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双语推荐:非局域对称

利用机械化算法得到了Kaup-Kupershmidt方程的非局域对称、约化,通过解约化方程得到了该方程的一些新的精确解.
In this paper, using the mechanization-method obtained nonlocal symmetry and reduction of the Kaup-Kupershmidt equation and solving the reduction equation, new solutions to the equation are obtained.

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利用变分法和数值计算方法研究了空间调制作用下Bessel型光晶格中玻色-爱因斯坦凝聚体系中孤立子的稳定性,给出了存在随空间周期变化的线性Bessel型光晶格和线性光晶格(原子之间线性相互作用的空间调制)时,各种参数组合下涡旋和涡旋孤立子的稳定性条件.首先,利用圆对称的高斯型试探波函数得出描述体系稳定性参数满足的Euler-Lagrange方程和变分法分析体系稳定性所需要的有效作用势能的表达式.然后,根据有效作用势能是否具有局域最小值判断体系是否具有稳定状态,得出体系具有稳定状态时参数所满足的条件.最后,利用有限差分法求解Gross-Pitaevskii方程验证变分法结果的正确性,所得结果和变分法结果一致.
Using variational and numerical solutions of the mean field Gross-Pitaevskii equation, we investigate the stabilities of nonrotating and vortex solitons in Bessel optical lattice by spatial modulation of the nonlinearity(nonlinear optical lattice). It is demonstrated that there exist the stable matter-wave solitons in a combination of optical lattices with linear Bessel optical lattices and nonlinear optical lattice. Using the time-dependent variational approach, we derive the odinary differential equations for the time evolutions of the width and phase of solitons. Through an effective potential, we obtain the stable criteria for all kinds of combinations of the system parameters. We perform direct numerical simulations to support our analytical results, and find that they are in goog agreement.

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本文通过分析不同几何配置下的偏振拉曼光谱对线性光学晶体的晶格振动模式进行了研究.首先根据因子群分析,将晶体的振动模按晶体对称群的不可约表示进行分类,其次测量了晶体在10-1600 cm-1范围内,不同几何配置下的偏振拉曼光谱,并在此基础上指认了晶体的晶格振动模式.300 cm-1以下的振动峰,归结为晶体的外振动,来自[BiO6],[ZnO4],[BO4]和[BO3]原子基团的平动和转动;300cm-1以上为晶体的内振动,主要与Bi-O,和Zn-O键振动有关.晶体拉曼光谱中最高振动频率达到1407 cm-1,被指认为[BO3]三角形中B-O键的伸缩振动,体现了[BO3]基团中高的电子非局域化程度.
Polarized Raman spectra of single crystal Bi2ZnOB2O6 have been recorded in the spectral range 10-1600 cm-1 at room tem-perature. Factor group analysis was used to obtain the normal modes of vibration of the crystal. The Raman peaks under 300 cm-1 are assigned to external modes, which are related to the rotational and transitional movement of the [BiO6], [ZnO4], [BO4] and [BO3] groups. Compared with the vibrational spectra of the compounds referred, the satisfactory assignment of most of the high-energy modes to vibrations of Bi-O, B-O and Zn-O bonds can be achieved. In particular, the Raman high-frequency peak located at 1407 cm-1 is attributed to the B-O vibration in the [BO3] triangle.

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基于准周期 Fibonacci 序列,提出了一维对称准周期序列固液介质声子晶体。利用传输矩阵法,数值研究了弹性波在其中的透射特性,以及局域谐振模的基本特征。弹性波正入射时,对低序列声子晶体,在声子带隙的中心频率处出现局域谐振模,且在其左右对称地出现两条局域谐振模。在较高序列结构的声子晶体中,仅在中心频率处出现一条局域谐振模。当弹性波斜入射时,声子带隙和谐振模都略微向高频方向移动。弹性波以较大角度斜入射时,只有低频弹性波透射。
On basis of quasi-periodic Fibonacci sequence,a symmetrical quasi-periodic phononic crystal composed of solid and liquid medium was proposed.Propagation of elastic wave in it and its local field resonant modes were investigated numerically with the transfer matrix method.It was shown that for the phononic crystal with lower order sequence,at the central frequency of the phononic band gap,a local field resonant mode appears;then,two local field resonant modes appear symmetrically at the left side and the right one of the central resonant mode;but for symmetrical quasi-periodic phononic crystal with higher order sequence,only there is a local field resonant mode at the central frequency;moreover,for an elastic wave oblique incident,the band gap and resonant modes slowly shift to higher frequency range;the resonant modes in the band gap can act as a super narrow bandwidth filter with multiple channels;for an elastic wave with larger incident angle,the lower frequency elastic wave can prop

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基于Newman的晶场叠模型与微观自旋哈密顿理论,建立了ZnGa2O4:Fe3+晶体材料中磁性离子Fe3+局域结构与其自旋哈密顿(spin-Hamiltonian,SH)参量(包括二阶零场分裂(zero-field splitting,ZFS)参量D,四阶ZFS参量(a-F),Zeeman g因子:g//,g⊥,△g(=g//-g⊥))之间的定量关系.采用以全组态完全对角化方法为理论背景的CFA/MSH(Crystal Filed Analysis/Microscopic Spin Hamiltonian)研究软件,研究了ZnGa2O4:Fe3+材料中磁性离子Fe3+的SH参量与其局域结构的依赖关系.研究表明:对于ZnGa2O4:Fe3+晶体材料,当磁性离子Fe3+的局域结构畸变参数△R=0.0487 nm,△θ=0.192°时,其基态SH参量理论计算结果与实验测量符合很好,进一步表明Fe3+掺入晶体材料后将引起磁性Fe3+离子局域结构的微小畸变,但其仍然保持D3d点群对称局域结构.在此基础上研究分析了SH参量的微观起源,结果表明:ZnGa2O4:Fe3+晶体材料的SH参量主要来源于SO(spin-orbit)磁相互作用机理,来自其他磁相互作用机理(包括SS(spin-spin),SOO(spin-other-orbit),OO(orbit-orbit),SO-SS-SOO-OO)的贡献比较小.
Relations between the spin-Hamiltonian (SH) parameters including the second-order zero-field splitting (ZFS) pa-rameter D,the fourth-order ZFS parameter (a-F ), the Zeeman g-factors: g//, g⊥, ?g(= g//-g⊥) and the structural parameters of ZnGa2O4:Fe3+ crystals have been established by means of the microscopic spin Hamiltonian theory and Newman’s crystal field (CF) superposition model. On the basis of this, the SH parameters for Fe3+ magnetic ions in ZnGa2O4:Fe3+ crystals are investigated theoretically using the CFA/MSH (crystal field analysis/microscopic spin-Hamiltonian) software based on the full configuration complete diagonalization method. It is found that the theoretically calculated parameters including the ZFS parameters D, (a-F ), and the Zeeman g-factors: g//, g⊥, ?g(=g//-g⊥) for ZnGa2O4:Fe3+ crystals are in good agreement with experimental data when taking into account the lattice distortions:?R = 0.0487 nm and ?θ = 0.192?. This investigation reveals that ther

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计算动词元胞网络(CVCN)是一种使用计算动词局域规则的新型元胞计算平台。对于利用语言描述的高级模型来建模人类个体之间的确定与不确定性社会行为,计算动词元胞网络是常成功的模型。由于计算动词理论有丰富的动词规则,因而计算动词元胞网络有多种形式。元胞网络是建模复杂系统的良好载体,将计算动词应用于元胞网络的构建,是解决复杂社会行为可计算化的一个行之有效的方法。计算动词元胞网络把物理语言学植入到元胞网络的局域规则中,从而实现物理信号推理到符号推理的转变。因此只需简单的计算动词局域规则即可建模高级的社会行为。本文提出新型的计算动词元胞网络模式——菱形对称波模式,分为典型性和典型性两类,在除图像处理上有应用,也在农业,电子等领域有着重要的研究价值。
CVCN(Computational Verb Cellular Networks)is a new computational platform using Computational Verb Theory. CVCN is a successful model when modeling unspecified behavior and specified behavior between human by advanced models of language de-scription. Because it has abundant verb rules, CVCN includes many kinds of forms.Cellular network is the perfect carrier when modeling complex systems, and putting Computational Verb Theory into the construction of cellular network is an effective method of making complicated social behavior computable. CVCN plants physical linguistics in the cellular network local rules and realize the transform from physical signal to symbol signal. Therefore, we can use the simple computational verb local rules to model the high-level social behavior. This paper proposed a new CVCV pattern—rhombus symmetrical wave pattern, it includes typical pattern and atypical pattern, and can be used in image processing and agriculture and electronics region.

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利用变分法研究了线性和线性交叉光晶格中偶极玻色-爱因斯坦凝聚(BEC)体系中物质波孤立子的稳定性.选用柱对称高斯型试探波函数,得出参数的Euler-Lagrange方程和体系的有效作用势能,根据有效势能是否具有局域最小值判断体系是否具有稳定孤立子解.结果表明,由于存在接触相互作用的空间调制,在排斥和吸引偶极相互作用下,均能形成稳定的孤立子解.给出了参数空间中存在稳定解的区域和物质波波包宽度随时间的变化曲线.
Stability of a dipolar Bose-Einstein condensate (BEC) soliton in crossed linear and nonlinear optical lattices is investigated using variational approximation. The Euler-Lagrange equations for variational parameters and the effective potential are derived by means of a cylindrically symmetric Gaussian ansatz, while the equilibrium widths are determined by minimization of the effective potential. In the presence of a periodic spatial variation of short-range contact interaction, the localized bound states can exist for both attractive and repulsive dipolar interactions. And the domain of stable dipolar BEC solitons is illustrated in a phase plot of the nonlinearities. Finally, we give the evolution of the variational width for different values of the nonlinearities.

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用三角对称下3d5组态离子的完全能量矩阵方法,通过理论模拟电子顺磁共振EPR谱,研究了Fe3+离子掺杂到石榴石晶体YAG(Y3Al5O12)和LAG(Lu3Al5O12)中形成的络合物离子(FeO6)9-的局域微观结构.结果表明,掺杂体系YAG:Fe3+中络合物离子(FeO6)9-的Fe-O键长R为2.017 4,LAG:Fe3+中络合物离子(FeO6)9-的R为2.029 6,与相应的实验数据吻合.并且YIG(Y3Fe5O12)和Fe2O3光谱数据计算值与实验观测数据也一致.
Using the complete energy matrices of trigonal symmetry for configuration 3d5 ions, the local micro-structures of ( FeO6 ) 9-complex ions in YAG ( Y3 Al5 O12 ) and LAG( Lu3 Al5 O12 ) garnets were investigated .The re-sults show that the Fe-O bond length R of (FeO6)9-complex ion in YAG is 2.017 4 ?, and R for (FeO6)9-com-plex ion in LAG is 2 .029 6?, which is consistent with the corresponding experimental data .Moreover , the present spectra on YIG(Y3Fe5O12) and Fe2O3 are in good agreement with the available experimental data .

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详细介绍并深化了在IBUU输运模型中引入核子的自旋轨道相互作用及其自旋自由度来研究重离子反应的工作。虽然自旋相关的平均场势中时间反演对称项与时间反演不对称项的贡献相反,但依然观察到体系存在局域自旋极化。发现最终的结果由时间反演不对称项决定,可以利用重离子碰撞中自旋向上核子与自旋向下核子的横向差分流来研究介质中自旋轨道相互作用的性质,包括其强度、密度依赖性和同位旋依赖性,而且即使在小体系下该差分流依然不失为自旋轨道相互作用的良好探针。
In this paper, we report and extend our recent work where the nucleon spin-orbit interac-tion and its spin degree of freedom were introduced explicitly for the first time in the isospin-dependent Boltzmann-Uehling-Uhlenbeck transport model for heavy-ion reactions. Despite of the significant can-cellation of the time-even and time-odd spin-related mean-field potentials from the spin-orbit interaction, an appreciable local spin polarization is observed in heavy-ion collisions at intermediate energies be-cause of the dominating role of the time-odd terms. It is also found that the spin up-down differential transverse flow in heavy-ion collisions is a useful probe of the strength, density dependence, and isospin dependence of the in-medium spin-orbit interaction, and its magnitude is still considerable even at smaller systems.

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通过分子动力学模拟(MD),研究在HCP镁中的一个对称倾斜晶界与基面滑移的位错相互作用而激发的变形孪晶,也就是孪晶形核与长大的过程(或者是孪晶界迁移,TBM)。{1121}孪晶在该过程中是最易被激发的孪生模式。一旦这样的孪晶形成了,它们就会不断长大。该种孪晶界迁移是由单纯的原子位置局域调整造成的。在模拟过程中同时也产生了二次孪晶{1122}。该二次孪晶模型的孪晶形核与长大需要克服的能垒与{1121}孪晶不同。同时,二次孪晶的孪晶界迁移过程是通过孪晶界上的锥形滑移而激发的。
Deformation twinning, i.e., twin nucleation and twin growth (or twin boundary migration, TBM) activated by impinged basal slip at a symmetrical tilt grain boundary in HCP Mg, was examined with molecular dynamics (MD) simulations. The results show that the {1 1 21}-type twinning acts as the most preferential mode of twinning. Once such twins are formed, they are almost ready to grow. The TBM of such twins is led by pure atomic shuffling events. A secondary mode of twinning can also occur in our simulations. The {1122} twinning is observed at 10 K as the secondary twin. This secondary mode of twinning shows different energy barriers for nucleation as well as for growth compared with the {1 1 21}-type twining. In particular, TBMs in this case is triggered intrinsically by pyramidal slip at its twin boundary.

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