全文获取类型
收费全文 | 226篇 |
免费 | 30篇 |
国内免费 | 25篇 |
专业分类
电工技术 | 3篇 |
综合类 | 11篇 |
化学工业 | 46篇 |
金属工艺 | 18篇 |
机械仪表 | 3篇 |
建筑科学 | 1篇 |
矿业工程 | 1篇 |
轻工业 | 1篇 |
武器工业 | 1篇 |
无线电 | 57篇 |
一般工业技术 | 127篇 |
冶金工业 | 9篇 |
原子能技术 | 1篇 |
自动化技术 | 2篇 |
出版年
2024年 | 1篇 |
2023年 | 12篇 |
2022年 | 5篇 |
2021年 | 9篇 |
2020年 | 12篇 |
2019年 | 14篇 |
2018年 | 7篇 |
2017年 | 19篇 |
2016年 | 13篇 |
2015年 | 8篇 |
2014年 | 21篇 |
2013年 | 14篇 |
2012年 | 11篇 |
2011年 | 14篇 |
2010年 | 16篇 |
2009年 | 9篇 |
2008年 | 12篇 |
2007年 | 15篇 |
2006年 | 7篇 |
2005年 | 10篇 |
2004年 | 8篇 |
2003年 | 18篇 |
2002年 | 3篇 |
2001年 | 9篇 |
2000年 | 3篇 |
1999年 | 1篇 |
1998年 | 2篇 |
1997年 | 3篇 |
1995年 | 2篇 |
1994年 | 1篇 |
1993年 | 1篇 |
1985年 | 1篇 |
排序方式: 共有281条查询结果,搜索用时 0 毫秒
81.
N. Balchev K. Nenkov B. Kunev J. Pirov M. Baychev A. Souleva 《Journal of Superconductivity》2004,17(3):363-367
A new Mn-containing material with nominal composition L0.5Sr0.5Mn0.5M0.5O3 (L = Y or Pr; M = Cu or Ru), as well as Y0.5Sr0.5MnO3 for comparison, were synthesized. The results of the XRD and EDX analyses show that the obtained samples are single-phased and isostructural, with L1–xAxMnO3. The L0.5Sr0.5Mn0.5Cu0.5O3 material displays a PM behavior down to 8 K where paramagnetic–antiferromagnetic transition begins. The Pr0.5Sr0.5Mn0.5Cu0.5O3 sample has a broad transition at 210 K and a magnetoresistance of 34% at 128 K. The Pr0.5Sr0.5Mn0.5Ru0.5O3 material has a paramagnetic–ferromagnetic transition beginning at 330 K and a ferromagnetic–antiferromagnetic one at about 160 K. The obtained value of T
c is the highest for the Pr-containing manganites. The roles of Pr/Sr ratio, anisotropy, and intergranular effects in the samples are discussed. 相似文献
82.
未掺杂氧化锆薄膜的铁磁性研究
宁帅,张政军(清华大学材料学院)
创新点说明:1,通过不同的物理气相沉积方法,实现了对未掺杂氧化锆薄膜的物相调控;2,发现了未掺杂氧化锆薄膜室温铁磁性对物相结构的依赖性;3,通过缺陷分析表征,发现四方相氧化锆的室温铁磁性主要由氧空位缺陷调控。
目的:未掺杂氧化锆薄膜的制备、物相和缺陷调控以及室温铁磁性研究。
方法:脉冲电子束沉积、直流反应磁控溅射、电子束蒸镀。
结果:1,通过不同的物理气相沉积方法,实现了未掺杂氧化锆薄膜的物相调控;2,发现了未掺杂氧化锆薄膜室温铁磁性的物相依赖性;3,通过缺陷分析表征,发现四方相氧化锆的室温铁磁性主要由氧空位缺陷调控。
结论: 1,制备了不同物相结构的未掺杂的氧化锆薄膜;2,发现了四方相氧化锆薄膜可以在室温下呈现铁磁性;3,四方相氧化锆薄膜中的室温铁磁性主要由氧空位缺陷引起。
关键词:氧化锆薄膜,物相调控,室温铁磁性,氧空位缺陷
相似文献83.
N. Kim J. W. Kim S. J. Lee Y. Shon T. W. Kang G. Ihm T. F. George 《Journal of Superconductivity》2005,18(2):189-193
We investigate magnetic properties of In1–xMnxP and Ga1–xMnxN quantum wells in the mean-field approximation and show the difference between them. In the case of the In1–xMnxP, the dependence of the Curie temperature (Tc) on the hole density exhibits a step-like behavior, reflecting the effect of a two-dimensional Fermi (hole) gas, when the hole–hole exchange interaction is ignored. When we take into account the hole–hole exchange interaction, however, this behavior is broken by the appearance of peaks at the specific two-dimensional carrier densities, and Tc is substantially enhanced in this region. In the case of Ga1–xMnxN, the step-like behavior is obscure, and it appears that Tc increases rather continuously with the increasing two-dimensional (2D) carrier density. This shows very weak step-like behavior compared to other III-Mn-V DMS quantum wells, because the hole effective mass of Ga1–xMnxN is very large, and the large hole effective mass reduces the energy splitting due to the confinement effect. In a multi-heavy-valence-subband model, the Curie temperature of the In1–xMnxP quantum well is about 68 K with 6.5×1012 holes per cm2 and the Mn mole fraction x = 0.05 and the exchange constant Jpd = 0.15 eV nm3. The Curie temperature of the p-type Ga1–xMnxN quantum well can be above room temperature, unless the spin-exchange interaction integral is abnormally small. 相似文献
84.
具有室温铁磁性能的Cr掺杂CdS纳米棒用简单的溶剂热法被成功地合成。X-射线衍射(XRD)分析表明产物为六方相CdS。 透射电镜(TEM)分析表明,不同铬含量的CdS均为纳米棒,CdS纳米棒长为100-350 nm,平均直径为20-30 nm,几乎与掺入铬的质量无关。 能量色散谱(EDS)测试表明,合成产物由S、Cd和Cr组成。振动样品磁强计(VSM)表明,Cr掺杂CdS纳米棒在室温下具有铁磁性,而没有Cr掺杂CdS纳米棒具有弱铁磁性。Cr掺杂CdS纳米棒(Cr = 4.17 at%,7.31 at%)的饱和磁化强度Ms分别约为3.907和8.798(10-3 emu/g),Hc的矫顽力约为96.21和 137.15 Oe。 CdS纳米棒室温铁磁性能的产生与CdS晶格中Cd原子被Cr的取代有着密切关系。 相似文献
85.
Moon-Ho Ham Min-Chang Jeong Woo-Young Lee Jae-Min Myoung Jeung-Mi Lee Joon-Yeon Chang Suk-Hee Han 《Journal of Electronic Materials》2004,33(2):114-117
We present the magnetic and magnetotransport properties of epitaxial (Ga,Mn)N films with nominal Mn concentration (x=0.1–0.73%)
grown by plasma-enhanced molecular beam epitaxy (PEMBE). X-ray diffraction (XRD) reveals that (Ga,Mn)N has the single-phase
wurtzite structure without secondary phases. The epitaxial (Ga,Mn)N films were found to exhibit n-type conductivity, ferromagnetic
ordering with Curie temperature in the range 550–700 K, and in-plane magnetic anisotropy. The negative magnetoresistance (MR)
was observed at temperatures below 50 K and was found to gradually increase with decreasing temperature. 相似文献
86.
Li Binbin Zhang Rong Xiu Xiangqian Tao Zhikuo Chen Lin Xie Zili Zheng Youdou Yu Huiqiang 《中国稀土学报(英文版)》2006,24(Z1)
The magnetic and structural properties of 2% Ni-doped ZnO powers prepared by sol-gel method were studied. X-ray diffraction (XRD) and high resolution transmission electron microscopy (HRTEM) of the sample do not show existence of any signal of second phase. The X-photoelectron spectroscopy (XPS) of the sample shows the chemical valence of Ni is 2 and the real Ni concentration is 2.19% determined by X-ray fluorescence spectra (XRFS). The magnetic property performed with superconducting quantum interference device (SQUID) shows that the sample exhibits ferromagnetism above room temperature and the Curie temperature (TC) is about 600 K. 相似文献
87.
An effect of alloying two ferromagnetic semiconductors (In,Mn)As and (Ga,Mn)As on the ferromagnetic properties of resultant (In,Ga,Mn)As alloys is reported. For conditions close to lattice-matching to InP substrates, y = 0.53 in (In
y
Ga1–y
)1–x
Mn
x
As, ferromagnetism up to Curie temperatures T
C = 100–110 K could be achieved for a Mn composition x = 0.13. Trends in the Curie temperature in (In,Ga,Mn)As are compared with (Ga,Mn)As and (In,Mn)As as a function of Mn content. Hole concentrations determined from magnetotransport, taking into account the anomalous Hall contribution to Hall resistance, gives p/Mn = 0.03 ratio to Mn composition in metallic case for x = 0.13. We mention the possible role of chemical ordering (short range) of Mn impurity atoms on hole concentration and, consequently, for the ferromagnetic properties. 相似文献
88.
具有宽过冷液相区的Fe63Co7NbxZr10-xB20非晶态合金的热稳定性和磁性研究 总被引:1,自引:0,他引:1
利用单辊急冷法制备出厚约35μm宽5mm的 Fe63Co7NbxZr10-xB20条带,并研究了合金的热稳定性、非晶结构和磁性能.结果表明,含4at%Nb的Fe63Co7Nb4Zr6B20合金过冷液相区Δ Tx最宽,达到79K.合金系的饱和比磁化强度σs随着Nb含量的增加而线性减小.合金系经973K退火900s,由于α\|Fe等相的析出,使得合金的σs和Hc均迅速升高. 相似文献
89.
90.
Jiye Fang John Wang Leong-Ming Gan Ser-Choon Ng Jun Ding Xiangyuan Liu 《Journal of the American Ceramic Society》2000,83(5):1049-1055
A fine strontium ferrite powder with high coercivity was successfully prepared by forming hydroxide precursor particles in the continuous ethanol-based phase of a microemulsion consisting of iso-octane, NP9, and an ethanol solution containing Sr2+ and Fe3+ cations at a molar ratio of 1:12. The microemulsion-derived hydroxide precursor was calcined at various temperatures, ranging from 600° to 1100°C, to develop the hexagonal strontium ferrite phase. X-ray diffractometry and infrared characterizations revealed that the formation mechanisms of strontium ferrite in the microemulsion-derived precursor differed from those of the precursor derived by conventional coprecipitation. The microemulsion resulted in a strontium ferrite of finer particle size and better magnetic properties than those of the conventionally coprecipitated strontium ferrite. The microemulsion-derived strontium ferrite exhibited an intrinsic coercivity of 6195 Oe and a saturation magnetization of 58.28 emu/g when calcined at 900o C. The saturation magnetization increased further, to 69.75 emu/g, when the microemulsion-derived precursor was calcined at 1100o C. 相似文献