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981.
982.
介绍了光纤寿命预期的疲劳实验方法和筛选实验方法。采用这两种方法,利用电子万能材料试验机和光纤筛选复绕机对室温下光纤进行了疲劳性能实验。实验得出,在张力小于850g的情况下,制导光纤的寿命可以达到10年以上;光纤的韦伯参数md和疲劳参数nd的大小影响光纤寿命。实验表明,当光纤的使用状态受力较大时,或使用贮存状态相差较大时,宜选用动态方法进行寿命预期;当贮存和使用状态受力变化不大时,宜选用筛选复绕方法预期光纤寿命。制导光纤寿命模型宜选用动态疲劳模型,通信光纤可选用筛选实验模型。实验还表明,提高光纤的抗疲劳因子nd和减小光缆中光纤的应变,可以更好地保持光缆中光纤的使用寿命和可靠性。 相似文献
983.
984.
We present nonlinear spectra of four-level ladder cesium atoms employing 6 S1/2→6 P3/2→7 S1/2→30 P3/2 scheme of a room temperature vapor cell.A coupling laser drives Rydberg transition,a dressing laser couples two intermediate levels,and a probe laser optically probes the nonlinear spectra via electromagnetically induced transparency(EIT).Nonlinear spectra are detected as a function of coupling laser frequency.The observed spectra exhibit an enhanced absorption(EA) signal at coupling laser resonance to Rydberg transition and enhanced transmission(ET) signals at detunings to the transition.We define the enhanced absorption(transmission) strength,HEA(HET),and distance between two ET peaks,γET,to describe the spectral feature of the four-level atoms.The enhanced absorption signal HEA is found to have a maximum value when we vary the dressing laser Rabi frequency Ωd,corresponding Rabi frequency is defined as a separatrix point,ΩdSe.The values of ΩdSe and further η=ΩdSe/Ωc are found to depend on the probe and coupling Rabi frequency but not the atomic density.Based on ΩdSe,the spectra can be separated into two regimes,weak and strong dressing ranges,Ωd≤ΩdSe and Ωd≥QdSe,respectively.The spectroscopies display different features at these two regimes.A four-level theoretical model is developed that agrees well with the experimental results in terms of the probe-beam absorption behavior of Rabi frequency-dependent dressed states. 相似文献
985.
The analysis of the LHCb data on \begin{document}$X(6900)$\end{document} ![]()
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found in the di-\begin{document}$J/\psi$\end{document} ![]()
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system was performed using a momentum-dependent Flatté-like parameterization. The use of the pole counting rule and spectral density function sum rule provides consistent evidence that both confining and molecular states are possible. Alternatively, the nature of \begin{document}$X(6900)$\end{document} ![]()
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cannot be distinguished if only the di-\begin{document}$J/\psi$\end{document} ![]()
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experimental data with current statistics are available. Nevertheless, we found that the lowest state in the di-\begin{document}$J/\psi$\end{document} ![]()
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system likely has the same quantum numbers as \begin{document}$X(6900)$\end{document} ![]()
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, and \begin{document}$X(6900)$\end{document} ![]()
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is probably not interpreted as a \begin{document}$J/\psi-\psi(2S)$\end{document} ![]()
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molecular state. 相似文献
986.
Zheng Chenglong Li Jie Li Jitao Yue Zhen Wang Silei Li Mengyao Zhao Hongliang Hao Xuanruo Zang Huaping Zhang Yating Yao Jianquan 《中国科学:物理学 力学 天文学(英文版)》2021,64(11):1-12
The usage of full-color imaging in digital pathology produces significant results. Compared with a grayscale image or a pseudocolor image containing contrast information, a full-color image can identify and detect the target object better with color texture information. Fourier ptychographic microscopy(FPM) is a high-throughput computational imaging technique that breaks the tradeoff between high resolution(HR) and a large field of view. It also eliminates the artifacts of scanning and stitching in digital pathology and improves its imaging efficiency. However, the conventional full-color digital pathology based on FPM is still time-consuming because of the repeated experiments with tri-wavelengths. A color transfer FPM approach termed "CFPM" was reported. The color texture information of a low-resolution full-color pathologic image is directly transferred to the HR grayscale FPM image captured by only a single wavelength. Both of the color space of FPM based on the standard CIE-XYZ color model and the display based on the standard RGB color space were established. Different FPM colorization schemes were analyzed and compared with 30 biological samples. Three types of evaluation approaches were provided, including the root-mean-square error(RMSE), the difference maps, and the image histogram cosine similarity. The average RMSE values of the conventional method and CFPM compared with the ground truth were 5.3% and 5.7%, respectively. Therefore, the reconstruction time is significantly reduced by 2/3 with the sacrifice of precision of only 0.4%. The CFPM method is also compatible with advanced fast FPM approaches to further reduce computation time. 相似文献
987.
Lei Pang Yingjuan Shao Wenqi Zhong Hao Liu 《Proceedings of the Combustion Institute》2021,38(3):4121-4129
Oxy-coal combustion with pressurized fluidized beds has recently emerged as a promising carbon capture and storage (CCS) technology for coal-fired power plants. Although a large number of energy efficiency analyses have shown that an increase in combustion pressure can further increase the net plant efficiency, there are few experimental studies of pressurized oxy-coal combustion conducted on fluidized bed combustors/boilers with continuous coal feeding. In this study, oxy-coal combustion experiments with lignite and anthracite were conducted with a 30 kWth pressurized fluidized bed combustor within the pressure range of 0.1 MPa to 0.4 MPa. The investigation focused on the elucidation of the impacts of combustion pressure on the combustion performance, pollutant emissions and desulfurization of oxy-coal combustion in fluidized beds. The results showed that an increase in pressure increased the combustion efficiency and combustion rate of coal particles, and the promoting effect of pressure increase was more significant for the high rank coal with smaller particle size and the high O2 concentration atmosphere. For both coals, NOx emissions decreased with pressure but N2O emissions increased with pressure and accounted for a considerable part of the nitrogen oxide pollutants under high pressure oxy-coal combustion conditions. The pressure had insignificant impact on the SO2 emissions of oxy-coal combustion but an increase in pressure enhanced the direct desulfurization of limestone. 相似文献
988.
先前报道的2,7-二苯芴酮具有不寻常的,伴随150 nm荧光红移的聚集诱导发光现象. 通过重复实验,发现这种异常行为由合成的2,7-二苯芴酮中少量2,7-二苯芴(DPF)造成. 固态纯2,7-二苯芴酮分子在528 nm处确实有强烈的荧光,是在二氯甲烷稀溶液中的4∽5倍(542 nm),但在固体中是蓝移而不是红移. 合成的2,7-二苯芴酮固体的荧光增强和波长红移现象由少量2,7-二苯芴杂质造成. 在稀溶液中,2,7-二苯芴的荧光远强于2,7-二苯芴酮且波长较短,当2,7-二苯芴酮中含有痕量(约1%)2,7-二苯芴时,主要的荧光峰来自于2,7-二苯芴. 因为2,7-二苯芴的吸收峰与2,7-二苯芴酮重叠,所以2,7-二苯芴的电子能可以转移到2,7-二苯芴酮上. 随着浓度的增加,因为2,7-二苯芴与周围2,7-二苯芴酮分子的距离更近,能量转移会变快. 这造成了2,7-二苯芴的荧光猝灭(356和372 nm)和2,7-二苯芴酮的荧光增强(溶液中542 nm,固体中528 nm). 因此,在高浓度溶液或者固体中,仅有542或528 nm的荧光峰出现,356和372 nm 处荧光峰消失. 相似文献
989.
990.
Yi ZHU Kumar Shyam Chenlu HU Zixuan CHEN Yapeng ZHANG Fengyi ZHAO Xianglun WEI Limin DUAN Nu XU Hao QIU 《原子核物理评论》2021,38(4):416-422
低温高密核物质测量谱仪(CEE)是研究高重子数密度区核物质性质的重离子碰撞实验谱仪。使用了先进的 SAMPA 电子学读出芯片的时间投影室(TPC)是 CEE 最核心的探测器。在集团重建的过程中,同一排读出板的信号被首先重建成 2 维集团,然后根据 2 维集团的 ADC 加权平均位置重建击中点。当信号 ADC 随漂移时间变化呈峰-谷-峰结构时,一个集团可能被重建成两个或更多击中点,从而提高双径迹分辨能力。使用模拟信号的测试显示,该重建算法在$x/ y$ 方向可以达到0.100/0.043 cm的位置分辨能力和1.1/2.8 cm的双径迹分辨能力。 相似文献