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821.
Jerk Influence Coefficients,via Screw Theory,of Closed Chains 总被引:2,自引:0,他引:2
In this paper a novel method for determining the kinematic influence coefficients up to the jerk analysis of closed chains with multiple degrees of freedom by means of screw theory, also known as motor algebra, is introduced. A closed chain is obtained by rigidly attaching the end-effector of a serial chain to the base link. This condition ensures that the velocity, acceleration, and jerk, both angular and of any point fixed to the end-effector are zero. Afterwards, a comparison between the kinematic equations of motion, up to the jerk analysis, obtained by traditional methods with those obtained by means of screw theory reveals the corresponding influence coefficients associated to the generalized coordinates employed to represent the motion of the closed chain. Finally, a numerical example is provided.
Sommario. In questo lavoro viene proposto un nuovo metodo per la determinazione dei coefficienti che consentono di sviluppare l'analisi cinematica (jerk incluso) di catene chiuse a molti gradi di liberta' per mezzo della screw theory o algebra dei moti spaziali. La catena chiusa e' ottenuta attaccando rigidamente l'end-effector di una catena seriale al membro di base. Questa condizione assicura che velocita' accelerazione e jerk, sia nel moto angolare che per ciascun punto solidale con l'end-effector siano nulli. Un confronto tra le equazioni cinematiche del moto, inclusa l'analisi del jerk, ottenute con metodi tradizionali e quelle ottenute dalla screw theory, mostra i corrispondenti coefficienti di influenza associati alle coordinate generalizzate impiegate per descrivere il moto della catena chiusa. Un esempio numerico conclude il lavoro. 相似文献
822.
K. Mallick P. Marcq 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,31(4):553-561
We study analytically and numerically the problem of a nonlinear mechanical oscillator with additive noise in the absence
of damping. We show that the amplitude, the velocity and the energy of the oscillator grow algebraically with time. For Gaussian
white noise, an analytical expression for the probability distribution function of the energy is obtained in the long-time
limit. In the case of colored, Ornstein-Uhlenbeck noise, a self-consistent calculation leads to (different) anomalous diffusion
exponents. Dimensional analysis yields the qualitative behavior of the prefactors (generalized diffusion constants) as a function
of the correlation time.
Received 10 October 2002 Published online 6 March 2003
RID="a"
ID="a"e-mail: mallick@spht.saclay.cea.fr 相似文献
823.
824.
A. Pautrat A. Daignere C. Goupil Ch. Simon B. Andrzejewski A.I. Rykov S. Tajima 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,33(3):279-284
We report complex impedance measurements in an untwinned YBaCuO crystal. Our broad frequency range covers both the quasi static
response and the resistive response of the vortex lattice. It allow us to characterize the irreversibility line without the
need of any frequency dependent pinning parameters. We confirm the validity of the two modes model of vortex dynamic, and
extract both the surface critical current and the flux flow resistivity around the first order transition Tm. This latter is identified by the abrupt loss of pinning and by an unexpected step of (T) at Tm.
Received 22 November 2002 / Received in final form 17 February 2003 Published online 20 June 2003
RID="a"
ID="a"e-mail: alain.pautrat@ismra.fr
RID="b"
ID="b"UMR 6508 associée au CNRS 相似文献
825.
A. Chernomoretz C. O. Dorso 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,24(1-3):197-202
In this communication we analyze the behavior of excited
drops that undergo fragmentation. We focus our attention on two
scenarios: in the first one the system is free to expand, while
in the second one it is confined inside a spherical volume. It
is shown that the caloric curve of free expanding systems does
not display a vapor branch. In the case of constrained ones,
they behave as undergoing a first order phase transition at low
densities while as a second order one at high densities. The
transition from liquid-like to vapor-like behavior is signaled
both by the caloric curves and thermal response functions. 相似文献
826.
J. Westergren S. Nordholm A. Rosén 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,22(1):81-97
The cooling of the metal cluster Pd13 in an atmosphere of rare gas has been studied by means of computer simulation. By simulation, the average energy transfer
in collisions between one cluster and one gas atom has been obtained. Emphasis has been placed on conditions when the temperatures
of the colliding species are almost equal. All modes of motion, inclusive the translation, must be considered in order to
obtain vanishing energy transfer at equilibrium. A simulation scheme is presented by which the energy transfer is zero to
the cluster when the gas and the cluster temperatures are equal. At equilibrium the energy transfer does however not vanish
for all impact parameters. In the collisions with Pd13, the cluster is heated by collisions with a small impact parameter but equally cooled by collisions with a large impact parameter.
Argon and krypton are found to cool Pd13 equally efficiently while neon and helium are less efficient cooling agents.
Received 28 September 2001 / Received in final form 8 August 2002 Published online 12 November 2002
RID="a"
ID="a"e-mail: JanW@phc.gu.se 相似文献
827.
P. Cacciani J. Cosléou F. Herlemont M. Khelkhal J. Legrand 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,22(2):199-207
When a gas sample of 13CH3F is prepared with a population of isomers (ortho and para forms) far from the equilibrium given by nuclear spin statistics,
it relaxes towards this equilibrium with an exponential decay rate. This phenomenon called nuclear spin conversion is mainly
governed by intramolecular spin-spin and spin-rotation interactions. In the quantum relaxation model [P.L. Chapovsky, Phys.
Rev. A 43, 3624 (1991)], two pairs of ortho-para levels (J
= 9, K
= 3; J'
= 11, K'
= 1) and (J
= 20, K
= 3; J'
= 21, K'
= 1) are principally responsible for the conversion. The levels of the second pair are coupled by both spin-spin and spin-rotation
interactions. The application of an electric field (up to 10 kV/cm) induces a crossing of the Stark components of this pair,
which is observed for the first time. A specific experimental set-up based on an electric field of alternating triangular
shape is used, which allows the determination of the strength of both interactions via the measurement of the spin conversion decay rates. This work yields the first experimental value for the electronic contribution
to the spin-rotation interaction in 13CH3F.
Received 23 May 2002 / Received in final form 18 September 2002 Published online 21 January 2003
RID="a"
ID="a"e-mail: Patrice.Cacciani@univ-lille1.fr 相似文献
828.
We consider a fifth-order partial differential equation (PDE) that is a generalization of the integrable Camassa–Holm equation. This fifth-order PDE has exact solutions in terms of an arbitrary number of superposed pulsons with a geodesic Hamiltonian dynamics that is known to be integrable in the two-body case N==2. Numerical simulations show that the pulsons are stable, dominate the initial value problem, and scatter elastically. These characteristics are reminiscent of solitons in integrable systems. But after demonstrating the nonexistence of a suitable Lagrangian or bi-Hamiltonian structure and obtaining negative results from Painlevé analysis and the Wahlquist–Estabrook method, we assert that this fifth-order PDE is not integrable. 相似文献
829.
A Global Solution to a
Two-dimensional Riemann Problem Involving Shocks as Free
Boundaries 总被引:4,自引:0,他引:4
YuxiZheng 《应用数学学报(英文版)》2003,19(4):559-572
We present a global solution to a Riemann problem for the pressure gradient system of equations.The Riemann problem has initially two shock waves and two contact discontinuities. The angle between the two shock waves is set initially to be close to 180 degrees. The solution has a shock wave that is usually regarded as a free boundary in the self-similar variable plane. Our main contribution in methodology is handling the tangential oblique derivative boundary values. 相似文献
830.
It is proved that the vortices of a Ginzburg-Landau system are attracted by impurities or inhomo-geneities in the super-conducting materials. The strong H1-convergence for the system is also studied. 相似文献