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SEBS分子链在不同溶剂中的荧光特性
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作者 张远方 林美 +4 位作者 李开武 徐绍钦 刘文峰 程欢 陈韶云 《塑料》 CAS CSCD 北大核心 2018年第2期57-60,共4页
利用荧光光谱法对SEBS分子链在不同溶剂中的荧光特性进行了分析。研究表明,室温下,SEBS在四氢呋喃和环己烷中的荧光发射波长为380 nm,且为本征荧光;而在甲苯溶液中的发射波长为375 nm,相对于本征荧光蓝移动了5 nm。在共振散色光谱中,3... 利用荧光光谱法对SEBS分子链在不同溶剂中的荧光特性进行了分析。研究表明,室温下,SEBS在四氢呋喃和环己烷中的荧光发射波长为380 nm,且为本征荧光;而在甲苯溶液中的发射波长为375 nm,相对于本征荧光蓝移动了5 nm。在共振散色光谱中,3种体系的共振光强度都是随着溶液浓度的增大呈线性增加,但甲苯溶液体系共振散色光强度的变化较缓慢。造成这些现象的原因在于四氢呋喃和环己烷分子中没有苯环结构,不具备荧光发射的条件,因而SEBS在这两种溶剂中具有本征荧光效应;而甲苯和SEBS都具有苯环结构,相邻的苯环间通过π电子的相互重叠形成T型结构的二聚体,导致了荧光强度的减弱和共振散色光强度变化较缓慢。 展开更多
关键词 SEBS 荧光光谱 共振散色 二聚体 构象
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Investigations on Left Hand Cut Contribution to Determination of κ(700) Pole
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作者 ZHOU Zhi-Yong 《Communications in Theoretical Physics》 SCIE CAS CSCD 2007年第5期883-886,共4页
The uncertainties of background contributions to J = 0 partial wave πK scattering phase shifts are carefully studied. We firstly point out that the circular cuts exhibit different characters in S1/1 and S3/2 waves. W... The uncertainties of background contributions to J = 0 partial wave πK scattering phase shifts are carefully studied. We firstly point out that the circular cuts exhibit different characters in S1/1 and S3/2 waves. While the former contributes negatively to the scattering length parameter, the latter contributes positively, i.e., has a wrong sign. This fact indicates that short range force contribu tions to the phase shift are non-negligible in the exotic channel. Nevertheless, it is verified that the κ pole will be affected only slightly with respect to the theoretical uncertainty in estimating the left hand cut contributions. 展开更多
关键词 πK scattering UNITARITY dispersion relations κ resonance
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Studies on σ Resonance in a New Unitarization Approach
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作者 ZHANGPeng ZHOUZhi-Yong QINGuang-You ZHENGHan-Qing 《Communications in Theoretical Physics》 SCIE CAS CSCD 2005年第2期268-274,共7页
The pole position of the σ meson is determined using the recently proposednew unitarization method combined with the two-loop SU(2) X SU(2) chiral perturbation theoryresults. The scattering length parameters and the ... The pole position of the σ meson is determined using the recently proposednew unitarization method combined with the two-loop SU(2) X SU(2) chiral perturbation theoryresults. The scattering length parameters and the effective range parameters predicted by our methodare in good agreement with experimental results. It is found that M_σ = 542 ± 26 ± 39 MeV, Γ_σ= 546 ± 122 ± 25 MeV. 展开更多
关键词 ππ scattering UNITARITY dispersion relations
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True-color real-time imaging and spectroscopy of carbon nanotubes on substrates using enhanced Rayleigh scattering 被引量:1
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作者 Wenyun Wu Jingying Yue +21 位作者 Xiaoyang Lin Dongqi Li Fangqiang Zhu Xue Yin Jun Zhu Jiangtao Wang Jin Zhang Yuan Chen Xinhe Wang Tianyi Li Yujun He Xingcan Dai Peng Liu Yang wei Jiaping Wang Wei Zhang Yidong Huang Li Fan Lina Zhang Qunqing Li Shoushan Fan Kaili Jiang 《Nano Research》 SCIE EI CAS CSCD 2015年第8期2721-2732,共12页
Single-walled carbon nanotubes (SWCNTs) illuminated by white light should appear colored due to resonance Rayleigh scattering. However, true-color imaging of SWCNTs on substrates has not been reported, because of th... Single-walled carbon nanotubes (SWCNTs) illuminated by white light should appear colored due to resonance Rayleigh scattering. However, true-color imaging of SWCNTs on substrates has not been reported, because of the extremely low scattering intensity of SWCNTs and the strong substrate scattering. Here we show that Rayleigh scattering can be greatly enhanced by the interface dipole enhancement effect. Consequently colorful SWCNTs on substrates can be directly imaged under an optical microscope by wide field supercontinuum laser illumination, which facilitates high throughput chirality assignment of individual SWCNTs. This approach, termed "Rayleigh imaging microscopy", is not restricted to SWCNTs, but widely applicable to a variety of nanomaterials, which enables the colorful nanoworld to be explored under optical microscopes. 展开更多
关键词 enhanced Rayleigh scattering Rayleigh imaging microscopy true-color imaging carbon nanotube interface dipole
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