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991.
With the use of the nonpolynomial closure 1/
z
in the Mott-Smith approximation of the solution of the Boltzmann equation, we obtain a value of the density gradient in the limit of a very weak shock wave that is close to the correct value. For the determination of the transverse temperature gradient we calculated the
x
2
/
z
moment of the Mott-Smith collision integral. The effective values of viscosity and thermal conductivity in the limit of a very weak shock wave were calculated for inverse-power potentials and found to agree almost exactly with the Chapman-Enskog values. Such a comparison can serve as a criterion for the evaluation of different bimodal theories. Various bimodal theories give different values of viscosity and thermal conductivity, but all of them give 33 % too high a value of the Eucken ratio. 相似文献
992.
993.
994.
G Ananthakrishna 《Pramana》1979,12(5):543-561
The model introduced for clustering of quenched-in vacancies in the first part of this series of papers is considered. Using
a generating function, the rate equations are converted into a first order partial differential equation for the generating
function coupled to a differential equation for the rate of change of the concentration of single vacancy units. A decoupling
scheme is effected which gives an exponentially decaying solution with a very short time constant for the concentration of
single vacancy units. The differential equation for the generating function is solved for times larger than the time required
for the concentration of single vacancy units to reach its asymptotic value. The distribution for the size of the clusters
is obtained by inverting the solution thus obtained. Several results that follow are shown to be in reasonably good agreement
with the experimental results. 相似文献
995.
In view of an excellent agreement between the recently determinedv
μ-hadron couplings and predictions of the standard model, the basic question discussed is how far its neutral current predictions
can be mimiced in going either from the isodoublet to an isotriplet (or an even higher isospin) left-handed representation
or from SU
L
(2) × U(1) toG × U(1), whereG is a simple group of rank two. This question is addressed with reference to a sufficiently broad class of schemes. Their
most distinctive properties are: in the higher isospin scheme, neutrino couplings are precisely in the form obtainable with
standard l.h. representation; the higher g.g. scheme isL+R type in which, to each light fermion of evenRU parity, a superheavy fermion of the same charge and oddRU parity is associated, parity conservation forbidding their mixing. Reasons for excluding theL-type andG
2 higher g.g. schemes are given. Their neutral current predictions are compared with those of the standard model. A higher
isospin representation can mimic the predictions of the standard model in inclusive and semi-inclusivev
μ-hadron reactions but is conclusively discriminated from the isodoublet representation by elasticv
μ
(−
p scattering. TheG × U(1) scheme can mimic standard model neutrino sector but is conclusively discriminated from minimal scheme by parity violating
effects. 相似文献
996.
A one-dimensional system of hard-rod particles with rotational-like internal degrees of freedom is considered. Particles interact with each other through the infinite-range, infinitely weak attractive Kac potential, and through a nearest-neighbor short-range potential. The latter depends also on the internal states of the interacting particles. Exact results for thermodynamic properties and for some correlation functions are obtained. It is found that the considered system exhibits several first-order transitions between phases with different rotational structure, i.e., with different ordering with respect to the internal degrees of freedom. The calculated equation of state seems to suggest that in the solutions of liquid-crystalline substances in neutral solvents there may exist regions in which the coefficient of thermal expansion is negative—an effect similar to that well known in liquid water. 相似文献
997.
LieWen Chen 《中国科学G辑(英文版)》2009,52(10):1494-1505
A phenomenological momentum-independent(MID) model is constructed to describe the equation of state(EOS) for isospin asymmetric nuclear matter,especially the density dependence of the nuclear symmetry energy Esym(ρ).This model can reasonably describe the general properties of the EOS for symmetric nuclear matter and the symmetry energy predicted by both the sophisticated isospin and momentum dependent MDI model and the Skyrme-Hartree-Fock approach.We find that there exists a nicely linear correlation betwee... 相似文献
998.
在复金慈堡-朗道方程描述的振荡介质中研究了平面波的反射.从理论上给出了产生反射的条件,导出了反射波和入射波这两个区域的分界线与两种介质分界线的夹角.发现两类反射,一类为回折射产生的反射,对于这类反射,理论上给出了反射角;另一类为纯反射,它与折射无关.理论分析与数值模拟结果均表明:只有当入射角大于临界入射角才会发生反射,而且反射角等于临界入射角;对于纯反射,反射角随波频率增大而增大.
关键词:
复金慈堡-朗道方程
平面波
反射 相似文献
999.
1000.
Michael Goldberg 《Proceedings of the American Mathematical Society》2007,135(10):3171-3179
We prove a dispersive estimate for the Schrödinger equation on the real line, mapping between weighted spaces with stronger time-decay ( versus ) than is possible on unweighted spaces. To satisfy this bound, the long-term behavior of solutions must include transport away from the origin. Our primary requirements are that be integrable and not have a resonance at zero energy. If a resonance is present (for example, in the free case), similar estimates are valid after projecting away from a rank-one subspace corresponding to the resonance.