wave equationfinite element methodlower error bounds on spaces of dataFourier methodThe three-level in time bilinear finite element method with a weight is studied for an initial-boundary value problem for the
2EW Sudakov corrections at one-loop In this section we discuss the structure of one-loop EW corrections in the high-energy limit where the algorithm of Refs. [18,22,23] allows to evaluate such corrections in logarithmic approximation (LA). In the following Sect.3we will discuss the implemen...
the structure of the equations, and the properties of one dimension, we establish the global existence and uniqueness of strong and classical solutions to the initial boundary value problem of compressible Navier–Stokes/Allen–Cahn system in one-dimensional bounded domain with the viscosity depending ...
Wave propagation of phonon and phason displacement modes in quasicrystals: determination of wave parameters J. Appl. Phys., 117 (5) (2015), p. 054905 View in ScopusGoogle Scholar [29] Li X.F. A general solution of elasto-hydrodynamics of two-dimensional quasicrystals Philos. Mag. Lett., 91...
To eliminate this error, one can generalize the approach of Fokinet al.21by assuming that the reflection coefficient depends on the incident wave propagation direction. This is achieved by measuring the reflection and transmission coefficients,RandT, respectively, of a finite length one-dimensional eff...
microscopic space-time satisfies the one dimensional classical wave equation. Next, let us consider Hypothesis Ⅱ. This is the Euler -Lagrangian equation in the microscopic space-time. The L is defined by the macroscopic space-time as follows, ...
The derivation above allows us to write down the effective strong interaction Hamiltonian Heff ¼ EAIM À (1/g)A, where IM is an M-dimensional identity matrix. Heff can be used to study additional perturbations on the system such as external electromagnetic fields in the strongly interacting...
数值算例表明,改进后的方法收敛更快,减少了计算时间且提高了计算精度. 关键词李代数深度积分,横向变速,象征,指数映射,地震波走时 0001—5733.2010.11.022 DOI:10.3969/j.issrL 中图分类号P631 The and in improvement precisionanalysisalgorithm Lie of seismicwave depthintegralone-way algebra ZHANG Lian—Pin91～...
Section 3 contains the general derivation of the linear tensor equation for one component that is equivalent to the Dirac equation. Formulations of the linear tensor equation in terms of antisymmetric second-rank tensors and 3D vectors are provided, respectively, in Sects. 4 and 5. The supplement...
Therefore the coset is just the space SU(2) which is isomorphic to the three dimensional sphere S3. In order to have an explicit effec- tive Lagrangian we need to introduce some particular coordinates on this space that will play the role of the WBGB fields. These three fields must be ...