共查询到17条相似文献,搜索用时 78 毫秒
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核磁共振T2谱多指数反演算法是开展复杂体系样品核磁共振(NMR)弛豫研究最重要的数学工具. 常用的T2谱多指数反演算法一般都是事先给出弛豫时间T2分布的布点, 然后转化为线性拟合问题进行求解. 在求解的T2谱较为分散的时候, 反演得到的T2谱精确度不高, 分辨率较低. 非线性拟合是解决这个问题的有效办法. 本文针对分散T2谱反演利用非线性拟合时遇到的初值依赖及运算复杂问题, 利用线性回归最小二乘方法, 改进了其中的带非负约束非线性优化模型, 将搜索的反演参数从T2, f 减少为T2, 加快了收敛速度, 减少了对初值的依赖, 提高了反演精度, 使算法更加稳健. 通过用改进的Levenberg-Marquardt算法和差分进化算法进行计算机模拟反演及实验数据反演, 验证了改进方法在核磁共振T2 谱反演中的有效性. 相似文献
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大气CO2是重要的温室气体,对大气CO2的全球监测有助于增进人类对气候变化的理解。相比于天基平台,地基观测数据通常具有更高的光谱分辨率、信噪比及其他已知参数,更容易实现较高的反演精度。地基反演方法可以作为天基算法的基础,并为天基观测结果提供必要的验证。本文针对地基观测的特点,建立了使用地基FTS数据反演大气CO2柱浓度的方法。模拟计算显示该方法在一定的系统误差条件下,具有获得较高反演精度的能力。对地基FTS实测数据进行的反演实验表明,该方法能够获得较精确的大气CO2浓度信息。 相似文献
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针对传统非相干宽带腔增强吸收光谱浓度反演方法的定量结果易受镜片反射率标定误差的影响问题, 提出了一种基于测量大气O2-O2吸收的浓度反演方法. 该方法是将非相干宽带腔增强吸收光谱技术的光学增强腔等效成吸收光程不随波长变化的多次反射池, 首先根据测得的宽带腔增强大气吸收谱和参考谱计算出光学厚度, 并应用差分光学吸收光谱算法拟合修正后的气体吸收截面到光学厚度, 反演得到大气中O2-O2以及被测气体的柱浓度, 然后根据O2-O2在大气中的含量已知且相对稳定这一特性, 确定出等效多次反射池的吸收光程, 最后从被测气体的柱浓度中扣除吸收光程信息得到被测气体的浓度值. 以监测大气中NO2实验为例, 应用该方法在454-487 nm波段反演得到了大气NO2的浓度(1-30 ppbv范围内), 并将反演结果与传统浓度反演方法的结果进行了对比, 发现两者的不一致性在7%以内. 实验结果表明, 非相干宽带腔增强吸收光谱技术可以利用大气O2-O2的吸收来定量其他被测气体的浓度, 而且定量结果对镜片反射率的标定误差不敏感. 相似文献
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利用野外测量21种地表岩石的高光谱发射率数据,进行包络线去除和归一化处理后,运用逐步回归法进行波段选择,分析了SiO2含量与包络线去除后特征波段发射率的定量关系。在此基础上,通过比较12种SiO2光谱指数,建立了定量反演SiO2含量的最优模型。结果表明:构建的SiO2光谱指数能有效预测SiO2含量,其中基于11.18和12.36μm波段的归一化SiO2光谱指数(normalization silicon dioxide index,NSDI)的预测能力最高;与回归模型相比,光谱指数更简单、实用;研究结果在岩石种类鉴定及SiO2含量的高精度提取方面有重要应用价值。 相似文献
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Chengying Xie Xiaohong Zhou Yuhu Zhang Yingxiang Guo Xiangguo Lei Yong Zheng Minliang Liu Litao Song Hualei Wang Haiping Yu Wentao Guo Peng Luo Zhijun Wu Lihua Zhu Xiaoguang Wu 《中国科学G辑(英文版)》2005,48(4):442-449
High-spin states in 190Tl have been studied via the 160Gd(35Cl, 5nγ) reaction. The level scheme, consisting of the πh
9/2⊗vi
13/2 oblate band and a cascade with character of single particle excitations, has been established. Spin values have been firmly
assigned to the oblate band in 190Tl, resulting in low-spin signature inversion in the πh
9/2⊗vi
13/2 oblate band for the first time. Based on the similarity of the level structure in doubly odd Tl nuclei, spin values for the
oblate bands in 192–200Tl should be re-assigned, and a consistent low-spin signature inversion has occurred in these oblate deformed nuclei. The
low-spin signature inversion phenomena can be interpreted qualitatively by using the 2-quasiparticle plus rotor model including
p-n residual interactions. 相似文献
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Finite pulse durations in diverse pulse schemes lead to the reduction of the magnitude of the magnetization vector due to T1 and T2 effects during the radio-frequency pulses. This paper presents an analysis of the steady state signal in the presence of relaxation effects during radio-frequency pulses in MRI spoiled gradient echo sequences. It is shown that minor attenuations of the magnetization vector can have dramatic consequences on the measured signal, and may thus entail a loss in SNR benefits at high static magnetic fields if a careful analysis is not performed. It is emphasized that it is the time-integrated magnetization vector trajectory that matters for these effects and not only the pulse duration. Some experimental results obtained on a phantom at 3 T verify this analysis. 相似文献
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设计了一种脉冲形成线用新型CaO-TiO2-Al2O3基介质陶瓷体系,采用传统固相法通过优化组分和制备工艺,调控材料的微结构,获得了介电性能优异的介质陶瓷。其介电常数在15~35之间可调,介电损耗小于0.002,频率稳定性好。在厚度为1 mm时,介电强度高达50 kV/mm。研究了厚度对CaO-TiO2-Al2O3基介质陶瓷介电强度的影响规律,当厚度从1 mm减小到0.1 mm时,介电强度呈非线性增大,从50 kV/mm(1 mm厚样品)提高到92 kV/mm(0.1 mm厚样品),可见,CaO-TiO2-Al2O3基介质陶瓷的电击穿与其机械损坏具有相似性。结合CaO-TiO2-Al2O3基介质陶瓷的化学组分和微观结构,CaO-TiO2-Al2O3基介质陶瓷优越的电击穿特性可以用弱点击穿理论解释。 相似文献
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The high-resolution infrared spectrum of HCF3 was studied in the ν6 fundamental (near 500 cm−1) and in the 2ν6 overtones (near 1000 cm−1) regions. The present study reports on the analysis of the hot bands in the ν6 region, as well as the first observation and assignment of the 2ν62 perpendicular band. Using ν6, 2ν6±2–ν6±1 and 2ν62 experimental wavenumbers, accurate coefficients C0 and DK0 of the K-dependent ground-state energy terms were obtained, using the so-called “loop method.” Ground-state energy differences Δ(K,J)=E0(K,J)−E0(K−3,J) were obtained for K=3–30. A least-squares fit of 81 such differences gave the following results (in cm−1): C0=0.1892550(15); DK0=2.779(26) × 10−7. 相似文献
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Ke Zhang Simian Li Guangfei Liang Huan Huang Yang Wang Tianshu Lai Yiqun Wu 《Physica B: Condensed Matter》2012,407(13):2447-2450
The crystallization dynamics of as-deposited amorphous Ge2Sb2Te5 films induced by nano- and picosecond single laser pulse irradiation is studied using in situ reflectivity measurements. Compared with nanosecond laser pulse, the typical recalescence phenomenon did not appear during the picosecond laser pulse-induced crystallization processes when the pulse fluence gradually increased from crystallization to ablation threshold. The absence of melting and recalescence phenomenon significantly decreased the crystallization time from hundreds to a few tens of nanoseconds. The role of pulse duration time scale on the crystallization process is qualitatively analyzed. 相似文献
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本文在多通道量子数亏损理论(MQDT)框架下,利用相对论多通道理论(RMCT),分别在冻结实近似、 考虑Δl=-1的偶极极化效应、Δl=+1的偶极极化效应、Δl=± 1的偶极极化效应、伸缩模效应以及同时考虑偶极极化效应和伸缩模效应等不同层次近似下,系统地计算了碱金属Li, Na, K, Rb, Cs和Fr七个里德伯系列的能级,即ns2S1/2, np2P1/2, np2P3/2, nd2D3/2, nd2D5/2, nf2F5/2 和nf2F7/2.计算结果表明,电子关联效应对碱金属原子的里德伯能级的影响很大.总的来说,偶极极化效应比伸缩模效应重要,而在偶极极化效应中, Δl = + 1的偶极极化效应比Δl = - 1的偶极极化效应重要.但对于Na的ns2S1/2,(nd2D3/2,nd2D5/2)里德伯系列的能级,和Li的(np2P1/2,np2P3/2)里德伯系列的能级,是伸缩模效应比较重要. 相似文献