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排序方式: 共有1132条查询结果,搜索用时 31 毫秒
991.
In its simpler form, the Heisenberg-Pauli-Weyl inequality says that
992.
Henri Berestycki FranÇois Hamel Luca Rossi 《Annali di Matematica Pura ed Applicata》2007,186(3):469-507
This paper is devoted to the study of some class of semilinear elliptic equations in the whole space:
The aim is to prove uniqueness of positive- bounded solutions—Liouville-type theorems. Along the way, we establish also various
existence results.
We first derive a sufficient condition, directly expressed in terms of the coefficients of the linearized operator, which
guarantees the existence result as well as the Liouville property. Then, following another approach, we establish other results
relying on the sign of the principal eigenvalue of the linearized operator about u= 0, of some limit operator at infinity which we define here. This framework will be seen to be the most general one. We also
derive the large time behavior for the associated evolution equation.
Mathematics Subject Classification (2000) 35B05, 35B50, 35J60, 35K55, 35K57, 35P15 相似文献
993.
994.
995.
稀土元素La掺杂对AlN性能影响的第一性原理研究 总被引:2,自引:0,他引:2
本文通过基于密度泛函理论的第一性原理计算方法研究了稀土元素La掺杂对纤锌矿结构AlN力学性能及压电性能的影响.计算得到的AlN各项力学性能及压电性能与实验值较吻合.掺杂稀土元素La会降低其体模量、剪切模量与杨氏模量,但会使AlN由脆性材料转变为韧性材料.压电性能计算结果表明,掺杂稀土元素La后,可使体系的压电性能提升15%左右.电子结构分析结果表明La的引入会降低体系中化学键的作用强度,从而提升了体系的塑性及压电性能. 相似文献
996.
阳离子掺杂能够有效提高材料的电化学性能,而对掺杂材料结构和电化学性质的研究能从理论上解释产生这种变化的原因.本文采用基于密度泛函理论的第一性原理方法,研究了过渡族金属掺杂的镁离子电池正极材料TM_(0.125)V_(0.875)S_4(TM=Mo、Fe、Co、Ni)的几何和电子结构变化,计算结果显示:通过采用范德华力修正的GGA+vdw-DF方法,获得了和实验结果相一致的晶格常数.阳离子掺杂后,a轴和b轴晶格常数减小,而c轴晶格常数增大.电子态密度分析表明离子掺杂能够有效降低带隙,提高材料的电子电导率.通过对镁离子扩散进行微动弹性带(NEB)计算,发现Fe掺杂能够有效降低扩散能垒,提高材料的离子迁移率. 相似文献
997.
998.
We have investigated the structural, electronic and magnetic properties in quaternary CoFeCrAl Heusler alloy. Rietveld refinement and Mössbauer spectroscopy of samples quenched from 973 K show absence of the A2 phase and presence of a highly ordered B2‐type structure. Full‐potential linearized augmented plane wave calculations using the experimental lattice constant show that there is an energy gap of 0.41 eV around the Fermi level in the bands for minority spin electrons. Partial substitution of Co by Fe in Co2CrAl thus brings excellent structural ordering while retaining the high Curie temperature, spontaneous magnetization and half‐metallicity necessary for application as spin valves. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
999.
Erjun Zhao Jinping Wang Jian Meng Zhijian Wu 《Journal of computational chemistry》2010,31(9):1904-1910
The phase stability and elastic properties of Re? B system were systematically investigated by use of the density functional theory. The formation enthalpies are negative for Re3B, Re7B3, Re2B, ReB, Re2B3, and ReB2, indicating that they are thermodynamically stable. Re7B3, Re2B, ReB, Re2B3, and ReB2 are mechanically stable. Combining the study of enthalpy and pressure relationship with the convex hull, it was found that the ground state phases are Re3B, Re7B3, and ReB2 at zero pressure, in agreement with the experimental observations. At the pressure of 90 GPa, Re3B, and ReB2 are the most stable phases. © 2010 Wiley Periodicals, Inc. J Comput Chem 2010 相似文献
1000.
F.E. Hildebrand 《哲学杂志》2013,93(34):4250-4290
The extraordinary properties of shape-memory alloys stem from the formation and evolution of their complex microstructure. At lower temperatures, this microstructure typically consists of martensitic laminates with coherent twin boundaries. We suggest a variational-based phase field model at finite strains for the formation and dissipative evolution of such two-variant martensitic twinned laminate microstructures. The starting point is a geometric discussion of the link between sharp interface topologies and their regularisation, which is connected to the notion of Γ-convergence. To model the energy storage in the two-phase laminates, we propose an interface energy that is coherence-dependent and a bulk energy that vanishes in the interface region, thus allowing for a clear separation of the two contributions. The dissipation related to phase transformation is modelled by use of a dissipation potential that leads to a Ginzburg–Landau type evolution equation for the phase field. We construct distinct rate-type continuous and finite-step-sized incremental variational principles for the proposed dissipative material and demonstrate its modelling capabilities by means of finite element simulations of laminate formation and evolution in martensitic CuAlNi. 相似文献