全文获取类型
收费全文 | 30284篇 |
免费 | 3569篇 |
国内免费 | 3306篇 |
专业分类
化学 | 13459篇 |
晶体学 | 308篇 |
力学 | 1101篇 |
综合类 | 162篇 |
数学 | 2016篇 |
物理学 | 7099篇 |
综合类 | 13014篇 |
出版年
2024年 | 150篇 |
2023年 | 479篇 |
2022年 | 911篇 |
2021年 | 960篇 |
2020年 | 961篇 |
2019年 | 885篇 |
2018年 | 843篇 |
2017年 | 842篇 |
2016年 | 1028篇 |
2015年 | 1287篇 |
2014年 | 1727篇 |
2013年 | 2026篇 |
2012年 | 2275篇 |
2011年 | 2377篇 |
2010年 | 1954篇 |
2009年 | 1828篇 |
2008年 | 2103篇 |
2007年 | 1944篇 |
2006年 | 1726篇 |
2005年 | 1514篇 |
2004年 | 1169篇 |
2003年 | 896篇 |
2002年 | 921篇 |
2001年 | 807篇 |
2000年 | 772篇 |
1999年 | 688篇 |
1998年 | 542篇 |
1997年 | 492篇 |
1996年 | 423篇 |
1995年 | 409篇 |
1994年 | 416篇 |
1993年 | 290篇 |
1992年 | 283篇 |
1991年 | 250篇 |
1990年 | 219篇 |
1989年 | 206篇 |
1988年 | 138篇 |
1987年 | 105篇 |
1986年 | 76篇 |
1985年 | 45篇 |
1984年 | 32篇 |
1983年 | 18篇 |
1982年 | 22篇 |
1981年 | 12篇 |
1980年 | 22篇 |
1979年 | 10篇 |
1976年 | 13篇 |
1975年 | 9篇 |
1974年 | 8篇 |
1973年 | 7篇 |
排序方式: 共有10000条查询结果,搜索用时 12 毫秒
1.
在图像相关位移测量方法中一般采用正方型子区搜索中心点的位移.当测量靠近裂纹或缺陷部位的位移时中心型子区失去效果,为了解决这一问题提出了非中心型子区的方法.证明了方法的有效性.认为在相关搜索时测量点既可选定在子区的中心位置,也可选定在非中心位置.进而提出了将测量点确定在子区角点的多种子区的方法.除通常的中心型子区外,至少还有4种子区可以采用,分别是右下角型、左下角型、右上角型和左上角型,这4种子区不但适用于表面裂纹或缺陷部位的位移测量,而且增加了图像有效信息的提取面积. 相似文献
2.
3.
4.
5.
6.
J. Song H. Jiang Z.J. Liu D.Y. Khang Y. Huang J.A. Rogers C. Lu C.G. Koh 《International Journal of Solids and Structures》2008,45(10):3107-3121
A finite-deformation theory is developed to study the mechanics of thin buckled films on compliant substrates. Perturbation analysis is performed for this highly nonlinear system to obtain the analytical solution. The results agree well with experiments and finite element analysis in wavelength and amplitude. In particular, it is found that the wavelength depends on the strain. Based on the accurate wavelength and amplitude, the membrane and peak strains in thin films, and stretchability and compressibility of the system are also obtained analytically. 相似文献
7.
Zhaoqiang Lu Lin Cheng Jun Li Kai Zhang Song Yi Jingui Qin 《Journal of polymer science. Part A, Polymer chemistry》2004,42(4):925-932
The synthesis and structural characterization of a series of novel, fluorinated poly(phthalazinone ether)s containing perfluorophenylene moieties are described. The monomers, 4‐(4′‐hydroxyaryl)phthalazin‐1(2H)‐ones ( 2a – 2d ), were conveniently and efficiently synthesized from phenols and phthalic anhydride in two steps via 2‐(4′‐hydroxybenzoyl)benzoic acids, which were first obtained by the Friedel–Crafts reaction in good yields and with high stereoselectivity and were then converted into 2a – 2d by fusion with hydrazine. All the polymers were prepared by nucleophilic aromatic substitution (SNAr) polycondensation between the compounds perfluorobiphenyl and 4‐(4′‐hydroxyaryl)phthalazin‐1(2H)‐ones ( 2a ‐ 2d ). The resulting fluorinated polymers were readily soluble in common organic solvents (e.g., CHCl3, tetrahydrofuran, dimethylformamide, dimethyl sulfoxide, N‐methylpyrrolidone, etc.) at room temperature. Their weight‐average molecular weights and the polydispersities ranged from (7.96–18.25) × 103 to 1.31–2.71, respectively. Their glass‐transition temperatures varied from 213 to 263 °C. They were all stable up to 390 °C both in air and in argon. The 5% weight‐loss temperatures of these polymers in air and argon ranged from 393–487 to 437–509 °C, respectively. Wide‐angle X‐ray diffraction studies indicated they were all amorphous and could be attributed to the presence of kink nonplanar moiety, phenyl phthalazinone along the polymer backbone. © 2004 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 42: 925–932, 2004 相似文献
8.
The reversible nonlinear conduction (RNC) in of high‐density polyethylene/acetylene carbon black composites with different degrees of crosslinking was studied above room temperature and below the melting point of high‐density polyethylene (HDPE). The experimental current density‐electric field strength curves can be overlapped onto a master curve, suggesting that the microscopic mechanisms for the appearance of RNC exist regardless of the ambient temperature and the crosslinking degree of the HDPE matrix. The relationship between the crossover current density and the linear conductivity can be explained in the framework of the dynamic random‐resistor‐network model. According to these results, two electron‐tunneling models are suggested to interpret the microscopic conduction behavior. © 2004 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 42: 1212–1217, 2004 相似文献
9.
本文研究了FZ与CZ硅中铜与电子辐照缺陷的相互作用.实验表明,这种作用使扩铜并经电子辐照的n型FZ硅出现两个未经报道的新的深中心,E(0.043)和E(0.396).前者只存在于FZ硅而不存在于CZ硅.后者在扩铜并经电子辐照的n型FZ和CZ硅中都存在.电子辐照再加适当温度的热处理还可电激活硅中的铜,另外,铜的存在还使硅中双空位的退火温度显著地降低.种种实验表明,在硅中与铜有关的六个主要能级分别对应于六种不同结构的深中心,在这些深中心之中既包含铜又包含点缺陷.其中E(0.043)很可能是铜与间隙硅原子的络合物,而E(0.167)及H(0.411)则很可能是铜与空位的不同形态的络合物. 相似文献
10.
The crystal and molecular structure of the complex containing cobalt-carbon and iron-sulfur cluster cores, (μ-p-CH3C6H4C2S) (μ-n-C3H7S)Fe2(CO)6Co2(CO)6, has been determined by X-ray diffraction method. The crystals are triclinic, space group P&1bar;, with a — 9.139(2), b=9.610(1), c-17.183(2) Å, α = 84.36(1), β-89.45(1), γ=88.15(1)°, V-1501.0 Å3; Z=2, Dc=1.74 g/cm3. R=0.072, Rw=0.081. The results of the structure determination show a cobalt-carbon cluster core formed through the reaction of (μ-p-CH3C6H4C2S)(μ-n-C3H7S)Fe2(CO)6 with Co2(CO)8. In the cobalt-carbon cluster core, the bond length of the original C≡C lengthened to 1.324 Å which is close to the typical value of carbon-carbon double bond. The groups connecting the carbons of the cluster core are in cis position and lie on the opposite side of cobalt atoms. In this complex, the conformation of —SC3H7 is e-type, while that of —SC2C6H4CH3 is a-type. 相似文献