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1.
A europium complex Eu (DBM)3 TPPO (Eu tris(benzoylmethide)-(triphenylphosphine oxide)) and silicon nanoparticles have been hybridized.The hybridization can evidently change the photoluminescence (PL) characteristics of the Eu complex in the following aspects:under an excitation of 390nm,the intensity of the PL peak at 611nm due to the ^5Du-^7F2 transition of the Eu^3 ions has been increased by 30%,and thc integrated PL intensity in the visible range has been increased by nearly 3 times;the PL excitation efficiency beyond 440nm has been improved cvidently;the peak in the PL excitation spectrum shifts from 408nm to 388nm,and the PL decay time decreases from 2.07 to 0.96μs,The experimental results indicatde that in the PL process,the photoexcited energy may transfer from the silicon nanoparticlcs to the Eu^3 ions.  相似文献   
2.
Yi-Peng Li 《中国物理 B》2021,30(8):86109-086109
The evolution of helium bubbles in purity Mo was investigated by in-situ transmission electron microscopy (TEM) during 30 keV He+ irradiation (at 673 K and 1173 K) and post-irradiation annealing (after 30 keV He+ irradiation with the fluence of 5.74×1016 He+/cm2 at 673 K). Both He+ irradiation and subsequently annealing induced the initiation, aggregation, and growth of helium bubbles. Temperature had a significant effect on the initiation and evolution of helium bubbles. The higher the irradiation temperature was, the larger the bubble size at the same irradiation fluence would be. At 1173 K irradiation, helium bubbles nucleated and grew preferentially at grain boundaries and showed super large size, which would induce the formation of microcracks. At the same time, the geometry of helium bubbles changed from sphericity to polyhedron. The polyhedral bubbles preferred to grow in the shape bounded by {100} planes. After statistical analysis of the characteristic parameters of helium bubbles, the functions between the average size, number density of helium bubbles, swelling rate and irradiation damage were obtained. Meanwhile, an empirical formula for calculating the size of helium bubbles during the annealing was also provided.  相似文献   
3.
硅光子学中的关键问题是研制高效率的硅基光源,文章为此提出了一种实现硅基发光的方法。采用共溅射的方法在n+型重掺杂硅衬底上制备了富硅氧化硅(SiO2∶Si)薄膜,然后用热扩散法进行了锰(Mn2+)掺杂和光学活化。高分辨透射电镜观察表明薄膜中形成了3~5 nm的硅纳米晶体。该薄膜在紫外光照射下发射出明亮的绿光,光致发光谱峰位在524 nm(2.36 eV),一般认为这是来自Mn2+能级4T1 →6A1基态跃迁的绿光辐射;其荧光寿命为0.8 ms。将该掺锰富硅二氧化硅(SiO2∶Si∶Mn2+)做成电致发光结构,在低反偏电压下观察到近乎白色的电致发光(EL),光谱范围覆盖了400~800 nm。研究表明,该电致发光谱来源于薄膜中的Mn2+以及氧化硅中的缺陷发光中心两者光谱的叠加;Mn2+的发光是靠薄膜中的热电子来激发的;并由此探讨了薄膜中的硅纳米晶体在电致发光过程中的作用。  相似文献   
4.
发展了恒温电容瞬态数据处理方法 ,称新方法为恒温电容瞬态时间积谱 (ICTTS) .用ICTTS方法测量分析了C70固体 p GaAs异质结的深能级 ,结果发现在C70 固体中存在两个很深的空穴陷阱 ,H1 和H2 ,它们的能级位置分别为Ev 0 85 6eV和Ev 1 0 37eV  相似文献   
5.
A pulsed InGaAsP-Si hybrid laser is fabricated using metal bonding. A novel structure in which the optical coupling and metal bonding areas are transversely separated is employed to integrate the silicon waveguide with an InGaAsP multi-quantum well distributed feedback structure. When electrically pumped at room temperature, the laser operates with a threshold current density of 2.9 kA/cm^2 and a slope efficiency of 0.02 W/A. The 1542nm laser output exits mainly from the Si waveguide.  相似文献   
6.
Etectroluminescence peaking at 1.3 μm is observed from high concentration boron-diffused silicon p^+-n junctions. This emission is efficient at low temperature with a quantum efficiency 40 times higher than that of the band-to-band emission around 1.1 μm, but disappears at room temperature. The 1.3-μm band possibly originates from the dislocation networks lying near the junction region, which are introduced by high concentration boron diffusion.  相似文献   
7.
Single crystalline ZnSe nanowires with both zincblende and wurtzite structures have been synthesized via a chemical vapour deposition method under different growth conditions. The nanowires are usually 50-80nm in diameter, and several tens of microns in length. Room-temperature photoluminescence spectra from zincblende and wurtzite ZnSe nanowires show a broad luminescence band peaked at around 2. 71 e V and a deep level emission band peaked at around 2.00 eV, respectively. Effects of post-growth annealing on the photoluminescence of these nanowires have been investigated. Strong room-temperature band-edge emission could be obtained from the annealed zincblende ZnSe nanowires.  相似文献   
8.
纳米钨合金块体材料的制备   总被引:3,自引:0,他引:3  
高比重钨合金由于具有一系列优异的物理力学性能, 因此在航空航天、国防军工和民用中有着广泛的应用前景.采用纳米技术制备高比重钨合金块体材料有望进一步提高其性能, 促使其应用.本文分析了纳米钨合金在粉末制备和成型烧结中存在的问题, 并针对纳米钨合金粉末成型和烧结过程中晶粒长大问题以及块体材料中存在大量微孔问题, 介绍了数种可行性控制方法.  相似文献   
9.
磁控溅射淀积掺Er富Si氧化硅膜中Er3+ 1.54μm光致发光   总被引:6,自引:1,他引:5       下载免费PDF全文
用磁控溅射淀积不同富Si程度的掺Er富Si氧化硅薄膜.室温下测量其光致发光谱,观察到各谱中都含有1.54和1.38μm两个发光峰,其中1.54和1.38μm的光致发光峰分别来自Er3+和氧化硅中某种缺陷.系统研究了Er3+1.54μm光致发光峰强度对富Si程度及退火温度的依赖关系.还发现1.54μm发光峰强度与1.38μm发光峰强度相互关联,对此进行了讨论 关键词: Er 富Si氧化硅 光致发光 纳米硅  相似文献   
10.
用磁控溅射淀积掺Er氧化硅、掺Er富硅氧化硅、掺Er氮化硅和掺Er富硅氮化硅薄膜,室温下测量这四种薄膜的光致发光(PL)谱,观察到这四种薄膜都具有1.54μm的峰位,其强度与薄膜的退火温度有关。为了确定1.54μmPL的最佳退火温度,这些薄膜都分别在600,700,800,900,1000,1100℃的温度下同时退火,发现两种富硅薄膜的最佳退火温度是800℃,不富硅的两种薄膜的最佳退火温度是900℃。样品的1.54μmPL最强,且800℃退火的掺Er富硅氧化硅薄膜的1.54μm峰强度是最强的,比不富硅的强了约20倍,还观察到这四种薄膜都具有1.38μm的PL带,且掺Er富硅氧化硅和掺Er富硅氮化硅这两种薄膜的PL在强度上1.38μm峰与1.54μm峰有一定的关系。  相似文献   
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