全文获取类型
收费全文 | 6731篇 |
免费 | 906篇 |
国内免费 | 559篇 |
专业分类
化学 | 1317篇 |
晶体学 | 59篇 |
力学 | 542篇 |
综合类 | 75篇 |
数学 | 2280篇 |
物理学 | 2013篇 |
无线电 | 1910篇 |
出版年
2024年 | 12篇 |
2023年 | 91篇 |
2022年 | 134篇 |
2021年 | 132篇 |
2020年 | 179篇 |
2019年 | 158篇 |
2018年 | 161篇 |
2017年 | 224篇 |
2016年 | 276篇 |
2015年 | 287篇 |
2014年 | 409篇 |
2013年 | 515篇 |
2012年 | 421篇 |
2011年 | 466篇 |
2010年 | 380篇 |
2009年 | 444篇 |
2008年 | 427篇 |
2007年 | 468篇 |
2006年 | 450篇 |
2005年 | 335篇 |
2004年 | 308篇 |
2003年 | 271篇 |
2002年 | 247篇 |
2001年 | 212篇 |
2000年 | 193篇 |
1999年 | 169篇 |
1998年 | 162篇 |
1997年 | 114篇 |
1996年 | 102篇 |
1995年 | 92篇 |
1994年 | 76篇 |
1993年 | 45篇 |
1992年 | 46篇 |
1991年 | 33篇 |
1990年 | 22篇 |
1989年 | 17篇 |
1988年 | 15篇 |
1987年 | 16篇 |
1986年 | 10篇 |
1985年 | 21篇 |
1984年 | 15篇 |
1983年 | 7篇 |
1982年 | 6篇 |
1981年 | 11篇 |
1980年 | 3篇 |
1979年 | 4篇 |
1977年 | 2篇 |
1959年 | 1篇 |
1957年 | 2篇 |
1936年 | 2篇 |
排序方式: 共有8196条查询结果,搜索用时 13 毫秒
61.
M. Nierlich L.L.B. F. Boue L.L.B. A. Lapp L.L.B. R. Oberthür I.L.L. 《Colloid and polymer science》1985,263(12):955-964
We have studied salt free semi dilute polyelectrolyte solutions by small angle neutron scattering. Specific labelling associated with an extrapolation method has allowed the separation of the form factor of a single polyelectrolyte chainS
1(q) and the structure factorS
2(q). Two lengths are deduced from these two factors: the persistence lengthb
t which characterizes the electrostatic interactions along the chain by a fitting ofS
1(q) with calculation of the scattering function for a wormlike chain, and fromS
2(q),q
m
–1
which characterizes the interactions between chains. These two lengths vary in the same way with the concentration of polyions (b
t C
p
–1/2
,q
m
–1
C
p
–1/2
) and a constant relation exists between them: only one length is then necessary to describe the structure of polyelectrolyte soltuion on this semidilute concentration range.Laboratoire Commun CEA-CNRS. 相似文献
62.
D. P. Singh R. Visvanathan A. E. Duncan B. Duponchel Y. Boussoualem S. Kumar 《Liquid crystals》2019,46(3):376-385
CdSe quantum dots (QDs) dispersed ferroelectric liquid crystal (FLC) has been subjected to small and wide-angle X-ray scattering and atomic force microscopy to understand the molecular organization in chiral smectic C (SmC*) phase. SAXS indicates that the presence of QDs causes enhancement in the smectic layer separation. The smectic order parameter for neat FLC and FLC–QDs mixtures is obtained in the range of 0.6 to 0.85. Both smectic order parameter and structural tilt are found to be lesser for FLC–QDs mixtures as compared to neat FLC. The insertion of QDs in SmC* matrix causes localized smectic layer distortion in such a way that spontaneous polarization remains almost the same but the electro-optic switching of molecules becomes faster. We have outlined the superiority of FLC–QDs mixtures for electrical energy storage and their suitability in electronic devices. 相似文献
63.
接触角及其在表面化学研究中的应用 总被引:34,自引:0,他引:34
润湿是一种流体取代界面上另一种流体的界面现象,通常是指液体从固体表面取代气体的过程。如在干净玻璃板上加水,排走表面上的空气形成薄的水膜,即为铺展润湿,简称铺展,此过程的特点是原固气界面消失,气液界面扩大,并形成新的固液界面。将固体完全浸渍于液体中,固气界面消失,气液界面不变,形成新的固液界面,此过程为现润湿(浸湿)。液体与固体接触,气液和固气界面减小,形成固液界面的过程为沾湿。润湿过程涉及固体和液 相似文献
64.
Summary -Lactoglobulin A and B (-LACT) were separated by displacement chromatography (DSC) on an ionexchange column using dextran sulfate as the displacer. A LALLS photometer and a UV detector, in series, were used to determine the molecular weight (MW) of the proteins, on-line. The results indicate that both, -LACT A and B, were present as dimers in the buffer used for the mobile phase. The MWs of the proteins were about 6–8% higher than the theoretical MW of a dimer (37,000). Additional control studies have shown the presence of a high molecular weight species in both the proteins, which could possibly be an aggregate. This species was observed in the LALLS signal but was nearly absent in the UV signal. Our work has demonstrated the feasibility of interfacing LALLS with displacement chromatography for detecting impurities or aggregates which may be difficult to detect by conventional detectors used for chromatography. 相似文献
65.
66.
67.
A comparison is made between the distribution of residue preferences, three dimensional nearest neighbour contacts, preferred rotamers, helix-helix crossover angles and peptide bond angles in three sets of proteins: a non-redundant set of accurately determined globular protein structures, a set of four-helix bundle structures and a set of membrane protein structures. Residue preferences for the latter two sets may reflect overall helix stabilising propensities but may also highlight differences arising out of the contrasting nature of the solvent environments in these two cases. The results bear out the expectation that there may be differences between residue type preferences in membrane proteins and in water soluble globular proteins. For example, the -branched residue types valine and isoleucine are considerably more frequently encountered in membrane helices. Likewise, glycine and proline, residue types normally associated with `helix-breaking' propensity are found to be relatively more common in membrane helices. Three dimensional nearest neighbour contacts along the helix, preferred rotamers, and peptide bond angles are very similar in the three sets of proteins as far as can be ascertained within the limits of the relatively low resolution of the membrane proteins dataset. Crossing angles for helices in the membrane protein set resemble the four helix bundle set more than the general non-redundant set, but in contrast to both sets they have smaller crossing angles consistent with the dual requirements for the helices to form a compact structure while having to span the membrane. In addition to the pairwise packing of helices we investigate their global packing and consider the question of helix supercoiling in helix bundle proteins. 相似文献
68.
69.
《Journal of computational chemistry》2018,39(12):721-734
New Lennard‐Jones parameters have been developed to describe the interactions between atomistic model of graphene, represented by REBO potential, and five commonly used all‐atom water models, namely SPC, SPC/E, SPC/Fw, SPC/Fd, and TIP3P/Fs by employing particle swarm optimization (PSO) method. These new parameters were optimized to reproduce the macroscopic contact angle of water on a graphene sheet. The calculated line tension was in the order of 10−11 J/m for the droplets of all water models. Our molecular dynamics simulations indicate the preferential orientation of water molecules near graphene–water interface with one O H bond pointing toward the graphene surface. Detailed analysis of simulation trajectories reveals the presence of water molecules with ≤∼1, ∼2, and ∼4 hydrogen bonds at the surface of air–water interface, graphene–water interface, and bulk region of the water droplet, respectively. Presence of water molecules with ≤∼1 and ∼2 hydrogen bonds suggest the existence of water clusters of different sizes at these interfaces. The trends observed in the libration, bending, and stretching bands of the vibrational spectra are closely associated with these structural features of water. The inhomogeneity in hydrogen bond network of water at the air–water and graphene–water interface is manifested by broadening of the peaks in the libration band for water present at these interfaces. The stretching band for the molecules in water droplet shows a blue shift as compared to the pure bulk water, which conjecture the presence of weaker hydrogen bond network in a droplet. © 2017 Wiley Periodicals, Inc. 相似文献
70.
Masae Takahashi Masako Shimazaki Jun Yamamoto 《Journal of Polymer Science.Polymer Physics》2001,39(1):91-100
We derived typical phase diagrams for aqueous solutions of methyl cellulose (MC) of different molecular weights via micro‐differential scanning calorimetry, small‐angle X‐ray scattering, and visual inspection. The phase diagrams showed the cooccurrence of gelation and phase separation and qualitatively agreed with the theoretically calculated diagrams. The sol–gel transition line and phase separation line of a lower critical solution point type shifted toward lower temperatures and lower concentrations with an increase in the MC molecular weight. The sol–gel transition line intersected at a temperature higher than the critical point of the phase separation; therefore, both sol–gel phase separation and gel–gel phase separation were possible, depending on the temperature. Specifically, through visual inspection of a high molecular weight MC sample in the critical temperature region, we observed phase separation into two coexisting gels with different polymer concentrations. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 39: 91–100, 2001 相似文献