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91.
We apply the technique of the Green's function to the vibronically tangled spectrum of pyrene in a biphenyl matrix. We can deperturb the spectrum mathematically and readily assign the resulting weighted density of states. The analysis is reasonably successful and agrees with ground-state data and estimates of the excited-state frequencies previously made by others.  相似文献   
92.
93.
The resonant absorption of the 58 keV Mößbauer line under excitation of one phonon states in TbO x was investigated. Using an ultra centrifuge, theγ energy was shifted by ±25meV. Narrow absorption lines at 14.1 meV, 16.0 meV and presumably at 12.3 meV are interpreted as being caused by localized modes of the terbium ion.  相似文献   
94.
Line-by-line absorption cross sections have been computed at 220° and 300°K for the X2Π32?A2Π32, v″ = 0 to v″ = 3 progressions of ClO. When the 300°K cross sections are convolved with a Gaussian function of 2 Å bandwidth, a maximum of 10.6 mb is observed at 277.4 nm, corresponding to the band head of the v″ = 0 to v′ = 11 transition. To calculate effective rate constants for predissociation of the A2Π32 state of ClO at altitudes ranging from 20 to 50km, the absorption cross sections were combined with estimates of the solar flux that penetrates to each altitude. The rate of predissociation is calculated to be much greater than the rate of direct photodissociation, but the former is still small compared to the loss rate of ClO caused by reactions with NO and O. Therefore, the contribution of predissociation to the destruction of ClO accounts for at most 2% of the total ClO loss. Further, calculations with a simplified chemical model indicate that the effect of ClO predissociation is to lower the rate of ozone depletion at all altitudes by a maximum of only 1%.  相似文献   
95.
Valence-shell binding energy spectra and momentum distributions of CS2 have been measured using non-coplanar symmetric binary (e,2e) spectroscopy. The present measurements are compared with previously published binding energy spectra calculated using the many body 2ph-TDA Green's function (GF) method and the symmetry-adapted cluster configuration-interaction (SAC CI) method. The measured and the calculated binding energy spectra both show extensive population splittings particularly above 20 eV, confirming a significant breakdown of independent particle ionization picture. A relatively strong-outer valence many-body state at 17.0 eV is shown to be satellite of the (2π0)?1 state, in accord with earlier conclusions of photoelectron studies. Momentum distributions measured at several carefully chosen binding energies are compared with the corresponding molecular orbital momentum distributions calculated using small and extended gaussian basis sets. The good qualitative agreement between momentum distributions measured in the inner-valence region wth theoretical 4σm and 5σg orbital momentum distributions confirms the qualitative predictions of satellite parentages by GF and SAC CI calculations. Momentum and position density contour maps of individual orbitals are used to interpret the shapes and atomic characters of the experimental momentum distributions. Momentum densities of the valence orbitals of CS2 are compared with those of the respective valence isoelectronic species CO2  相似文献   
96.
The temporal development of the small-signal gain on the Cl2(DA) transition at 258 nm has been investigated by means of an amplified spontaneous emission (ASE) technique. For electron beam pumped He/Cl2 mixtures, the gain appears only at the end of the pumping pulse, whereas for He/Cl2/CCl4 mixtures the temporal gain profile coincides with the fluorescence pulse, and the maximum gain coefficient increases by about a factor of two. The observed effects are due to the mixing of both halogen donors and can be explained by considering the quenching of theD-state by electrons.  相似文献   
97.
Summary Potential energy curves for the weakly bound6+,6, and4+ states of NO are presented at various levels of correlation treatment. The binding energies for the van der Waals minima vary from about 30 cm–1 for the6+ state to about 20 cm–1 for the4+ and6 states. We investigate the importance of constraining the wave function to dissociate to a spherically symmetric O atom where the oxygen 2p orbitals are equivalent. For high levels of correlation treatment, we find that these restrictions have little effect on the potential, while greatly increasing the length of the CI expansion.  相似文献   
98.
Full configuration-interaction (FCI) calculations have been performed for the ã 1A1–b1B1and ã 1A1–(2)1A1transitions in CH2 and for selected dipole and quadrupole transitions in BeO. The FCI transition moments are compared to those obtained from correlation treatments that truncate the n-particle expansion. The state-averaged MCSCF/SOCI and FCI results agree well, even for BeO, where the CASSCF level nonorthogonal transition moment differs from the state-averaged CASSCF transition moment.  相似文献   
99.
Total and partial-channel photoabsorption cross-section calculations in H2O are reported employing the time-dependent Hartree-Fock approximation and Stieltjes-Tchebycheff imaging procedures, and comparisons are made with the corresponding results of recent (e, 2e), (e, e + ion), and synchrotron-radiation dipole oscillator-strength studies.  相似文献   
100.
Summary We have compared transition moments (TMs) obtained using the length and velocity representations for transitions from the ground state of H2 to the lowest two1 u and two1 u + Rydberg states, theA 1X 1+ transition in BH, and theA 1 u X 1 g + transition in C2. For H2, the TMs in the length and velocity representations agree well even in cases where the one-particle basis is incomplete and the TM has not converged. For BH and C2 the TM in the length representation converges rapidly with improvements in the one-particle basis set and is insensitive to inner-shell correlation. In contrast, in the velocity representation convergence with improvements in the one-particle basis is much slower, especially for C2, and the TMs are significantly changed by inner-shell correlation. Thus the difference between the TMs in the length and velocity representations would not appear to be a viable diagnostic of TM convergence.  相似文献   
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