全文获取类型
收费全文 | 12773篇 |
免费 | 1153篇 |
国内免费 | 558篇 |
专业分类
电工技术 | 432篇 |
综合类 | 599篇 |
化学工业 | 3712篇 |
金属工艺 | 723篇 |
机械仪表 | 277篇 |
建筑科学 | 418篇 |
矿业工程 | 309篇 |
能源动力 | 552篇 |
轻工业 | 1272篇 |
水利工程 | 161篇 |
石油天然气 | 482篇 |
武器工业 | 48篇 |
无线电 | 1073篇 |
一般工业技术 | 2339篇 |
冶金工业 | 1553篇 |
原子能技术 | 170篇 |
自动化技术 | 364篇 |
出版年
2024年 | 403篇 |
2023年 | 527篇 |
2022年 | 484篇 |
2021年 | 631篇 |
2020年 | 583篇 |
2019年 | 566篇 |
2018年 | 449篇 |
2017年 | 545篇 |
2016年 | 547篇 |
2015年 | 434篇 |
2014年 | 649篇 |
2013年 | 721篇 |
2012年 | 721篇 |
2011年 | 773篇 |
2010年 | 508篇 |
2009年 | 563篇 |
2008年 | 440篇 |
2007年 | 582篇 |
2006年 | 615篇 |
2005年 | 521篇 |
2004年 | 443篇 |
2003年 | 406篇 |
2002年 | 327篇 |
2001年 | 309篇 |
2000年 | 242篇 |
1999年 | 220篇 |
1998年 | 200篇 |
1997年 | 151篇 |
1996年 | 136篇 |
1995年 | 126篇 |
1994年 | 107篇 |
1993年 | 95篇 |
1992年 | 96篇 |
1991年 | 74篇 |
1990年 | 47篇 |
1989年 | 37篇 |
1988年 | 36篇 |
1987年 | 16篇 |
1986年 | 26篇 |
1985年 | 23篇 |
1984年 | 25篇 |
1983年 | 12篇 |
1982年 | 8篇 |
1981年 | 7篇 |
1980年 | 7篇 |
1977年 | 6篇 |
1976年 | 6篇 |
1975年 | 8篇 |
1973年 | 3篇 |
1951年 | 12篇 |
排序方式: 共有10000条查询结果,搜索用时 15 毫秒
61.
MBE growth and properties of ZnO on sapphire and SiC substrates 总被引:9,自引:0,他引:9
M. A. L. Johnson Shizuo Fujita W. H. Rowland W. C. Hughes J. W. Cook J. F. Schetzina 《Journal of Electronic Materials》1996,25(5):855-862
Molecular beam epitaxy (MBE) of ZnO on both sapphire and SiC substrates has been demonstrated. ZnO was used as a buffer layer
for the epitaxial growth of GaN. ZnO is a würtzite crystal with a close lattice match (<2% mismatch) to GaN, an energy gap
of 3.3 eV at room temperature, a low predicted conduction band offset to both GaN and SiC, and high electron conductivity.
ZnO is relatively soft compared to the nitride semiconductors and is expected to act as a compliant buffer layer. Inductively
coupled radio frequency plasma sources were used to generate active beams of nitrogen and oxygen for MBE growth. Characterization
of the oxygen plasma by optical emission spectroscopy clearly indicated significant dissociation of O2 into atomic oxygen. Reflected high energy electron diffraction (RHEED) of the ZnO growth surface showed a two-dimensional
growth. ZnO layers had n-type carrier concentration of 9 × 1018 cm−3 with an electron mobility of 260 cm2/V-s. Initial I-V measurements displayed ohmic behavior across the SiC/ZnO and the ZnO/GaN heterointerfaces. RHEED of GaN
growth by MBE on the ZnO buffer layers also exhibited a two-dimensional growth. We have demonstrated the viability of using
ZnO as a buffer layer for the MBE growth of GaN. 相似文献
62.
63.
Copper (titanium) [Cu(Ti)] films with low titanium (Ti) concentration were found to form thin Ti-rich barrier layers at the
film/substrate interfaces after annealing, which is referred to as self-formation of the barrier layers. This Cu(Ti) alloy
was one of the best candidates for interconnect materials used in next-generation ultra-large-scale integrated (ULSI) devices
that require both very thin barrier layers and low-resistance interconnects. In the present paper, in order to investigate
the influences of annealing ambient on resistivity and microstructure of the Cu alloys, the Cu(7.3at.%Ti) films were prepared
on the SiO2 substrates and annealed at 500°C in ultra-high vacuum (UHV) or argon (Ar) with a small amount of impurity oxygen. After annealing
the film at 500°C in UHV, the resistivity was not reduced below 16 μΩ-cm. Intermetallic compounds of Cu4Ti were observed to form in the films and believed to cause the high resistivity. However, after subsequently annealing in
Ar, these compounds were found to decompose to form surface TiO
x
and interfacial barrier layers, and the resistivity was reduced to 3.0 μΩ-cm. The present experiment suggested that oxygen
reactive to titanium during annealing played an important role for both self-formation of the interfacial barrier layers and
reduction of the interconnect resistivity. 相似文献
64.
65.
掺锗CZSi原生晶体中氧的微沉淀 总被引:3,自引:1,他引:3
利用锗硅单晶(锗浓度约为1019cm-3)切制成的籽晶和一般无位错硅单晶生长的缩细颈工艺以及从晶体头部至尾部平稳降低拉速的工艺,生长了直径为60、50和40mm,掺锗量为0.1%和0.5%(锗硅重量比)的锗硅单晶.利用化学腐蚀-金相显微镜法、扫描电子显微镜(SEM)能谱分析和X射线双晶衍射等方法观测了掺锗硅的原生晶体中缺陷及氧的沉淀的状况.发现用CZ法生长的锗硅原生晶体与常规工艺生长的CZSi晶体不同,体内存在着较高密度的氧微沉淀.在晶体尾部,由于锗的分凝使熔体中锗高度富集,出现了"组分过冷"现象,在晶粒间界应力较大处有锗的析出并出现了枝状结晶生长.晶体中高密度氧的微沉淀经过1250℃热处理1h后会溶解消失. 相似文献
66.
A new design concept for diffusion barriers in high‐density memory capacitors is suggested, and both RuTiN (RTN) and RuTiO (RTO) films are proposed as sacrificial oxygen diffusion barriers. The newly developed RTN and RTO barriers show a much lower sheet resistance than various other barriers, including binary and ternary nitrides (reported by others), up to 800 °C, without a large increase in the resistance. For both the Pt/RTN/TiSix/n++poly‐plug/n+ channel layer/Si and the Pt/RTO/RTN/TiSix/n++poly‐plug/n+ channel layer/Si contact structures, contact resistance—the most important electrical parameter for the diffusion barrier in the bottom electrode structure of capacitors—was found to be as low as 5 kohm, even after annealing up to 750 °C. When the RTN film was inserted as a glue layer between the bottom Pt electrode layer and the TiN barrier film in the chemical vapor deposited (Ba,Sr)TiO3 (CVD–BST) simple stack‐type structure, the RTN glue layer was observed to be thermally stable to temperatures 150 °C higher than that to which the TiN glue layer is stable. Moreover, the capacitance of the physical vapor deposited (PVD)–BST simple stack‐type structure adopted TiN glue layer initially degraded after annealing at 500 °C, and, thereafter, completely failed. In the case of the RTN and RTO/RTN glue layers, however, the capacitance continuously increased up to 550 °C. Thus, the new RTN and RTO films, which act as diffusion barriers to oxygen, are very promising materials for achieving high‐density capacitors. 相似文献
67.
对射频放电产生单重态氧进行了实验研究,在不同掺杂物种、不同电极间距、不同稀释配比的情况下,研究了单重态氧相对产率的变化规律,分析了单位氧流量注入能量对单重态氧产率和电效率的影响。实验表明,NO和Hg蒸气的加入,使放电产生单重态氧的相对产率都有显著的提高。随着电极间距的缩小,可以实现高气压工作,放电总压可以达到22.6 kPa,氧气分压超过了4.0 kPa,产率方面也有大幅度提高。单位氧流量注入能量在150~400 J/mmol时,单重态氧产率比较高;电效率较高的区域对应的单位氧流量注入能量在150 J/mmol左右。 相似文献
68.
Electrical conductivity measurements were made on the pyrochlore compounds (Gd1–xCax)2Sn2O7 (x =0, 0.0036, 0.0057, 0.03) as a function of temperature, oxygen partial pressure and Ca doping concentration. An effective Frenkel constant and oxygen vacancy mobility were derived. Intrinsic anion disorder was found to be lower than the expected value based on the relative radii of the cations in the A and B sites (A2B2O7). Low oxygen vacancy mobilities as well as low anion disorder resulted in considerably lower ionic conductivities in GdsSn2O7 relative to the previously studied Gd2(Ti1–xZrx)2O7 system. The temperature and composition dependence of the p-type electronic conductivity were evaluated and the oxidation enthalpy was derived. 相似文献
69.
Single phase SrFe1.2Co0.3Ox sample with layered crystal structure was prepared using a solid state reaction method. Electrical conductivity and apparent oxygen diffusion coefficients of the SrFe1.2Co0.3Ox sample were measured as functions of temperature in atmospheres of various oxygen partial pressures
. Total and ionic conductivities were determined by using the conventional four-probe and electron blocking four-probe methods, respectively. The apparent oxygen diffusion coefficient was derived from the time-dependent conductivity relaxation data of the reequilibrium process after abruptly changing the
in the surrounding atmosphere. Several atmospheres of different
were established by the use of premixed gas cylinders. The conductivity of SrFe1.2Co0.3Ox increases with increasing temperature and
. At 900°C in air, the total conductivity and ionic conductivity are 10 and 8S · cm-2, respectively. The ionic transference number ( 0.8 in air) does not have strong temperature dependence. The activation energy increases with decreasing
. In air, the activation energy has a low value of 0.37 eV. The apparent oxygen diffusion coefficient was
at 950°C over a wide range of
. 相似文献
70.