全文获取类型
收费全文 | 42篇 |
免费 | 20篇 |
国内免费 | 1篇 |
专业分类
化学 | 16篇 |
晶体学 | 1篇 |
力学 | 2篇 |
物理学 | 44篇 |
出版年
2023年 | 2篇 |
2022年 | 4篇 |
2021年 | 3篇 |
2020年 | 3篇 |
2019年 | 2篇 |
2018年 | 5篇 |
2017年 | 4篇 |
2016年 | 3篇 |
2015年 | 5篇 |
2014年 | 1篇 |
2013年 | 5篇 |
2012年 | 4篇 |
2011年 | 3篇 |
2010年 | 4篇 |
2009年 | 1篇 |
2008年 | 1篇 |
2007年 | 1篇 |
2006年 | 1篇 |
2005年 | 1篇 |
2004年 | 2篇 |
2003年 | 1篇 |
2001年 | 1篇 |
2000年 | 3篇 |
1999年 | 1篇 |
1996年 | 1篇 |
1995年 | 1篇 |
排序方式: 共有63条查询结果,搜索用时 0 毫秒
61.
本文采用固相法在500℃合成了Er3+/Eu3+共掺BiOCl 荧光粉, 并通过XRD, SEM, 吸收, 激发和发射光谱研究了其结构、形貌和发光特性. XRD 和SEM结果表明在500℃下即可成功合成纯四方相片层结构的Er3+/Eu3+共掺BiOCl荧光粉. 吸收光谱表明掺杂Er3+/Eu3+离子使BiOCl形成杂质能级; 激发光谱显示该荧光粉具有来自于基质BiOCl价带(VB)到导带(CB)跃迁的优异宽带近紫外激发特性. 在380 nm近紫外光激发下, 同时获得了Er3+离子和Eu3+离子的特征发射峰, 其中发光中心位于410 nm (2H9/2→4I15/2), 525 nm (2H11/2→4I15/2), 554 nm (4S3/2→4I15/2), 673 nm (4F9/2→4I15/2)的发射峰来自于Er3+离子的跃迁, 而581 nm(5D0→7F0), 594 nm (5D0→7F1), 622 nm (5D0→7F2), 653 nm (5D0→7F3), 699 nm (5D0→7F4)的发射峰则来自于Eu3+离子的跃迁. 值得注意的是, 与传统Er3+/Eu3+掺杂的材料不同, 该荧光粉还具有独特高效的紫光(Er3+)和长波红光(Eu3+)发射特性, 分析表明这与BiOCl的结构有关; 并且通过改变掺杂浓度, 实现了发光颜色由黄绿光→黄光→橙红光的调节. 研究结果表明Er3+/Eu3+共掺BiOCl荧光粉有望成为一种潜在的近紫外激发白光LED荧光粉. 相似文献
62.
DAI Jianming ZHANG Lizhe ZHANG Weili CHAI Lu WANG Yong Xing Qirong WANG Qingyue 《中国光学快报(英文版)》2000,9(5)
A compact and efficient CW Cr: LiSGaF laser pumped by two 670 nm laser diodes was reported. Average power as high as 125 mW was generated with a absorbed pump power of 800 mW. The slope efficiency was 17.2%, and the threshold was 72 mW. The tunability of the laser in detail was investigated and a tuning range of 100 nm from 790 to 890 nm was obtained. 相似文献
63.
Resonance enhancement has been increasingly employed in the emergent femtosecond stimulated Raman spectroscopy (FSRS) to selectively monitor molecular structure and dynamics with improved spectral and temporal resolutions and signal-to-noise ratios. Such joint efforts by the technique-and application-oriented scientists and engineers have laid the foundation for exploiting the tunable FSRS methodology to investigate a great variety of photosensitive systems and elucidate the underlying functional mechanisms on molecular time scales. During spectral analysis, peak line shapes remain a major concern with an intricate dependence on resonance conditions. Here, we present a comprehensive study of line shapes by tuning the Raman pump wavelength from red to blue side of the ground-state absorption band of the fluorescent dye rhodamine 6G in solution. Distinct line shape patterns in Stokes and anti-Stokes FSRS as well as from the low to high-frequency modes highlight the competition between multiple third-order and higher-order nonlinear pathways, governed by different resonance conditions achieved by Raman pump and probe pulses. In particular, the resonance condition of probe wavelength is revealed to play an important role in generating circular line shape changes through oppositely phased dispersion via hot luminescence (HL) pathways. Meanwhile, on-resonance conditions of the Raman pump could promote excited-state vibrational modes which are broadened and red-shifted from the coincident ground-state vibrational modes, posing challenges for spectral analysis. Certain strategies in tuning the Raman pump and probe to characteristic regions across an electronic transition band are discussed to improve the FSRS usability and versatility as a powerful structural dynamics toolset to advance chemical, physical, materials, and biological sciences. 相似文献