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961.
在考虑海床表面附近黏性边界层的影响下, 考察了波浪与弹性多孔海床之间的相互作用.波浪场包括势流部分和边界层部分,海床域控制方程由比奥固结理论给出.波浪场和海床域通过交界面处应力连续和速度连续条件进行耦合.在简谐波和小变形的前提下,通过联立求解势流方程、波浪边界层方程和海床准静态比奥固结方程得到了波浪运动及相应的海床动力响应的解析解.通过与以往文献的实验结果进行对比,解析解的合理性得到了验证.通过参数分析讨论了实际问题中需要考虑波浪和海床相互作用机制的海床土质条件,以及流体黏性对波能衰减的影响规律. 相似文献
962.
963.
B. Dóra A. Virosztek 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,22(2):167-178
We consider the possibility of formation of an unconventional spin density wave (USDW) in quasi-one-dimensional electronic
systems. In analogy with unconventional superconductivity, we develop a mean field theory of SDW allowing for the momentum
dependent gap Δ() on the Fermi surface. Conditions for the appearance of such a low temperature phase are investigated. The excitation spectrum
and basic thermodynamic properties of the model are found to be very similar to those of d-wave superconductors in spite of the different topology of their Fermi surfaces. Several correlation functions are calculated,
and the frequency dependent conductivity is evaluated for various gap functions. The latter is found to reflect the maximum
gap value, however with no sharp onset for absorbtion.
Received 19 February 2001 相似文献
964.
D. Karevski Y-C. Lin H. Rieger N. Kawashima F. Iglói 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,20(2):267-276
We study the critical behavior of Ising quantum magnets with broadly distributed random couplings (J), such that P(ln J) ∼ | ln J|-1 - α, α > 1, for large | ln J| (Lévy flight statistics). For sufficiently broad distributions, α < , the critical behavior is controlled by a line of fixed points, where the critical exponents vary with the Lévy index, α.
In one dimension, with = 2, we obtained several exact results through a mapping to surviving Riemann walks. In two dimensions the varying critical
exponents have been calculated by a numerical implementation of the Ma-Dasgupta-Hu renormalization group method leading to
≈ 4.5. Thus in the region 2 < α < , where the central limit theorem holds for | ln J| the broadness of the distribution is relevant for the 2d quantum Ising model.
Received 6 December 2000 and Received in final form 22 January 2001 相似文献
965.
Recent observation and theoretical investigations have led to the significance of electrostatic ion cyclotron (EIC) waves
in the electrodynamics of acceleration process. The instability is one of the fundamental of a current carrying magnetized
plasma. The EIC instability has the lowest threshold current among the current driven instabilities. On the basis of local
analysis where inhomogeneities like the magnetic shear and the finite width current channel, have been ignored which is prevalent
in the magnetospheric environment. On the basis of non-local analysis interesting modification has been incorporated by the
inclusion of magnetic shear. In this paper we provide an analytical approach for the non-local treatment of current driven
electrostatic waves in presence of parallel electric field. The growth rate is significantly influenced by the field aligned
electron drift. The presence of electric field enhances the growth of EIC waves while magnetic shear stabilizes the system. 相似文献
966.
In a two-fluid system where the lower fluid is bounded below by a rigid bottom and the upper fluid is bounded above by a free surface, two kinds of solitary waves can propagate along the interface and the free surface: classical solitary waves characterized by a solitary pulse or generalized solitary waves with nondecaying oscillations in their tails in addition to the solitary pulse. The classical solitary waves move faster than the generalized solitary waves. The origin of the nonlocal solitary waves can be understood from a physical point of view. The dispersion relation for the above system shows that short waves can propagate at the same speed as a “slow” solitary wave. The interaction between the solitary wave and the short waves creates a nonlocal solitary wave. In this paper, the interfacial-wave problem is reduced to a system of ordinary differential equations by using a classical perturbation method, which takes into consideration the possible resonance between short waves and “slow” solitary waves. In the past, classical Korteweg–de Vries type models have been derived but cannot deal with the resonance. All solutions of the new system of model equations, including classical as well as generalized solitary waves, are constructed. The domain of validity of the model is discussed as well. It is also shown that fronts connecting two conjugate states cannot occur for “fast” waves. For “slow” waves, fronts exist but they have ripples in their tails. 相似文献
967.
The noncollinear interaction of guided optical waves with magnetostatic waves under inclined bias magnetic field is theoretically studied in detail. Similar approach can also be applied to the collinear interaction. Calculation results indicate that the diffraction efficiency (DE) in magnitude is equal to the mode-conversion efficiency (MCE) under vertical bias magnetic field, but they differ greatly under inclined bias magnetic field. By comparison to the case of vertical magnetization, the DE or the MCE can be greatly increased under inclined magnetic field. The characteristic of the DE curves obtained is basically in agreement with the experimental result.`` 相似文献
968.
Jean Ndzié Ewodo 《Journal of statistical physics》2001,104(5-6):1253-1272
In this paper, we study the propagation of acoustic waves in a layered random medium. Using the time-reversed method, we prove the space-time refocusing effect and the stabilization for acoustic signals. This work is a generalization of ref. 4 and 7 in the three-dimensional case. 相似文献
969.
Yusry O. El-Dib 《Nonlinear dynamics》2001,24(4):399-418
A rigorous mathematical reduction of the procedure widely usedfor studying a class of the nonlinear problems with perturbations,namely the method of the multiple scales, is used. A profound analysis,which provides an approach for deriving a coupled nonlinearSchrödinger equations. The investigation has been achieved byperturbing the nonlinear dynamical system about the linear dynamicalproblem. Modulated wavetrains are described to all orders ofapproximation. Moreover, we extend our approach to deal with equationshaving periodic terms. Two types of simultaneous nonlinearSchrödinger equations are derived. One type is valid at thenon-parametric system and the second type represents a modification forthe first type which is governed the non-resonance case. Two parametriccoupled nonlinear Schrödeinger equations are derived to govern thesecond-sub-harmonic resonance. In addition other two coupled equationsare found for the third-sub-harmonic resonance case. These systems ofequations control the stability behavior at the parametric resonancecases. The stability criteria for the several types of coupled nonlinearSchrödinger equations are studied. These criteria are achieved by atemporal periodic perturbation. 相似文献
970.