稀疏矩阵及稀疏线性方程组求解已成为大规模电网状态估计计算效率的瓶颈,阐释了基于BTF和Gilbert-Peierls算法的稀疏矩阵直接求解器KLU(Clark Kent LU),并将其嵌入到智能调度技术支持系统中生产运行的状态估计程序功能。首先在计算得到...稀疏矩阵及稀疏线性方程组求解已成为大规模电网状态估计计算效率的瓶颈,阐释了基于BTF和Gilbert-Peierls算法的稀疏矩阵直接求解器KLU(Clark Kent LU),并将其嵌入到智能调度技术支持系统中生产运行的状态估计程序功能。首先在计算得到雅可比矩阵的基础上基于OpenMP并行化技术快速求解信息矩阵;然后使用KLU求解器进行信息矩阵的因子表符号分析和数值分解;最后在状态估计计算过程中使用KLU求解器求解线性方程组,从而提高大规模电网状态估计的计算效率。通过省中心、分中心、模型数据中心D5000的状态估计实际应用,证明了该方法的有效性和实用性。展开更多
The spectral parameters of Nd3+ ions in Nd3+:Klu(WO4)2 crystal were calculated based on Judd-Ofelt theory and obtained as follows: for the oscillator strengths ?λ: ?2 = 7.5029×10-20 cm2, ?4 = 7.1837×10-20...The spectral parameters of Nd3+ ions in Nd3+:Klu(WO4)2 crystal were calculated based on Judd-Ofelt theory and obtained as follows: for the oscillator strengths ?λ: ?2 = 7.5029×10-20 cm2, ?4 = 7.1837×10-20 cm2 and ?6 = 3.1189×10-20 cm2; the radiative lifetime is 123 μs; the quantum efficiency is equal to 64.55%; and β1 = 0.5498, β2 = 0.3943, β3 = 0.0551 and β4 = 0.0027 for the fluorescence branch ratios.展开更多
The laser host crystals of KLu(WO4)2(KLuW) with large sizes up to 43 × 35 × 16 mm3 have been grown along, [110], b, and c crystallographic directions, respectively, by the top-seeded solution growth (TSSG) s...The laser host crystals of KLu(WO4)2(KLuW) with large sizes up to 43 × 35 × 16 mm3 have been grown along, [110], b, and c crystallographic directions, respectively, by the top-seeded solution growth (TSSG) slow-cooling method. The macro defects are observed using optical microscopy. The main defects found were cracks, inclusions, growth striations, sector boundaries and twin boundaries. The formation mechanism and approaches to reduce or eliminate the defects have been analyzed.展开更多
Optical absorption and emission intensities of Nd3+ ion in KLu(WO4)2 crystal were investigated. Based on the Judd-Offelt theory, we calculated the following spectral parameters: phenomenological intensity parameters ...Optical absorption and emission intensities of Nd3+ ion in KLu(WO4)2 crystal were investigated. Based on the Judd-Offelt theory, we calculated the following spectral parameters: phenomenological intensity parameters Ω2=5.567×10–20, Ω4=3.597×10–20, and Ω6= 3.800×10–20 cm2. The radiative lifetime of levels 4F3/2 was 182.58 μs. The fluorescence branching ratio for the transition 4F3/2→4I11/2 was 46.98%. In addition, the radiative transition probabilities AJ,J’, oscillator strengths PJ,J’ and the values of inte...展开更多
文摘稀疏矩阵及稀疏线性方程组求解已成为大规模电网状态估计计算效率的瓶颈,阐释了基于BTF和Gilbert-Peierls算法的稀疏矩阵直接求解器KLU(Clark Kent LU),并将其嵌入到智能调度技术支持系统中生产运行的状态估计程序功能。首先在计算得到雅可比矩阵的基础上基于OpenMP并行化技术快速求解信息矩阵;然后使用KLU求解器进行信息矩阵的因子表符号分析和数值分解;最后在状态估计计算过程中使用KLU求解器求解线性方程组,从而提高大规模电网状态估计的计算效率。通过省中心、分中心、模型数据中心D5000的状态估计实际应用,证明了该方法的有效性和实用性。
基金This work was supported by the National Natural Science Foundation of China (50272066) and Key Project of Science and Technology of Fujian Province (2001F004)
文摘The spectral parameters of Nd3+ ions in Nd3+:Klu(WO4)2 crystal were calculated based on Judd-Ofelt theory and obtained as follows: for the oscillator strengths ?λ: ?2 = 7.5029×10-20 cm2, ?4 = 7.1837×10-20 cm2 and ?6 = 3.1189×10-20 cm2; the radiative lifetime is 123 μs; the quantum efficiency is equal to 64.55%; and β1 = 0.5498, β2 = 0.3943, β3 = 0.0551 and β4 = 0.0027 for the fluorescence branch ratios.
文摘The laser host crystals of KLu(WO4)2(KLuW) with large sizes up to 43 × 35 × 16 mm3 have been grown along, [110], b, and c crystallographic directions, respectively, by the top-seeded solution growth (TSSG) slow-cooling method. The macro defects are observed using optical microscopy. The main defects found were cracks, inclusions, growth striations, sector boundaries and twin boundaries. The formation mechanism and approaches to reduce or eliminate the defects have been analyzed.
基金Project supported by Program for New Century Excellent Talents in University (NCET-08-0722)
文摘Optical absorption and emission intensities of Nd3+ ion in KLu(WO4)2 crystal were investigated. Based on the Judd-Offelt theory, we calculated the following spectral parameters: phenomenological intensity parameters Ω2=5.567×10–20, Ω4=3.597×10–20, and Ω6= 3.800×10–20 cm2. The radiative lifetime of levels 4F3/2 was 182.58 μs. The fluorescence branching ratio for the transition 4F3/2→4I11/2 was 46.98%. In addition, the radiative transition probabilities AJ,J’, oscillator strengths PJ,J’ and the values of inte...
