Pt掺杂MoSe2吸附CF3I分解组分的第一性原理研究

CF₃I作为SF₆最具潜力的新型环保绝缘气体,在电气设备出现局部放电、过热等缺陷故障时,会产生C₂F₆和C₂F₄等强温室气体,为确保电力设备稳定运行,有必要对CF₃I典型分解组分吸附去除.本文基于密度泛函理论的第一性原理计算方法,通过吸附能、吸附距离、电荷转移和态密度等吸附指标,分别探究了不同数量Pt掺杂MoSe₂对C₂F₆和C₂F₄气体分子的吸附性能.研究结果表明：不同数量Pt掺杂在MoSe₂表面均存在稳定的掺杂结构,且相较本征MoSe₂,Pt掺杂后的MoSe₂导电性均得到了有效增强;Pt掺杂MoSe₂对CF₃I分解组分的吸附效果：Pt₂-MoSe₂>Pt-MoSe<...     

CF2自由基与HNCO反应机理的量子化学研究

采用密度泛函理论B3LYP 方法研究了CF2 自由基与HNCO 的反应机理, 并在B3LYP/6-311＋＋G**水平上对反应物、中间体、过渡态进行了全几何参数优化, 通过频率分析和内禀反应坐标(IRC)确定了中间体和过渡态.为了得到更精确的能量值, 又用CCSD(T)/6-311＋＋G**方法计算了在B3LYP/6-311＋＋G**水平优化后的各个驻点的相对能量. 根据统计热力学及用Winger校正的Eyring过渡态理论,利用自编程序,计算不同温度下低势垒反应的平衡常数和速率常数.计算结果表明单重态的CF2 自由基与HNCO 的反应有四条反应通道, 三重态的CF2 自由基与HNCO 的反应有两条反应通道.其中单重态反应通道CF2＋HNCO→1IM1→1TS1→1IM2→1TS2→1IM3→CF2NH＋CO(P1)为主反应通道.三重态反应通道CF2＋HNCO→36IM1→36TS1→36IM2→HCF2+NCO(3P5)为主反应通道.     

Constrained snake vs. conventional snake for carotid ultrasound automated IMT measurements on multi-center data sets

Accurate intima-media thickness (IMT) measurement of the carotid artery from minimal plaque ultrasound images is a relevant clinical need, since IMT increase is related to the progression of atherosclerosis.In this paper, we describe a novel dual snake-based model for the high-performance carotid IMT measurement, called Carotid Measurement Using Dual Snakes (CMUDS). Snakes (which are deformable contours) adapt to the lumen-intima (LI) and media-adventitia (MA) interfaces, thus enabling the IMT computation as distance between the LI and MA snakes. However, traditional snakes might be unable to maintain a correct distance and in some spatial location along the artery, it might even collapse between them or diverge. The technical improvement of this work is the definition of a dual snake-based constrained system, which prevents the LI and MA snakes from collapsing or bleeding, thus optimizing the IMT estimation.The CMUDS system consists of two parametric models automatically initialized using the far adventitia border which we automatically traced by using a previously developed multi-resolution approach. The dual snakes evolve simultaneously and are constrained by the distances between them, ensuring the regularization of LI/MA topology. We benchmarked our automated CMUDS with the previous conventional semi-automated snake system called Carotid Measurement Using Single Snake (CMUSS).Two independent readers manually traced the LIMA boundaries of a multi-institutional, multi-ethnic, and multi-scanner database of 665 CCA longitudinal 2D images. We evaluated our system performance by comparing it with the gold standard as traced by clinical readers.CMUDS and CMUSS correctly processed 100% of the 665 images. Comparing the performance with respect to the two readers, our automatically measured IMT was on average very close to that of the two readers (IMT measurement biases for CMUSS was equal to −0.011 ± 0.329 mm and −0.045 ± 0.317 mm, respectively, while for CMUDS, it was 0.030 ± 0.284 mm and −0.004 ± 0.273 mm, respectively). The Figure-of-Merit of the system was 98.5% and 94.4% for CMUSS, while 96.0% and 99.6% for CMUDS, respectively. Results showed that the dual-snake system CMUDS reduced the IMT measurement error accuracy (Wilcoxon, p < 0.02) and the IMT error variability (Fisher, p < 3 × 10⁻²).We propose the CMUDS technique for use in large multi-centric studies, where the need for a standard, accurate, and automated IMT measurement technique is required.     

聚对苯二甲酸乙二酯膜的表面碳氟等离子体改性及XPS取样深度与接触角间的关系

高聚物界面的能量、结构等性质，对理论研究和实际应用都是极为重要的．因为许多聚合物材料都具有一个或多个界面的多相结构，这些界面的结构和强度等，显著地影响着这些多相材料的物理、力学性能等，而它们之间的关系，是一个极为复杂的问题，只有综合界面科学、流变学、...     

Insight and performance of LC-DFT vs DFT in the NMR shielding and chemical shift calculations: Case of CHClCH?CF3

Fifteen density functional theory (DFT) methods and fifteen long-range corrected density functional theory (LC-DFT) methods were used in the present work to assess nuclear magnetic resonance parameters such as nuclear shielding constant (NSC), nuclear chemical shift (NCS), and nuclear anisotropic shielding constant (NAS). These different methods were associated with the full basis set 6-311++G(3df,3pd). The gauge-independent atomic orbital was used for the calculation of nuclear shielding tensors of the nuclei contained in the stereoisomers cis- and trans-CHClCHCF₃. Thus, the effects of LC are clearly observed for heavy nuclei (¹³C, ¹⁹F, ³⁵Cl). The results of NSC, NCS, and NAS from DFT are better described than LC-DFT with regard to the KT3 method. Moreover, the results from the LC-DFT are better described than the standard DFT with regard to CCSD(T). Based on the latter method used as the benchmark, the NSCs of nuclei are well fitted by the competitive functionals LC-TPSSTPSS and LC-PKZBPKZB. In the particular case of the trans-isomer, mPWPKZB was found to be the best method. For the NCSs, the more accurate methods include the latter two LC functionals and the non-LC functionals TPSSTPSS and mPWPKZB. The accuracy of NAS depends strongly on the nuclei. Thus, CAM-B3LYP describes it well for ¹⁹F and LC-PKZBPKZB for ³⁵Cl. The rest of nuclei are well fitted by all the methods except ¹³C₁ and ¹³C₂, which are better reproduced by the LC-DFT except the LC-PKZBPKZB, LC-TPSSTPSS, and CAM-B3LYP functionals.     

A comparative study of CH4 and CF4 rf discharges using a consistent plasma physics and chemistry simulator

A self-consistent, one-dimensional simulator for the physics and chemistry of radio frequency (rf) plasmas was developed and applied for CH₄ and CF₄. The simulator consists of a fluid model for the discharge physics, a commercial Boltzmann equation solver for calculations of electron energy distribution fuction (EEDF), a generalized plasma chemistry code, and an interface module among the three models. The CH₄ and CF₄ discharges are compared and contrasted: CH₄ plasmas are electropositive, with negative ion densities one order of magnitude less than those of electrons, whereas CF₄ plasmas are electronegative, with ten times more negative ions than electrons. The high-energy tail of tire EEDF in CH₄, lies below both the Druyvensteyn and Maxwell distributions, whereas tire EEDF high-energy tail in CF₄ lies between the two. For CH₄, the chemistry model was applied for four species, namely, CH₄ CH₃ CH₂, and H, whereas for CF₄, five species were examined namely CF₄, CF₃, CF₂, CF, and F The predicted densities and profiles compare favorably with experimental data. Finally, the chemistry results were fedback into the physics model until convergence was obtained.     

La3+离子对叶绿体CF1-ATPase活力影响研究

为进一步弄清La3+离子对光合磷酸化及Hill反应影响作用机制,采用分光光度法,控制反应液中La3+离子浓度在0～20μmol.L-1范围,对纯化的游离态CF1-ATPase水解ATP活性测定结果表明:La3+离子对CF1-ATPase具有明显的促进作用。而且随La3+离子浓度增大,CF1-ATPase活性动力学曲线明显呈现"S"型。但当La3+离子浓度大于25μmol.L-1之后,La3+离子对游离态CF1-ATPase则表现出一定的抑制作用。而La3+离子浓度在0～30μmol.L-1范围内,受La3+离子作用类囊体膜CF1-ATPase活性动力学曲线则呈现双"S"形曲线。热稳定性实验结果表明:La3+离子可以降低CF1-ATPase活化能,提高CF1-ATPase的热稳定性。La3+离子对CF1-ATPase活性的影响可能与CF1-ATPase分子上别构位点有关,这也可能是La3+离子促进叶绿体Hill反应的关键部位。     

具有统计增强效应的(CF2)n-PIN夹层探测阵列

采用灵敏区尺寸为φ60mm, 厚度1000μm的大面积电流型厚PIN半导体探测器+聚四氟乙烯片+PA101低噪声放大器, 构建了灵敏度为10^－11C.cm²,具有显著统计增强效应的夹层高灵敏PIN探测阵列. 采用Monte-Carlo数值模拟方法, 研究了该探测阵列的统计增强效应和对γ射线探测灵敏度. 该阵列在极低强度脉冲γ射线探测中具有明显的统计增强效应, 且能量响应平坦, 单个阵列探测范围可达7个量级, 其γ灵敏度比直径为φ20mm, 厚度为250μm的单个PIN探测器高4个量级并可进行直接标定, 是低强度裂变n/γ混合场脉冲γ射线波形面积测量较理想的探测器, 已在有关科学实验中获得成功应用.     

关于sn可度量空间的注记

具有σ局部有限sn网的空间称为sn可度量空间.本文利用紧覆盖映射、点星网、CF族的概念,给出了sn可度量空间的新刻画.