Mössbauer study of the annealing effect on low‐alloyed steels

Structural analyses of Fe-Cr and Fe-Cr-Ni low‐alloyed steels before and after annealing at 600^○C using Mössbauer spectrometry, X‐ray diffraction and scanning electron microscopy are reported. At the received state, the two steels present a fine bainitic microstructure with equal hardness. From Mössbauer analysis, two iron sites are identified as substitutional by Cr, Mo, Ni atoms and as insertional by carbon in bainitic ferrite. Both sites are locally deformed by residual stresses. The presence of small quantities of retained austenite and ε carbide has been observed. Annealing for one hour at 600^○C causes a decrease in hardness for both steels with a decrease of retained austenite. After longer time of annealing, precipitation of (Fe,Ni)₂₃C₆ occurs in the Fe-Cr-Ni steel and increases hardness.     

基于蛋清栅绝缘层的高性能C_(60)有机场效应晶体管(英文)

采用生物材料(蛋清)作为栅绝缘层制备了基于C60为有源层的有机场效应晶体管。器件展现出了合理的电学特性,场效应迁移率和阈值电压分别为2.59 cm2·V-1·s-1和1.25 V。有机场效应晶体管展现良好性能的原因是蛋清具有较高的介电常数及热退火后形成的光滑表面形貌。实验结果表明,对于制备有机场效应晶体管来说,蛋清是一种有前途的绝缘层材料。     

基于核映射多光谱特征融合的高光谱遥感图像分类法

多光谱遥感图像的波段设定在理论和实践上都极具地物针对性,在更有效的数据挖掘方法帮助下可以提取足够的光谱特征以区分地物,本文将光谱匹配技术用于相似性度量,以提高分类准确度.首先选定光谱角制图、光谱相关制图、Mahalanobis距离、光谱相似度和光谱信息差异做为光谱度量;随后选择高斯核函数,在选定核函数之后,得到了核映射下的光谱特征度量来挖掘高光谱遥感数据的光谱特征.最后采用核映射多光谱特征融合法对多光谱遥感图像光谱特征的相似性进行描述,得到基于核映射多光谱特征融合的高光谱遥感图像分类算法.使用MATLAB中的LIBSVM工具箱对AVIRIS高光谱遥感数据进行分类实验,并与已有算法进行对比,结果表明本文提出的算法具有较高的分类准确度和性能.     

HL-2M偏滤器结构动力学分析

用有限元软件分析了动载荷作用下的偏滤器结构动力学响应。通过对动力学和静力学计算结果的对比,确定载荷的动态放大因子。计算结果表明,所设计的偏滤器结构在瞬态电磁力载荷作用下能满足设计准则的要求。     

HL-2M装置等离子体放电反馈控制系统

通过对HL-2M装置极向场线圈的参数和初始等离子放电控制需求的分析,基于实时采集系统和反射内存实时数据传输的先进控制集成技术,完成了整个HL-2M初始等离子体放电反馈控制系统的设计。新系统实现了稳定的1ms控制周期和实时数据传输,同时解决了实时控制周期和数据传输的延迟。实验结果表明新设计的等离子控制系统能满足初始等离子体极向场线圈电流控制的需求。     

Comparison of radiation degradation induced by x-ray and 3-MeV protons in 65-nm CMOS transistors

The total ionizing dose(TID) response of 65-nm CMOS transistors is studied by 10-ke V x-ray and 3-Me V protons up to 1 Grad(SiO_2) total dose.The degradation levels induced by the two radiation sources are different to some extent.The main reason is the interface dose enhancement due to the thin gate oxide and the low energy photons.The holes' recombination also contributes to the difference.Compared to these two mechanisms,the influence of the dose rate is negligible.     

Magnetic order in LaEuSrCuO studied [2pt] by Fe Mössbauer spectroscopy

⁵⁷Fe M?ssbauer effect studies of La_1.65Eu_0.20Sr_0.15CuO₄ doped with 0.5 at% ⁵⁷Fe performed in the temperature region 300 K > T > 4.2 K give an onset temperature for magnetic ordering of K. This temperature practically is the same as that found in Nd doped La_2-xSr_xCuO₄. It indicates that the magnetic ordering temperature in the LTT phase of rare earth (RE) doped La_2-xSr_xCuO₄ is independent of the RE moment. The direction of the ⁵⁷Fe magnetic moment in the magnetically ordered state is within the CuO₂ plane, while it has been found to be parallel to the c-axis in Nd doped La_2-xSr_xCuO₄. Received: 23 June 1998 / Accepted: 14 July 1998     

Detection of acoustic emission and simultaneous observation of nuclear quadrupole resonance in the α ⇋ β phase transition of paradichlorobenzene

Acoustic emission has been observed in the α ? β transition of monocrystalline samples of paradichlorobenzene. No acoustic emission has been detected in the β → α transition of single crystals nor in the α ? β transitions in polycrystalline samples. The simultaneous observation of acoustic emission and Nuclear Quadrupole Resonance when several α ? β transition cycles are carried out reveals some features of this solid state phase transition.     

Critical behavior of La0.67−y (Sr, Ba, Ca)0.33+y Mn1−x Sn x O3 (x = 0.01, 0.02, y = 0, 0.07) perovskites

The magnetic critical behavior of the manganese perovskite series $ {\text{La}}_{{0.67 - y}} {\left( {{\text{Sr,}}\,\,{\text{Ba,}}\,\,{\text{Ca}}} \right)}_{{0.33 + y}} {\text{Mn}}_{{1 - x}} {\text{Sn}}_{x} {\text{O}}_{3} The magnetic critical behavior of the manganese perovskite series (x = 0.01, 0.02, y = 0, 0.07) is studied by means of dc magnetic measurements and ¹¹⁹Sn M?ssbauer spectroscopy. The structure can be described by a rhombohedral unit cell (space group R–3C) for the samples where the A-site is occupied by La and Sr or La and Ba ions and orthorhombic unit cell (space group Pnma) for the samples where the A-site is occupied by La and Ca ions. Arrott and scaling plots show that the samples, where the A-site is occupied by La and Sr or La and Ba ions, follow the behavior of a conventional second-order ferromagnetic transition. In contrast, the samples that contain La and Ca ions in the A-site show anomalous behavior around Curie point. M?ssbauer measurements show two magnetic phases below T _c. One of them exhibits stronger exchange interactions with more rapid electron transfer between Mn³⁺/Mn⁴⁺, compared to the other.     

Effect of C60 ion sputtering on the compositional depth profiling in XPS for Li(Ni,Co,Mn)O2 electrodes

The performance of a Li-ion cell strongly depends on the solid-electrolyte interface (SEI) on electrodes. The depth distribution of composition in SEI is normally determined by means of X-ray Photoelectron Spectroscopy (XPS) via Ar ion sputtering. Recently, a new kind of ion gun using C60 ions as sputtering source was introduced. In this report, a comparison between the effects of these two kinds of ion guns on the quantification of Li(Ni,Co,Mn)O₂ electrodes was made. It was found that the C60 ion gun is more suitable for analyzing the composition and chemical state of Li(Ni,Co,Mn)O₂ electrode since that it causes lower chemical damage in the superficial layer.