Towards the meV limit of the effective neutrino mass in neutrinoless double-beta decays

We emphasize that it is extremely important for future neutrinoless double-beta(0νββ)decay experiments to reach the sensitivity to the effective neutrino mass|mββ|≈1 meV.With such a sensitivity,it is highly possible to discover the signals of 0νββ decays.If no signal is observed at this sensitivity level,then either neutrinos are Dirac particles or stringent constraints can be placed on their Majorana masses.In this paper,assuming the sensitivity of|mββ|≈1 meV for future 0νββ decay experiments and the precisions on neutrion oscillation parameters after the JUNO experiment,we fully explore the constrained regions of the lightest neutrino mass m1 and two Majorana-type CP-violating phases{ρ,σ}.Several important conclusions in the case of normal neutrino mass ordering can be made.First,the lightest neutrino mass is severely constrained to a narrow range m1∈[0.7,8]meV,which together with the precision measurements of neutrino mass-squared differences from oscillation experiments completely determines the neutrino mass spectrum m2∈[8.6,11.7]meV ing phases is limited to ρ∈[130°,230°],which cannot be obtained from any other realistic experiments.Third,the sum of three neutrino masses is found to beΣ≡m1+m2+m3∈[59.2,72.6]meV,while the effective neutrino mass for beta decays turns out to be mβ≡(|Ue1|2m1^2+|Ue2|2m2^2+|Ue3|2m3^2)1/2∈[8.9,12.6]meV.These observations clearly set up the roadmap for future non-oscillation neutrino experiments aiming to solve the fundamental problems in neutrino physics.     

非相对论弱相互作用玻色气体的有效场理论处理

采用有效场理论研究了非相对论弱相互作用玻色-爱因斯坦凝聚量子气体的一般性质.在分析了系统的不可重整化性质后,从有效拉氏量出发,计算了最低阶环路修正下拉氏量参量的运动耦合常数(running coupling constant)的形式,并且得到了相应的微分方程.研究结果表明,不同于相对论玻色气体的有效理论,对非相对论弱相互作用的玻色气体,可以移除该有效理论中的内禀能量尺度,即可令该有效理论的内禀能量尺度取无穷大值.所得的分析结果将有助于对玻色-爱因斯坦凝聚的临界性质和行为的深入研究.     

用环境友好催化剂H-β沸石制备紫罗兰酮

用环境友好催化剂Ｈ－β沸石催化假性紫罗兰酮环化制备紫罗兰酮。考察了催化剂的用量、反应温度和时间对反应的影响,并测定了假性紫罗兰酮环化反应的速率常数和活化能（３６．４ｋＪ／ｍｏｌ）．Ｈ－β沸石能被回收、再生和重复使用,且与用新鲜Ｈ－β沸石时几乎有相同的紫罗兰酮产率。     

用HZSM-5沸石催化剂合成丙酸酯的研究

迄今为止,工业上生产羧酸酯主要采用以浓硫酸作催化剂的均相酯化反应法,然而此法存在腐蚀设备、后处理工序复杂等缺点.ZSM-5沸石具有独特的晶体结构和优良的物化性能,是许多有机催化反应的理想催化剂.文献[1]报道了用HZSM-5沸石作催化剂合成乙酸乙酯,我们在常压液-固相酯化反应中用自制的ZSM-5沸石催化合成了一系列丙酸酯,该催化剂具有良好的催化活性、选择性和稳定性.     

常压下邻氯甲苯在ZSM-5沸石催化剂上的异构化

邻氯甲苯是“杀草丹”生产过程的副产物,量大价值低。若将它异构化,所得对氯甲苯可直接再作为“杀草丹”的主要原料;所得间氯甲苯水解为间甲酚后又是“速灭威”等农药的主要原料。因此邻氯甲苯异构化是个有意义的综合利用课题。1980年以来国外对邻氯     

以NaHSO4催化假性紫罗兰酮合成紫罗兰酮

以甲苯为溶剂，用NaHSO4催化假性紫罗兰酮合成紫罗兰酮，收率60％。考察了反应温度、反应时间、催化剂用量及其它相关因素对收率的影响，确立了优化的反应条件。     

广义行列式与Cramer法则

设A是一个n阶方阵,B是一个n×m矩阵,则容易证明:当A可逆时,矩阵方程AX=B有唯一解:X=A~(-1)B。如果m=1,则由此便得到熟知的Cramer法则。因此,以上结论自然可视为Cramer法则的一种推广。文[4]利用k阶子式阵曾给出Cramer法则的另一种推广。本文则定义一种广义行列式,并由此给出Cramer法则的又一种非常自然的     

大阳岔寒武-奥陶系界线层型剖面的无铰纲及沉积岩微量元素地球化学

本文通过对我国吉林浑江大阳岔寒武-奥陶系界线标准层型剖面中的无铰纲腕足类生物成因磷灰石,及沉积岩中的REE,U,Th,Sr,Ba,Co,Ni,Cr,V,Cu,Pb,Zn,Sc,Au,As等16种微量元素的系统分析,探讨了稀土元素分布模式及微量元素含量与组合沿剖面变化规律,为寒武-奥陶系界线层型剖面的建立和沉积环境的研究提供了地球化学依据。     

TRACE ELEMENT GEOCHEMISTRY OF INARTICULATE BRACHIOPODS AND SEDIMENTARY ROCK ON THE CAMBRIAN-ORDOVICIAN BOUNDARY

That the contents and compositions of trace elements, especially REE in sedimentary rock and agustite originating from inarticulate brachiopods, conodont, etc. change in the vertical direction usually has a close relation with the stratigraphic boundary of important biologies. This paper systematically analyses REE and 16 trace elements such as U, Th, Sr, Ba, Co, Ni, Cr, V, Cu, Pb, Zn, Sc, Au, As in sedimentary rocks and the agustite on the standard stratified section of the Cambrian-Ordovician Boundary in Dayangcha, Huniiang, Jilin Province. Based on this, the authors investigate the REE distribution pattern and the law of the contents and compositions of trace elements changing, providing the geochemical evidence for building stratified sections of the Cambrian-Ordovician boundary and discussing sedimentary environments.     

双波长分光光度法测定水中硝酸盐

用紫外法测定水中硝酸盐已被美国列为标准方法,但易受常见化合物干扰,需进行不同的校正。我们根据硝酸盐的紫外吸收特征和双波长分光光度计的优点,对硝酸盐的吸收曲线用数学方法处理,其微分系数dA/dλ与硝酸盐的浓度有线性关系。以A/2.0毫微米为纵座标,波长(λ)为横座标作图,获得一级导数光谱,最高点在271毫微米,是吸收曲线斜率最大的地方,此波长用做λ_2,λ_1选用226毫微米,硝酸盐用氮计算时其线性范围在0—6毫克/升,检测限为0.07毫