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61.
Perturbative unitarization from non-linear effects is thought to deplete the gluon density for transverse momenta below the saturation scale. Such effects also modify the distribution of gluons produced in heavy-ion collisions in transverse impact parameter space. I discuss some of the consequences for the initial conditions for hydrodynamic models of heavy-ion collisions and for hard “tomographic” probes. Also, I stress the importance of realistic modelling of the fluctuations of the valence sources for the small-x fields in the impact parameter plane. Such models can now be combined with solutions of running–coupling Balitsky–Kovchegov evolution to obtain controlled predictions for initial conditions at the LHC. 相似文献
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Pressure broadening of Lyman‐lines of hydrogen‐like lithium (Li2+) has been studied using a quantum statistical approach to the line shape in dense plasmas, for details see [1]. In this communication, we concentrate on the electronic self‐energy, which is a basic input to the theory of spectral line profiles. We discuss the effect of strong, i.e. close, collisions which have been neglected so far for Li2+ plasmas, but play generally an important role in dense plasmas, as has been shown in [2]. We present a method to calculate an improved electronic self‐energy including strong collisions based on a two‐body T‐matrix and an effective optical potential. The method is tested for level broadening of the ground state of hydrogen (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
66.
We present the results of deriving the Israel-Stewart equations of relativistic dissipative fluid dynamics from kinetic theory via Grad’s 14-moment expansion. Working consistently to second order in the Knudsen number, these equations contain several new terms which are absent in previous treatments. 相似文献
67.
T. Gaitanos C. Fuchs H.H. Wolter A. Faessler 《The European Physical Journal A - Hadrons and Nuclei》2001,12(4):421-433
We investigate differential in-plane and out-of-plane flow observables in heavy-ion reactions at intermediate energies from
0.2-2 AGeV within the framework of relativistic BUU transport calculations. The mean field is based on microscopic Dirac-Brueckner-Hartree-Fock
(DB) calculations. We apply two different sets of DB predictions, those of ter Haar and Malfliet and more recent ones from
the Tübingen group, which are similar in general but differ in details. The latter DB calculations exclude spurious contributions
from the negative-energy sector to the mean field which results in a slightly softer equation of state and a less repulsive
momentum dependence of the nucleon-nucleus potential at high densities and high momenta. For the application to heavy-ion
collisions in both cases non-equilibrium features of the phase space are taken into account on the level of the effective
interaction. The systematic comparison to experimental data favours the less repulsive and softer model. Relative to non-relativistic
approaches one obtains larger values of the effective nucleon mass. This produces a sufficient amount of repulsion to describe
the differential flow data reasonably well.
Received: 8 January 2001 / Accepted: 12 November 2001 相似文献
68.
We calculate the one-particle hadronic spectra and correlation functions of pions based on a hydrodynamical model. Parameters
in the model are so chosen that the one-particle spectra reproduce experimental results of √s= 130 AGeV Au + Au collisions at RHIC. Based on the numerical solution, we discuss the space-time evolution of the fluid. Two-pion
correlation functions are also discussed. Our numerical solution suggests the formation of the quark-gluon plasma with large
volume and low net baryon density. 相似文献
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A new process of a nuclear excitation to discrete states in peripheral heavy ion collisions is studied. High-energy photons
are emitted by the exited nuclei with energies up to a few tens of GeV at angles of a few hundred microradians with respect
to the beam direction. We show that a two-stage process, where an electron-positron pair is produced by virtual photons emitted
by nuclei and then the electron or positron excites the nucleus, has a large cross-section. It is equal to about 5 b for CaCa
collisions. On the one hand, it produces a significant γ-rays background in the nuclear fragmentation region but, on the other
hand, it could be used for monitoring the nuclear beam intensity at the LHC. These secondary nuclear photons could be a good
signal for triggering peripheral nuclear collisions.
Received: 14 December 2001 / Accepted: 22 January 2002 相似文献