Ni离子注入多晶ZrO2的表面电性能和结构

对氧化钇(Y₂O₃)部分稳定氧化锆(ZrO₂)样品在室温下进行了Ni离子注入(140kev,5×10¹⁵-2×10¹⁷ios/cm²)和热退火处理.应用电学测量,Rutherford背散射技术(RBS),X射线光电子能谱(XPS)和喇曼光谱方法研究了Ni离子注入多晶ZrO₂的表面电性能,注入层结构及其热退火的影响。     

第2系列ZrO2(Y2O3)薄膜的慢正电子研究

用慢正电子技术研究了在溅射时不加偏压,衬底加热300℃,纯Ar气氛下制备的用Y_{2O3稳定的ZrO2薄膜材料(简称YSZ薄膜),发现了YSZ薄膜在不同 深度处的缺陷分布情况,退火温度对YSZ薄膜缺陷有影响.简要讨论了致密、优质YSZ薄膜的 制备方法.}     

Y+SO2反应动力学成像

本文利用时间切片离子速度成像技术、交叉分子束和激光溅射技术研究了高碰撞能下(36 kcal/mol)钇原子与二氧化硫分子的反应动力学. 利用多光子电离在482∽615 nm的波长范围内得到了产物YO的时间切片离子速度成像. YO的切片图像显示其较宽的速度分布和前-后向散射为主的角分布,其中前向散射信号明显强于后向散射. 这种空间分布暗示了该反应通过一个中间体进行,且中间体的寿命不超过一个转动周期. 中间体的形成意味着该氧化反应电子转移机理的发生.     

Fe离子注入多晶Al2O3的光电子能谱研究

本文应用光电子能谱(XPS)方法分析Fe离子注入多晶Al₂O₃样品中各离子的存在状态。通过微机对谱峰进行高斯拟合处理,得出注入离子Fe不同价态的相对含量。 关键词：     

He离子注入ZnO中缺陷形成的慢正电子束研究

在ZnO单晶样品中注入了能量为20—100keV、总剂量为4.4×10¹⁵cm^-2的He离子.利用基于慢正电子束的多普勒展宽测量研究了离子注入产生的缺陷.结果表明，He离子注入ZnO产生了双空位或更大的空位团.在400℃以下退火后，He开始填充到这些空位团里面，造成空位团的有效体积减少.经过400℃以上升温退火后，这些空位团的尺寸开始增大，但由于有少量的He仍然占据在空位团内，因此直到800℃这些空位团仍保持稳定.高于800℃退火后，由于He的脱附，留下的空位团 关键词： 慢正电子束 ZnO 离子注入 缺陷     

非晶纳米发光材料(Y,Eu)2O3-SiO2发射光谱的分析研究

EXAFS测定表明sol-gel方法制备的纳米非晶(Y,Eu)₂O₃-SiO₂发光材料中,发光中心Eu³⁺的局域环境和晶态X₂型Y₂SiO₅Eu中Eu³⁺离子的局域环境相似。以此结构为依据,用M. F. Reid的方案计算了晶场迭加模型中的能级参数及光谱强度参数,并得到了与实验结果基本一致的理论光谱图.     

电子束蒸发法制备ZrO2薄膜的相变模型分析

 用电子束蒸发方法制备了纯的ZrO₂薄膜和含Y₂O₃摩尔分数为7%和13%的ZrO₂薄膜,即YSZ薄膜,通过测定薄膜的损伤阈值来验证温度诱导相变模型;并用X射线衍射（XRD）来测定ZrO₂和YSZ镀膜材料和薄膜的结构特征。结果表明：ZrO₂镀膜材料和薄膜室温下都表现为单斜相,YSZ镀膜材料和薄膜室温下都以立方相存在;YSZ薄膜的损伤阈值远高于ZrO₂薄膜的损伤阈值,这是因为添加Y₂O₃后的YSZ材料的相比较稳定,在蒸发过程中不会发生相变,而ZrO₂材料则发生相变,产生缺陷,缺陷在激光作用下成为吸收中心和初始破坏点,导致ZrO₂薄膜的损伤阈值降低。     

OCS分子在128 nm附近的光解动力学研究：S(3PJ=2,1,0)、S(1D2)以及S(1S0)产物通道

本文利用时间切片离子成像技术对OCS分子进行了真空紫外波段的光解动力学研究. 在四个光解光波长(从129.32到126.08 nm)下测量了硫原子解离产物S(³P_J=2,1,0)、S(¹D₂)、S(¹S₀)的速度影像,并从中清晰地发现了四个主要的解离产物通道：S(³P_J=2,1,0)+CO(X¹Σ⁺),S(³P_J=2,1,0)+CO(A³π),S(¹D₂)+CO(X¹Σ⁺)和S(¹S₀)+CO(X¹Σ⁺). 在实验影像中,产物CO分子的部分振动态结构能够得到分辨. 实验还获取解离产物总平动能谱,产物分支比和角分布. 对实验结果进行分析显示除绝热解离通道S(³P_J=2,1,0)+CO(A³π)之外,在其他三个产物通道中非绝热效应都起到非常重要的作用.     

正磷酸盐晶体Ba3(PO4)2和Sr3(PO4)2高温拉曼光谱研究

测量了碱土金属正磷酸盐Ba₃(PO₄)₂和Sr₃(PO₄)₂常温及高温拉曼光谱, 对拉曼振动模式进行指认, 并分析了晶体拉曼振动光谱及晶体结构在高温下的变化. 在温度升高的过程中, 拉曼振动频率向低频移动且振动峰宽度展宽, 晶体中的P-O平均键长随温度升高而变长, 但O-P-O的键角并未发生变化. 晶体在900 ℃以下无结构相变发生. 关键词： 3(PO₄)₂和Sr₃(PO₄)₂')" href="#">Ba₃(PO₄)₂和Sr₃(PO₄)₂ 高温拉曼光谱 振动模式 高温结构     

紫外波段CH2I2分子的光解离动力学研究

利用离子速度成像方法,研究CH2I2分子在277—305nm范围内若干波长处的光解离动力学.通过同一束激光经(2+1)共振多光子电离(REMPI)过程探测光解碎片I(2P32)和I(2P12),得到了不同激发波长处的离子速度分布图像,从而获得CH2I2光解产物的能量分配和角分布.实验发现,碎片CH2I自由基有很高的内能激发,约占总可资用能的80%,该能量分配可以较好地用冲击模型来解释.实验还发现,产物I(2P32)和I(2P12)具有很不相同的平动能分布,结合所得到的碎片能量分配和角分布,我们对碎片I(2P32)和I(2P12)生成机理进行了分析,指出CH2I2分子电子激发态的绝热和非绝热解离决定了碎片的平动能分布. 关键词： CH2I2 离子速度成像 绝热和非绝热解离     

Etude par spectrometrie Mössbauer (57Fe) de FeMo2S4

We have investigated FeMo₂S₄ by transmission Mössbauer spectroscopy on the ⁵⁷Fe nucleus between 4.2 and 1037 K, using both powdered and single crystal samples.The temperature dependences of the isomer shift and the quadrupole splitting indicate the existence of ferrous ions with well localized 3d electrons. The two different crystallographic Fe sites cannot be separated over the experimental temperature range. The local symmetry of the iron site is lower than axial (η ~ 0.47) and the crystal field splittings Δ₁ and Δ₂ of the Fe²⁺ ? T_2g Orbitals, estimated by the Ingalls' method, are close to 250 and 900 cm^?1.The hyperfine field makes an angle of 14° with the normal on the plane (a, b), deviating a little from the direction of the magnetic moments determined to be perpendicular to (a, b) by neutron diffraction study.At higher temperatures, and more particularly near T_N, a line broadening is observed, and the spectra have to be fitted by a hyperfine field distribution. The broadening comes from the presence of about 7% “abnormal” Fe-sites observed in the paramagnetic spectra, and whose origin is discussed.The Néel temperature was determined to be 112 ± 1 K for the powdered sample and 106 ± l K for the single crystal.     

57Fe M?SSBAUER STUDY ON (NdDy)TiFe11Ny COMPOUNDS

⁵⁷Fe M?ssbauer spectra have been obtained at room temperature for (NdDy)TiFe₁₁, and at 11 K and room temperature for the corresponding nitrides (NdDy)TiFe₁₁N_y. The magnetic behaviors of Fe atoms at different sites have been studied. We have found a larger increase of the hyperfine fields upon nitrogenation due to the higher nitrogen content in these compounds and got a bigger enhancement of the isomer shift in 8j site because of the nearest nitrogen environment.     

57Fe Mössbauer effect evidence for magnetostriction in UFe2

Temperature dependent ⁵⁷Fe Mössbauer experiments on UFe₂ have shown that above T_c (158 K) the logarithm of the reoil-free fraction is a linear function of temperature, with θ_M = 325 K. Below T_c there is a non-linear increase in z.hsl which is interpreted in terms of a reduction in the mean square amplitude of the iron atom motion associated with magnetostriction of the unit cell.     

Resonances in the reaction 56Fe(p, γ)57Co

Resonances in the reaction ⁵⁶Fe(p, γ)⁵⁷Co have been surveyed over the energy range 1.2 ? E_p ? 1.5 MeV wherein the analogues of the ground state $\text{(J}{}^{\mathrm{\pi }}\text{=}\text{1}\text{2}{}^{\mathrm{?}}\text{, 0.014}\text{MeV}$ state $\text{(J}{}^{\mathrm{\pi }}\text{=}\text{3}\text{2}{}^{\mathrm{?}}\text{)}$ and 0.136 MeV state $\text{(J}{}^{\mathrm{\pi }}\text{=}\text{5}\text{2}{}^{\mathrm{?}}\text{)}$ of ⁵⁷Fe are expected to occur. Gamma-ray angular distributions have been used to establish resonance and bound-state spins, and decay schemes have been determined. The analogue resonances appear to be severely fragmented, however the density of resonances of a given spin correlates quite well with (³He, d) results and with the expected analogue-state positions.     

SrTb2Fe2O7 studied by mössbauer spectra of 57Fe

The temperature dependence of the hyperfine parameters of ⁵⁷Fe in SrTb₂Fe₂O₇ gave a magnetic ordering temperature T_N=542 K, saturation effective magnetic fieldH_eff(0)=552 kGand Debye temperature θ_D=330 K. The princip al axis of the PFG tensorV_zzis angled at 9° to the crystallographic c axis. Mössbauer spectra at 4.2 K reveal reorientation of iron spin.     

A 57Fe and 119Sn Mössbauer study of BaFe4Sn2O11

The Mössbauer spectrum of BaFe₄Sn₂O₁₁ has been recorded for both ⁵⁷Fe and ¹¹⁹Sn isotopes at a variety of temperatures. In the paramagnetic state the ⁵⁷Fe spectra are interpreted in terms of three iron environments. Magnetic ordering begins at 77 K and is virtually complete by 4.2 K to give an average magnetic hyperfine field of 504 kG. The ¹¹⁹Sn spectra also reflect the magnetic ordering and a magnetic hyperfine field of 45 kG is transferred to the tin nuclei.     

Structure of 57Fe studied with 56Fe(d, p)57Fe reactions

${}^{56}\text{Fe}\text{(}\text{d}\text{, p}\text{)}{}^{57}\text{Fe}$ reactions have been studied with 10 MeV vector polarized deuterons over the angular range 15° ≦ θ_p ≦ 80°. Angular distributions of the vector analysing power and the differential cross section have been measured for reactions leading to levels in ⁵⁷Fe. Distorted wave Born approximation calculations are compared to the measurements. The observed j-dependence of the vector analysing power results in eighteen new spin-parity assignments for levels in ⁵⁷Fe. Spectroscopic factors are extracted from the differential cross-section measurements. The results are compared to the predictions of the single-particle shell model and to models including collective structure.