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171.
Thomas Enevoldsen Jens Oddershede Stephan P. A. Sauer 《Theoretical chemistry accounts》1998,100(5-6):275-284
We present correlated calculations of the indirect nuclear spin-spin coupling constants of HD, HF, H2O, CH4, C2H2, BH, AlH, CO and N2 at the level of the second-order polarization propagator approximation (SOPPA) and the second-order polarization propagator
approximation with coupled-cluster singles and doubles amplitudes – SOPPA(CCSD). Attention is given to the effect of the so-called
W
4 term, which has not been included in previous SOPPA spin-spin coupling constant studies of these molecules. Large sets of
Gaussian basis functions, optimized for the calculation of indirect nuclear spin-spin coupling constants, were used instead
of the in general rather small basis sets used in previous studies. We find that for nearly all couplings the SOPPA(CCSD)
method performs better than SOPPA.
Received: 6 July 1998 / Accepted: 8 September 1998 / Published online: 23 November 1998 相似文献
172.
H. Reinhardt 《Annals of Physics》2009,324(4):735-786
We study the Hamiltonian approach to 1 + 1 dimensional Yang-Mills theory in Coulomb gauge, considering both the pure Coulomb gauge and the gauge where in addition the remaining constant gauge field is restricted to the Cartan algebra. We evaluate the corresponding Faddeev-Popov determinants, resolve Gauss’ law and derive the Hamiltonians, which differ in both gauges due to additional zero modes of the Faddeev-Popov kernel in the pure Coulomb gauge. By Gauss’ law the zero modes of the Faddeev-Popov kernel constrain the physical wave functionals to zero colour charge states. We solve the Schrödinger equation in the pure Coulomb gauge and determine the vacuum wave functional. The gluon and ghost propagators and the static colour Coulomb potential are calculated in the first Gribov region as well as in the fundamental modular region, and Gribov copy effects are studied. We explicitly demonstrate that the Dyson-Schwinger equations do not specify the Gribov region while the propagators and vertices do depend on the Gribov region chosen. In this sense, the Dyson-Schwinger equations alone do not provide the full non-abelian quantum gauge theory, but subsidiary conditions must be required. Implications of Gribov copy effects for lattice calculations of the infrared behaviour of gauge-fixed propagators are discussed. We compute the ghost-gluon vertex and provide a sensible truncation of Dyson-Schwinger equations. Approximations of the variational approach to the 3 + 1 dimensional theory are checked by comparison to the 1 + 1 dimensional case. 相似文献
173.
By using the path integral approach, we investigate the problem of Hooke's atom (two electrons interacting with Coulomb potential in an external harmonic-oscillator potential) in an arbitrary time-dependent electric field. For a certain infinite set of discrete oscillator frequencies, we obtain the analyticalsolutions. The ground state polarization of the atom is then calculated. The same result is also obtained through linear response theory. 相似文献
174.
In this paper, the gluon propagator in Landau gauge has been studied
on a lattice, including the quenched and the unquenched one. The
small geometry size of lattice we use is 163×32, and the
big one is 203×64. For the quenched approximation, we fit
the numerical results and give a little different fitting values. We also obtain unquenched effects by comparing the gluon propagator resulting from the quenched and unquenched configurations, for both the two-flavor and three-flavor cases. For the unquenched
configurations, an obvious quark mass dependence has not been found in
the small quark mass case, but is found in the three-flavor case when the quark mass is big. 相似文献
175.
176.
Claudio N. Cavasotto 《Theoretical chemistry accounts》2000,104(6):491-498
An alternative theoretical approach to the polarization propagator based on a new finite expansion of a finite-dimensional
matrix is presented. The general equations for such an expansion are derived and the validity conditions stated. This method
is used to accomplish an approximate scheme for the self-energy of the particle–hole propagator within the superoperator formalism.
Within this scheme each contribution includes corrections to infinite order in electronic interaction and so describes collective
effects in a natural way. Individual contributions can be interpreted as describing the propagation of the interaction through
a particular subset of electronic excitations. Comparison with other known approximation levels, such as the random-phase
approximation, is also analyzed.
Received: 14 February 2000 / Accepted: 18 April 2000 / Published online: 18 August 2000 相似文献
177.
《Theoretical chemistry accounts》1997,95(5-6):215-241
Using the intermediate hamiltonian theory as a unique conceptual frame and the technique of CI matrix dressing, a wide series
of single-reference methods for the treatment of the ground state correlation are reviewed, compared, and sometimes improved.
These methods range from independent excitation approximation (the very next step beyond MP2) to coupled cluster, going through
the so-called electron pair approximations and the (SC)2CI formalism. A hierarchy of these methods can be established according to two criteria:
1. The physical effects incorporated in the model space, the choice of which is flexible.
2. The quality of the evaluation of the coefficients of the external space determinants. This evaluation, which remains based
on a single reference expansion of the wave function, may simply ensure the size consistency or incorporate the linked contributions
from the outer space.
These formulations in terms of diagonalizations of dressed CI matrices avoid convergence problems, but their main advantage
is their flexibility, since they apply to multi-reference SDCI spaces as well as to SDCI spaces. The use of a common frame
allows one to propose consistent combinations of methods of various costs for the treatment of various parts of the correlation
energy.
Received May 13, 1996/Final version received December 9, 1996/Accepted December 9, 1996 相似文献
178.
We include effects of nonlocal quark condensates into QCD sum rules (QSR) via the Källén–Lehmann representation for a dressed fermion propagator, in which a negative spectral density function manifests their nonperturbative nature. Applying our formalism to the pion form factor as an example, QSR results are in good agreement with data for momentum transfer squared up to Q2≈10 GeV2. It is observed that the nonlocal quark condensate contribution descends like 1/Q2, different from the exponential decrease in Q2 obtained in the literature, and contrary to the linear rise in the local-condensate approximation. 相似文献
179.
采用电弱统一标准模型, 对光子γ和中间玻色子Z0 混合圈链图传播子的构架方式及其重整化问题作了详细分析与讨论, 并完成了有关解析计算, 获得了由参与电弱相互作用的各种混合圈构成的γ和Z0的重整化链图传播子的解析计算结果. 此外, 我们还将此结果应用于高能物理中备受关注的一类轻子反应e+e-→μ+μ-中, 获得了在γ和Z0所构架出的重整化混合圈链图传播中e+e-→μ+μ-反应截面的解析计算结果, 并将本文所获得的这一理论计算结果与实验观测值作了对比分析, 发现本文理论计算结果与实验观测值符合非常好, 并由此也获得了有关辐射修正的重要信息. 本文研究结果也可为探讨一般复杂传播子的理论研究与应用提供某些参考.
关键词:
标准模型
链图传播子
重整化
辐射修正 相似文献
180.
Reverse time migration has drawn great attention in exploration geophysics because it can be used successfully in areas with large structural and velocity complexity. But its computational cost is considerably high. This paper concerns the fast implementation of the optimized separable approximation of the two‐way propagator, which is the most computational expensive step in reverse time migration. On the basis of the low‐rank property of the propagator and the idea of randomized algorithm, a randomized method is introduced for optimized separable approximation‐based one‐step extrapolation. Numerical results of approximating the propagator show that the randomized method is more efficient than the conventional interpolation method. At the same time, numerical experiments of wavefield extrapolation show that the proposed method is much more accurate than the conventional finite‐difference plus pseudo‐spectrum scheme. Copyright © 2014 John Wiley & Sons, Ltd. 相似文献