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41.
The production of neutral pions by the interaction of 200A·GeV p and16O projectiles with a Au target has been studied in the pseudorapidity range 1.5≦η≦2.1. Transverse momentum spectra have been measured between 0.4 GeV/c and 3.6 GeV/c and their dependence on the centrality of the collision has been investigated. The peripheral-collision spectra display a marked change of slope with a hard component starting at about 1.8 GeV/c, in contrast to central-collision data. The data are discussed in comparison to p+p and α+α data from the ISR.  相似文献   
42.
The nuclear interaction between natural copper and 1 GeV 12C has been investigated with radiochemical methods. Charge and mass distributions have been derived. The form of the mass yield curve is determined by the total kinetic energy in the system.  相似文献   
43.
A graphite cathode in N,N-dimethylformamide with tetraalkylammonium salts as supporting electrolyte was found to be able to accept reversibly a rather large charge in a way somewhat akin to the formation of anion radicals and ion pairs of polycondensed aromatic hydrocarbons. The charged graphite has certain similarities with an amalgam, it can thus be used as an insoluble chemical reducing agent. The charging of the graphite depends on the size of the cation, in the presence of very large cations the cathode disintegrates. The nature of the charge is discussed on the basis of i-E curves and coulometric results.  相似文献   
44.
45.
The response of damped linear finite systems (discrete and continuous) to harmonic, stationary random, and transient excitations is studied. The assumed damping may be light or heavy, viscous and/or hysteretic (the latter being frequency-independent or frequency-dependent), and proportionally or non-proportionally distributed over the structure. Closed-form analytic transfer functions are derived for beam systems. In order to rationalize subsequent numerical calculations, the transfer functions are approximated by using truncated series. Complex eigenfrequencies of the structure and complex residues of the actual transfer function are used. Special interest is paid to the mathematical modelling of experimentally measured damping. Causality requirements are considered. Numerical examples are given. An efficient method (by which aliasing is eliminated) for numerical Fourier transformation has been developed and applied.  相似文献   
46.
Shock-tube HeXe-laser absorption data at ωL=2850.633 cm-1 for CH3COOCH3 at 757≤T, °K≤1344, NO2at 412≤T, °K≤1859, andCH3at 1283≤T, °K≤1562 are presented. Approximate models are used for the effective spectral absorption coefficient of vibration-rotation lines for analytical representations of the results around atmospheric pressures. For CH3COOCH3, an equivalent Voigt-profile for an isolated line was adopted in order to account for a dependence on total pressure of the laser absorption coefficient. Shock-tube emission data at λ=6.890 μ(Δλ=0.197μ) forCH3COOCH3at 814≤T, °K≤1651 and for CH3at 1377≤T, °K≤1562 in the v4-fundamental of the H-bond bending mode of the CH3-group are well described at atmospheric pressures by approximations of just-overlapping-line models for polyatomic molecules. The adopted models are useful for concentration-time history measurements of methyl acetate, nitrogen dioxide, and methyl radicals behind shock waves.  相似文献   
47.
The delayed neutron emission probability(P n) has been measured for79-83Ga,87-89Br,92-96Rb127-132In134,135Sb137-139I and141 -145Cs, by means of sources produced at the OSIRIS isotope separator at Studsvik. The half-life determinations of127, 129, 132In have been improved.  相似文献   
48.
Target remnants withZ<3 from proton-nucleus and16O-nucleus reactions at 60 and 200 GeV/nucleon were measured in the angular range from 30° to 160° (?1.7<η<1.3) employing the Plastic Ball detector. The excitation energy of the target spectator matter in central oxygen-induced collisions is found to be high enough to allow for complete disintegration of the target nucleus into fragments withZ<3. The average longitudinal momentum transfer per proton to the target in central collisions is considerably higher in the case of16O-induced reactions (≈300 MeV/c) than in proton-induced reactions (≈130 MeV/c). The baryon rapidity distributions are roughly in agreement with one-fluid hydrodynamical calculations at 60 GeV/nucleon16O+Au but are in disagreement at 200 GeV/nucleon, indicating the higher degree of transparency at the higher bombarding energy. Both, the transverse momenta of target spectators and the entropy produced in the target fragmentation region are compared to those attained in head-on collisions of two heavy nuclei at Bevalac energies. They are found to be comparable or do even exceed the values for the participant matter at beam energies of about 1–2 GeV/nucleon.  相似文献   
49.
Positronium yields as a function of pyridine concentration were studied in nine nonpolar solvents. Strong enhancements in the Ps yields on addition of low concentrations (< 0.3 M) of the positive hole scavenger pyridine were found in those liquids where the hole moves rapidly (i.e. partly delocalized), but not in those where the hole moves slowly. Pyridine acts also as a very weak Ps inhibitor in all systems investigated if its concentration exceeds a certain limit (≈ 0.3 M). The results can be well interpreted within the framework of the spur reaction model of Ps formation.  相似文献   
50.
Single crystals of methyl methacrylate (MMA), methyl acrylate (MA), and acrolein (A) have been prepared by a low-temperature technique. After irradiation with γ-rays at 77°K the paramagnetic species were identified by ESR spectroscopy. MMA gave a seven-line single spectrum from radicals formed by hydrogen addition. The hyperfine coupling constants are slightly anisotropic with a mean value of 22 G. Radical pairs were observed as ΔMs = 1 and ΔMs = 2 transitions; the hyperfine coupling was 11 G. From the strongly anisotropic dipolar interaction, upper limits for the distances between the pair components were calculated to be 5.45 Å and 6.3 Å. MA gave a five-line main spectrum with the same hyperfine coupling values and two radical pairs, one with a distance 5.9 Å between the components. In a there was also a strongly anisotropic interaction. The hyperfine coupling of the ΔMs = 2 transition was 9.8 G. The number of radical pairs compared to the total number of radicals increases only slightly with the radiation dose. This makes it likely that pair formation occurs in the spurs and blobs formed by the γ-radiation. At an increased temperature the radical pairs disappeared; the spectrum of MMA changed to that characteristic of propagating polymer radicals.  相似文献   
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