzed isomerization of γ‐carbonyl‐substituted allylic alcohols to their corresponding carbonyl compounds was achieved for the first time by C?H bond activation. This catalytic redox‐neutral process resulted in the synthesis of 1,4‐dicarbonyl compounds. Notably, allylic alcohols bearing tetrasubstituted olefins can also be transformed into their corresponding carbonyl compounds. Density functional theory calculations show that the carbonyl group at the γ‐position of allylic alcohols are beneficial to the formation of their corresponding allylic alcohol radicals with high vertical electron affinity, which contributes to the completion of the photoredox catalytic cycle.     

硝基苯加氢合成对氨基酚用负载铂催化剂的制备

 用甲醛还原沉积法制备了活性炭负载的铂催化剂（Pt／AC）和不\r\n同载体负载的铂催化剂，并考察了催化剂对硝基苯加氢制备对氨基酚反\r\n应的催化性能．结果表明，还原Pt（Ⅳ）的甲醛用量是影响催化剂性能\r\n的关键因素，甲醛必须过量而且存在一个最佳值．增加催化剂的铂负载\r\n量，不能有效提高加氢反应速度，反而易降低对氨基酚选择性；低铂负\r\n载量催化剂具有较高的活性、选择性及稳定性．XPS和TEM表征结果表明\r\n，金属铂集中分布于活性炭颗粒外部，其颗粒大小介于2～12nm间．炭\r\n载体催化剂的活性和选择性明显高于金属氧化物载体催化剂．掺入适量\r\n的Mg可显著提高Pt／AC催化剂的活性和选择性．     

Structural and upconversion fluorescence properties of Er/Yb-codoped oxychloride lead-germanium-bismuth glass

Structural and infrared-to-visible upconversion fluorescence properties of Er³⁺/Yb³⁺-codoped oxychloride lead-germanium-bismuth glass have been studied. The Raman spectrum investigation indicates that PbCl₂ plays an important role in the formation of glass network, and has an important influence on the upconversion luminescence owing to lower phonon energy. Intense green and red emissions centered at 525, 546, and 657 nm, corresponding to the transitions ²H_11/2→⁴I_15/2, ⁴S_3/2→⁴I_15/2, and ⁴F_9/2→⁴I_15/2, respectively, were observed at room temperature. The quadratic dependence of the 525, 546, and 657 nm emissions on excitation power indicates that a two-photon absorption process occurs under 975 nm excitation.     

Comparative investigation of up-conversion luminescence in Tm-doped oxide-chloride germanate and tellurite glasses

Tm³⁺-doped oxide-chloride germanate and tellurite glasses have been synthesized by conventional melting method. Intense up-conversion luminescence emissions were simultaneously observed at room temperature in these glasses. The possible up-conversion mechanisms are discussed and estimated. However, in these Tm³⁺-doped glasses, tellurite glass showed weaker up-conversion emissions than germanate glass, which is inconsistent with the prediction from the difference of maximum phonon energy between tellurite and germanate glasses. In this paper, Raman spectroscopy was employed to investigate the origin of the difference in up-conversion luminescence in the two glasses. Our results confirm that, besides the maximum phonon energy, the phonon density of host glasses is also an important factor in determining the up-conversion efficiency.     

HL—1装置密度极限破裂分析

HL-1装置上观测到大量的密度极限破裂放电。其主要特性是破裂前偏离几何中心的磁面位移很小,中心区总是观测到锯齿现象,破裂后,其电流中断时间大于20ms。本文详细分析了出现在电流上升段,坪段及下降段密度极限破裂的特征。其中一类是由于辐射功率超过加热功率所确定的村上极限,没有观测到先兆振荡;另一类是由于约束变坏所确定的赫吉尔极限,可观测到驰豫几毫秒的先兆振荡,这类放电破裂后多数能恢复。该装置运行的最大村上参数是0.35×10~(20)m~(-2).T~(-1)。     

HL—1装置的低q放电实验

装置获得的最低qL值是衡最托卡马克磁流体不稳定性的控制水平的重要品质参数.通过精细调节补充送气和电流上升率的方法控制电流密度分布,使用钛吸气方法控制边缘等离子体参数,HL-1装置获得了最低qL值为1.8的稳定等离子体。实验结果表明,若电流上升率与密度上升率之比为(23—40)×10~(-19)kA·m~3的范围内,最利于获得低MHD增长率的稳定放电。预计这与中心q(0)<1峰化的电流密度分布有关。     

多道HCN激光干涉仪在HL－1装置上的电子密度分布测量

本文描述了为测量ＨＬ－１装置电子密度分布而研制的多道远红外（ＦＩＲ）激光干涉仪系统及其特点。首次对装置在弹丸加料以及拉瓦尔（Ｌａｖａｌ）超声分子束注入实验条件下的等离子体电子密度时－空分布进行了观测和初步分析。同时，介绍一种处理密度相移信号的新方法。     

HL－1电子密度行为在各种条件下的实验研究

在ＨＬ－１装置电子密度测量中，进一步改进了密度相移信号的处理方法。在氘放电、氦补充送气条件下得到了ＨＬ－１最高电子密度１０．８×１０１３ｃｍ－３。总结了密度在各种实验条件下的行为，并对各种实验条件对密度的影响进行了分析。