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111.
QCD perturbation theory for confined quarks and gluons (inhadrons) is discussed.Based on the equivalent potential for the quark-gluon interaction derived, the energyshifts of hadrons and hadron mass difference in MIT bag (cavity) model and correcpond-ing approximation of the w. f. with Gassian form are calculated. 相似文献
112.
113.
LU ZhongDao SA BenHao Masanori Matsuda Junichi Nagata Atsushi Nakamura Osamu Miyamura 《中国物理C(英文版)》2000,24(8):743-747
The Λ multiplicity and Λ/p ratio are studied by hadron transportation-string fragmentation model in relativistic heavy ion collisions. Firstly, the dependence of Λ multiplicity and Λ/p ratio on the system size and the collision centrality is studied. It shows that the Λ and p multiplicities go up as the increase of system size and the increase of collision centrality. However, their ratio keeps almost a constant. The effect of Λ annihilation cross section to Λ multiplicity and Λ/p ratio is also studied. It is found that this effect is weak: Λ multiplicity and Λ/p ratio have a little amount of increase by the decrease of Λ annihilation cross section. Even the cross section is down to zero, Λ/p ratio is only 1.2 in 200A GeV AuAu head on collision. The Λ/p ratio is obtained to be 0.28 in pp collision, lying in the range of experimental data:0.2—0.3. It is also obtained that the ratio in AA collisions is 3—5 times of that in pp collision. 相似文献
114.
J. Gottlieb 《Fresenius' Journal of Analytical Chemistry》1870,9(1):251-253
Ohne Zusammenfassung 相似文献
115.
The carbon shifts of the Iboga-type alkaloids catharanthine, voacangine, coronaridine, ibogaine, dihydrocatharanthine and epiibogamine were recorded and correlated with the conformation of the natural bases. A 13C-NMR. analysis of heyneanine determined its C(19) configuration and a similar study of epiheyneanine proved its structure. 相似文献
116.
The dynamic response of parametrically excited microbeam arrays is governed by nonlinear effects which directly influence
their performance. To date, most widely used theoretical approaches, although opposite extremes with respect to complexity,
are nonlinear lumped-mass and finite-element models. While a lumped-mass approach is useful for a qualitative understanding
of the system response it does not resolve the spatio-temporal interaction of the individual elements in the array. Finite-element
simulations, on the other hand, are adequate for static analysis, but inadequate for dynamic simulations. A third approach
is that of a reduced-order modeling which has gained significant attention for single-element micro-electromechanical systems
(MEMS), yet leaves an open amount of fundamental questions when applied to MEMS arrays. In this work, we employ a nonlinear
continuum-based model to investigate the dynamic behavior of an array of N nonlinearly coupled microbeams. Investigations focus on the array’s behavior in regions of its internal one-to-one, parametric,
and several internal three-to-one and combination resonances, which correspond to low, medium and large DC-voltage inputs,
respectively. The nonlinear equations of motion for a two-element system are solved using the asymptotic multiple-scales method
for the weakly nonlinear system in the afore mentioned resonance regions, respectively. Analytically obtained results of a
two-element system are verified numerically and complemented by a numerical analysis of a three-beam array. The dynamic behavior
of the two- and three-beam systems reveal several in- and out-of-phase co-existing periodic and aperiodic solutions. Stability
analysis of such co-existing solutions enables construction of a detailed bifurcation structure. This study of small-size
microbeam arrays serves for design purposes and the understanding of nonlinear nearest-neighbor interactions of medium- and
large-size arrays. Furthermore, the results of this present work motivate future experimental work and can serve as a guideline
to investigate the feasibility of new MEMS array applications. 相似文献
117.
Simaan S Marks V Gottlieb HE Stanger A Biali SE 《The Journal of organic chemistry》2003,68(2):637-640
Octakis(bromomethyl)naphthalene (4) adopts in the crystal a chiral conformation with a helical central naphthalene core and the bromomethyl groups disposed in an alternate up-down "in" arrangement. According to MM3 calculations, this conformation is less stable than the corresponding all alternated "out" form, while B3LYP/LANL2DZ calculations suggest the opposite stability order. The topomerization barrier (16.0 kcal mol(-1)) is ascribed to an enantiomerization process requiring 180 degrees rotation of all the bromomethyl groups and reversal of the helical sense of the naphthalene core. 相似文献
118.
119.
The φ meson productions in Au+Au and/or Pb+Pb collisions at AGS, SPS,RHIC, and LHC energies have been studied systematically with a hadron andstring cascade model LUCIAE. After considering the energy dependence of themodel parameter α in string fragmentation function and adjusting itto the experimental data of charged multiplicity to a certain extent,the model predictions for φ meson yield, rapidity, andtransverse mass distributions are compatible with the experimental data atAGS, SPS and RHIC energies. A calculation for Pb+Pb collisions at LHC energyis given as well. The obtained fractional variable in string fragmentationfunction shows a saturation in energy dependence. It is discussed that thesaturation of fractional variable in string fragmentation function might be aqualitative representation of the energy dependence of nuclear transparency. 相似文献
120.
Aubin C Bernard C Detar C Dipierro M El-Khadra A Gottlieb S Gregory EB Heller UM Hetrick J Kronfeld AS Mackenzie PB Menscher D Nobes M Okamoto M Oktay MB Osborn J Simone J Sugar R Toussaint D Trottier HD;Fermilab Lattice;MILC;HPQCD 《Physical review letters》2005,94(1):011601
We present the first three-flavor lattice QCD calculations for D-->pilnu and D-->Klnu semileptonic decays. Simulations are carried out using ensembles of unquenched gauge fields generated by the MILC Collaboration. With an improved staggered action for light quarks, we are able to simulate at light quark masses down to 1/8 of the strange mass. Consequently, the systematic error from the chiral extrapolation is much smaller than in previous calculations with Wilson-type light quarks. Our results for the form factors at q(2)=0 are f(D-->pi)(+)(0)=0.64(3)(6) and f(D-->K)(+)(0)=0.73(3)(7), where the first error is statistical and the second is systematic, added in quadrature. Combining our results with experimental branching ratios, we obtain the Cabibbo-Kobayashi-Maskawa matrix elements |V(cd)|=0.239(10)(24)(20) and |V(cs)|=0.969(39)(94)(24), where the last errors are from experimental uncertainties. 相似文献