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1.
Dan Phuong Nguyen Se-Young O Chan-Woo Park Keesam Shin Chan-Gyu Lee Toshitada Shimozaki Takahisa Okino 《Journal of magnetism and magnetic materials》2008,320(14):e264-e267
[Fe(0.5 nm)/Pt(0.5 nm)]40, [Fe(1 nm)/Pt(1.5 nm)]20 and [Fe(3 nm)/Pt(3 nm)]10 multilayer were prepared by DC magnetron sputtering. By conventional furnace annealing (CA) at 270–600 °C for various time, all of the films still remained the disordered structure with the soft magnetic phase. By rapid thermal annealing (RTA) at 500 °C for various time, we obtained the [Fe(1 nm)/Pt(1.5 nm)]20 and [Fe(3 nm)/Pt(3 nm)]10 films with L12 ordered FePt3 phase which was almost ferromagnetic at room temperature. However, the [Fe(0.5 nm)/Pt(0.5 nm)]40 films was still disordered state even under RTA. Compared with CA, RTA exposed an outstanding effect on accelerating the phase transition when the film thickness is over [Fe(0.5 nm)/Pt(0.5 nm)]40. 相似文献
2.
本文用X射线粉末法测定了Li2K(IO3)3与Li2NH4(IO3)3的晶体结构和原子参数。发现Li3K(IO3)3,Li2NH4(IO3)3与Li2Rb(IO3)3同晶型,属单斜晶系,空间群为P21/α,每个单胞含有四个化合式量。室温的点阵常数分别为α=11.198?,b=11.046?,c=8.254?,β=111.53°,及α=11.327?,b=11.078?,c=8.341?,β=111.87°。讨论了二元化合物的形成与离子半径的关系。
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3.
应用不对称2DNOESHY实验方法研究了顺铂配合物Cis-Pt (NH3)2(Guo)2Cl2的水溶液中的构象,表明鸟苷同铂配合后其糖环构象发生明显的变化。 相似文献
4.
反式二氯二L-苯丙氨酸乙酯合铂[Pt(C11H15NO2)2Cl2]属单斜晶系,空间群为P21,α=13.555(6)?,b=6.487(3)?,c=15.588(5)?,β=109.42(3)°,Z=2。该化合物晶体结构由重原子法求解,用块矩阵最小二乘方法修正,R=0.0617,Rw=0.0575。Pt—N 2.065(14)?,2.084(14)?;Pt—Cl 2.285(7)?,2.312(8)?。结构由以N—H……O氢键联结的分子层交错堆积组成。
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5.
通过含新结构单元钴化合物:Co3(bdt)3(PBu3)3(Ⅰ),Co3(tdt)3(PBu3)3(Ⅱ),[Co3(bdt)3(PPh3)3][CoBr3(dmf)](Ⅲ)和[Co3(edt)3(PEtB)3]2[Co2Cl4(Et2SO2)2](Ⅳ)(bdt=1,2-S2C6H42-,tdt=4-Me-1,2-S2C6H32-,edt=SCH2CH2S2-)的磁极矩和1H NMR等研究表明:它们均具顺磁性,钴原子之间存在着反铁磁偶合作用,同时还讨论了它们的磁学性质和分子结构之间关系。 相似文献
6.
本文用差热分析、高温和室温X射线衍射分析等方法研究了Mg(IO3)2·4H2O的相变过程: Mg(IO3)2·4H2O晶体属单斜晶系,空间群为P2或Pm,每个晶胞含有两个化合式量,点阵常数为a=8.307?,b=6.627?,c=8.541?,β=1.00°45′。我们用X射线粉末法测定了α-Mg(IO3)2的晶体结构。α-Mg(IO3)2属六角晶系,其空间群是P63。在14℃的点阵参数为a=5.4777?,c=5.1282?,c/a=0.9362。每个单胞含一个化合式量,6OII占据在6(c)等效位置上,21V占据在2(b)等效位置上,Mg++无序地占据着2(a)等效位置的一半。其原子参数为xc=0.096,yc=0.344,zc=0.162,zb=0,za=0.981。从结构来看,它与α-LiIO3同晶型,所不同的是2(a)位置只有一半被Mg++离子占据着,另一半为空位。
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7.
系统研究了核磁共振碳谱与化学位移和规律,以及分子拓扑指数在定量[结]构[波]谱关系(QSSR)中的应用.本文基于矢量路径长度矢量p=(P1, P2, P3,…, Pm)与分子中原子相互作用,提出了一种新型分子距边矢量并发现它与烷烃13C NMR 化学位移和有良好线性相关性, 回归方程及其统计参数为:
CSS=bν+p3=Σmj=0bjνj+b10p3=b0ν+b1ν1+b2ν2+b3ν3+b4ν4+b5ν5+b6ν6+b7ν7+b8ν8+b9ν9ν+b10P3 =-13.6011+22.2133 ν1+28.4121 ν2+25.9416 ν3+26.6709 ν4+14.4976 ν5+5.7240 ν6-5.3830 ν7-3.2152 ν8-15.0213 ν9-25.7099 ν10+12.2786P3 (n=63, R=0.9970, EV=99.68%, RMS=3.7348, F=2418.2; 交互校验CV为: R=0.9893, EV=98.83%, RMS=7.1261, F=664.046); 结果良好. 相似文献
8.
为了得到准确的In2O3晶体电子结构, 本文分别采用GGA, GGA+U, HSE06的方法计算了电子结构, 并进行了G0W0修正, 通过比较计算结果, 得到HSE06+G0W0方法计算得到的禁带宽带最接近实验结果. 在此基础上使用Hedin的G0W0近似方法和Bethe-Salpeter方程计算得到了In2O3晶体的光学性质, 计算结果与实验结果吻合很好, 在此基础上通过对准粒子能带结构、光学跃迁矩阵和光学吸收谱的分析, 给出了In2O3晶体的光学跃迁机理. 相似文献
9.
The magnetic susceptibility of (IPA)2FeCl4, (IBuA)2FeCl4 and (IPA)2CuCl4, where IPA = (CH3)2CHNH+3 and IBuA = (CH3)2CHCH2NH+3, were measured in the temperature range form 80 K up to a temperature near the melting points of the samples. The results obtained were interpreted in termw of a canted two-dimensional antiferromagnet. The variation of the magnetic susceptibility with the change in the composition was also discussed. 相似文献
10.
Susumu Nakayama Yoshikatsu Higuchi Yuki Kondo Masatomi Sakamoto 《Solid State Ionics》2004,170(3-4):219-223
A series of apatite-type La–Ge–O ceramics were prepared and their cation-defect at the 4f+6h sites and oxide ion-defect at 2a site were investigated. In LaxGe6O12+1.5x ceramics of x=6–12, the higher conductivities were obtained in the region of apatite composition, Lax(GeO4)6O1.5x−12 (x=8–9.33), and the highest conductivity was achieved for La9(GeO4)6O1.5 (x=9), where the number of cation (La3+) occupying the 4f+6h sites is 9 and the number of oxide ion occupying the 2a site is 1.5. The ceramics with cation- and oxide ion-defects were La9−0.66xSrx(GeO4)6O1.5 (x=0–1), La9−1.33xZrx(GeO4)6O1.5 (x=0–1), La9−xSrx(GeO4)6O1.5−0.5x (x=0–3), La9−xZrx(GeO4)6O1.5+0.5x (x=0–1), Lax(GeO4)3x−21(AsO4)27−3xO1.5 (x=0–3), Lax(GeO4)33−3x(AlO4)3x−27O1.5 (x=0–3), La9(GeO4)6−x (AlO4)xO1.5−0.5x (x=0–3), La9(GeO4)6−x(AsO4)xO1.5+0.5x (x=0–1), La9.33−xSrx(GeO4)6O2−0.5x (x=0–1.2) and Lax(GeO4)4.5(AlO4)1.5O1.5x−12.75 (x=8.8–9.83), which were prepared by the partial substitution of La3+and GeO44−of the basic apatite La9(GeO4)6O1.5 with Sr2+ or Zr4+ and AlO45− or AsO43−. Such substitutions lowered the conductivity of La9(GeO4)6O1.5. These results were discussed by the electrostatic interaction between Sr2+, Zr4+, AlO45− or AsO43− and oxide ion as a conductive species. 相似文献
11.
采用高温固相反应合成了NaZnLa(PO4)2中掺杂Ce3+、Tb3+的荧光体,对其晶体结构、发光行为进行了研究,并尝试对NaZnLa(PO4)2:Ce,Tb荧光体进行调制。NaZnLa(PO4)2是LaPO4的同构物,为单斜晶系独居石结构,从XRD谱数据得到NaZnLa(PO4)2基质的晶胞参数为a=0.6823nm,b=0.7045nm,c=0.6497nm,β=1039°,v=0.303nm3,其晶胞参数与单斜LaPO4的晶胞参数相似。在NaZnLa(PO4)2:Ce,Tb荧光体中,Ce3+对Tb3+有良好的敏化作用,掺杂适量的BO33-、Al3+、Dy3+,可以增强发光亮度。 相似文献
12.
Anomalies are found in the near-band-edge luminescence properties of Δ2-light-hole indirect excitons in Si1−yCy-based tensilely strained quantum wells (QWs). The experimental spectra exhibit a clear signature of phonon-assisted transitions on the lower energy side of the “no-phonon” transition, which indicates the relevance of “virtual” indirect valleys and in-plane k-dispersion, as opposed to the theoretical prediction that the zone-centered Δ2 valleys take over the conduction band edge. Intervalley scattering between [0 0 1]-Δ2 valleys and in-plane Δ4 valleys is suggested as the underlying mechanism. On the other hand, the experimental evidence was found for “apparently enhanced” quantum-confined Stark red shifts for Si1−yCy-based QWs. However, quantitative estimates are in conflict with the experimental results and predict a blue shift due to exciton weakening which masks the Stark effect as in the case of Δ4-heavy hole excitons in Si1−xGex-based QWs. 相似文献
13.
14.
H. M. Luo B. Qu Z. Y. Chen Y. T. Qian W. C. Yu 《Physica C: Superconductivity and its Applications》1996,270(3-4):249-252
New Pb based layered superconducting cuprates (Pb0.5Cd0.5)(Sr0.9R0.1)2(R′0.7Ce0.3)2Cu2Oy with (R,R′) = (Eu,Gd), (Eu,Dy) and (Nd,Gd), have been successfully synthesized. The structure of (Pb,Cd)(Sr,Eu)2(Gd,Ce)2Cu2Oy is determined using XRD data. The X-ray powder diffraction pattern can be indexed by the tetragonal structure with lattice parameters a = 3.8250 Å, C = 29.2235 Å and a space group of I4/mmm. The effects of synthesis conditions on (Pb,Cd)(Sr,Eu)2(Gd,Ce)2Cu2Oy are studied and a Tc(onset) of 26 K is obtained by resistance measurements. It is isostructural to the superconductor (Pb,Cu)(Sr,Eu)2(Eu,Ce)2Cu2Oy. 相似文献
15.
By the concept of effective boson numbers, systematics of E21+E41+E61+, R=E21+/E41, B(E2, 01+→21+) and Q0 for even-even nuclei with A≥70 are presented. New features of energy spectra are noticed and an intuitive understanding is given. 相似文献
16.
B. Bozzini D. De Vita A. Sportoletti G. Zangari P.L. Cavallotti E. Terrenzio 《Journal of magnetism and magnetic materials》1993,120(1-3):300-304
ew baths for Co-Pt electrodeposition have been developed and developed and ECD thin films (≤0.3μm) have been prepared and characterized structurally (XRD), morphologically (SEM), chemically (EDS) and magnetically (VSM); their improved corrosion, oxidation and wear resistance have been ascertained. Such alloys appear suitable candidates for magnetic storage systems, from all technological viewpoints. The originally formulated baths contain Co-NH3-citrate complexes and Pt-p salt (Pt(NH3)2(NO2)2). Co-Pt thin films of fcc structure are deposited obtaining microcrystallites of definite composition. At Pt 30 at% we obtain fcc films with a=0.369 nm, HC=80 kA m, and high squareness; increasing Co and decreasing Pt content in the bath it is possible to reduce the Pt content of the deposit, obtaining fcc structures containing two types of microcrystals with a = 0.3615 nm and a = 0.369 nm deposited simultaneously. NaH2PO2 additions to the bath have a stabilizing influence on the fcc structure of a = 0.3615 nm, Pt 20 at% and HC as high as 200 kA/m, with hysteresis loops suitable for both longitudinal or perpendicular recording, depending on the thickness. We have prepared 2.5 in. hard disks for magnetic recording with ECD Co-Pt 20 at% with a polished and texturized ACD Ni-P underlayer. Pulse response, 1F & 2F frequency and frequency sweep response behaviour, as well as noise and overwrite characteristics have been measured for both our disks and high-standard sputtered Co-Cr-Ta production disks, showin improved D50 for Co-Pt ECD disks. The signal-to-noise ratio could be improved by pulse electrodeposition and etching post-treatments. 相似文献
17.
在化学计量的熔料里,用提拉法生长了K5Bi0.9Er0.1(MoO4)4单晶。该晶体属于三方晶系,空间群为R3m,z=1.5,晶胞参数为a=6.029?,c=20.823?(六方表示)。晶体具有层状结构,沿着(0001)面容易解理。晶体在室温下的吸收光谱包括有若干条吸收带,它们是稀土离子所特有的。其中三个主要的吸收峰分别相当于从Er3+离子的基态 4I15/2向 4G11/2, 2H11/2和 4I13/2能级的跃迁。本文还给出晶体中相当于 4I13/2→ 4I15/2跃迁的荧光发射光谱。
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18.
在不同pH条件下以N-烷基亚胺二乙酸[R-N (CH2COOH)2,R=Me,i-Pr,n-Pr,HO-Et]为配体合成了一系列二氨铂(Ⅱ)类配合物.13C NMR (20MHz)研究结果表明该类配体均以N、O与铂配位,配位方式不随合成时pH值的改变而改变,在弱酸条件下,配合物处于交换平衡状态,平衡常数由不同pH下未配位羧基碳的化学位移计算而得. 相似文献
19.
采用高温固相法合成了荧光体Ba10(PO4)4(SiO4)2:Ce3+和Ba10(PO4)4(SiO4)2:Eu2+,研究了两种荧光体的光谱特性。结果表明,两者都呈现较强的宽带激发特征。根据同种基质中Eu2+和Ce3+两种离子光谱特征的相关性,通过测得的Ba10(PO4)2(SiO4)2基质中Ce3+的光谱数据估算了Ba10(PO4)2(SiO4)2:Eu2+中Eu2+的斯托克斯位移(ΔS)和激发能量,估算结果与Ba10(PO4)2(SiO4)2:Eu2+样品的光谱分析结果十分吻合。Ba10(PO4)2(SiO4)2:Eu2+可以同时被紫光和蓝光激发,发出偏白的绿光,可用作白光LED的荧光粉。 相似文献