质点弹簧系统的振动（Ⅱ）

质点弹簧系统的振动（Ⅱ）陈代绶，陈世红（成都治金管理干部学院成都６１００８１）（成都理工学院成都）对于本刊９４年第２期刊载的《质点弹簧系统的振动》一文，有的读者认为：既然系统中存在不同频率、不同阶次的振动，那末各阶振动应相互影响，能量彼此交混，因此只...     

磁膜畴壁蠕移的频率特性

本文叙述难向交变场频率（５０ｃ／ｓ－２００ Ｍｃ／ｓ）对坡莫会金磁膜中畴壁蠕移的影响（即蠕移频谱）的实验结果．实验发现蠕移频谱上有三个峰出现,即１１０－１４０ Ｍｃ／ｓ的高频峰,３０－４０Ｍｃ／ｓ的中频峰和 １００ ｋｃ／ｓ的低频峰．并测定了磁膜厚度、难向直流偏场对蠕移频谱的影响．对壁线运动和与之伴随产生的暂态逸散场的初浅的理论分析表明：（１）壁线运动的暂态逸散场是导致畴壁蠕移的一个原因;（２）壁线运动有共振特征,蠕移频谱上的高频峰和中频峰的出现分别是９０°线（或Ｎｅｅｌ线）和Ｂｌｏｃｈ线共振的反映;（３）低频下的蠕移不是壁线运动的暂态逸散场引起,而可能是由Ｎｅｅｌ壁段的某种作用所导致．     

太赫兹波段谐振频率可调的开口谐振环结构

开口谐振环(SRRs) 结构可以激励磁谐振, 实现负的磁导率. 提出在SRRs两环间隙内引入相对交错的金属短线, 并研究了金属短线对谐振频率的影响. 结果表明: 随着金属短线数目的增多, 谐振频率显著降低, 同时金属短线的结构参数如长度、宽度及间距也会对谐振频率产生影响. 最后验证了金属短线的引入对减小器件尺寸有明显作用, 且不因介质基底的存在而受到影响. 新型磁谐振单元可为今后超材料的设计及实际应用提供新的参考. 关键词： 左手材料 开口谐振环 太赫兹 小型化     

空气介质阻挡放电单个微放电通道发光强度及振动激发温度的空间分布

通过清洗放电方法,在平行平板介质阻挡空气放电中得到了单个稳定的微放电通道（又称放电丝）.测量了从瞬时阳极到瞬时阴极单个放电丝的发光强度及振动激发温度的空间分布.研究表明：在外加电压的每半周中放电丝发光呈现杯型分布,杯底位于瞬时阴极处;振动温度在两平行板间隙的中心处最高而在瞬时阳极处最低. 关键词： 介质阻挡放电 微放电通道 振动温度     

在一维均匀铁磁链中磁振动的内禀局域模

利用多标度方法和准离散近似,我们考察了在一维均匀铁磁链中磁振动的内禀局域模; 结果表明磁振动的内禀局域模在许多方面都与晶格振动的内禀局域模相类似;它们是近邻自旋之间非线性相互作用的结果.这种内禀局域模的存在并没有破坏系统的平移对称性,它们能在任何晶格位被激发.它们的量子本征频率在简谐磁振动频带的上方.     

L波段双频磁绝缘线振荡器的设计与粒子模拟

 提出了利用角向分区来产生双频高功率微波的思想,并根据常规磁绝缘线振荡器的互作用主要在轴向而与角向无关的物理机制,通过在常规磁绝缘线振荡器内设置谐振腔深度的角向分区,建立了L波段双频磁绝缘线振荡器的模型,并利用电磁模拟软件,优化设计了L波段双频磁绝缘线振荡器。粒子模拟的结果为：在电子束电压为530 kV,电流为45.5 kA的条件下,得到了稳定的双频高功率微波输出,其微波频率分别为1.28 GHz和1.50 GHz,周期平均功率约为2.65 GW,功率效率约为11%,两个频率的频谱幅度相差约0.4 dB。     

弦振动实验装置的改进

弦振动实验装置的改进郑稷（重庆师范专科学校６３２１６８）弦振动实验是力学实验中一个重要而典型的实验．该实验的主要内容是研究弦振动的基频与弦长（其他条件不变）和基频与张力（其他条件不变）的关系．实验方法有两种：（１）采用振动频率固定的振动体，通过改变弦...     

一种大功率梳状谱微波产生方法

梳状谱微波通常指具有中心频率，频谱分布与梳子形状相似，在一定带宽内多个频点具有能量分布的电磁波。梳状谱微波在电子对抗方面具有其它对抗方式所不具备的独特优势，在通信对抗、雷达对抗等领域显现出了极好的应用前景。该文介绍了一种大功率梳状谱微波产生方法，利用路径编码脉冲压缩技术将宽带连续波源产生的微波进行压缩，获得了中心频率2.85 GHz、频带宽度1 GHz、频谱间隙250 kHz、峰值功率160 kW的梳状谱微波。后续实验进一步表明，利用该方法获取的梳状谱微波的中心频率、频带宽度、频谱间隙都是灵活可调的，能够应用在多种电子对抗场景当中提升对抗干扰能力。     

TinLa（n=1—7）的密度泛函研究

采用密度泛函理论（B3LYP）和LANL2DZ基组,对Ti_n和Ti_nLa（n=1—7）的各种异构体进行优化,并计算了它们的振动频率和电子结构特征.通过分析掺杂La原子前后团簇的平均键长、对称性、束缚能、能级间隙和磁矩,讨论了La原子引起Ti_n（n=1—7）团簇各种性质的变化及其产生机理. 关键词： 密度泛函 基态结构 稳定性 磁矩     

Curie温度附近稀磁半导体(Ga,Mn)As的电学噪声谱性质

建立了自发噪声谱测量系统来研究稀磁半导体（Ga,Mn）As的电学噪声性质.通过测量（Ga,Mn）As材料的自发噪声谱,发现（Ga,Mn）As的自发涨落会随温度升高而逐渐增大,同时,外加磁场会降低（Ga,Mn）As的自发涨落,这来源于外加磁场导致的（Ga,Mn）As磁畴部分有序化.此外,不同频率的噪声随温度的变化规律有很大差异：当频率低于30 kHz的时候,噪声谱和温度的变化关系和热噪声很相似,但数值上明显大于热噪声的值;当频率在30 kHz左右的时候,噪声大小和温度成线性关系;当频率大于30 kHz以后,在相变点附近噪声大小和温度的关系出现了明显的转折,高频高温噪声的大小和热噪声的理论值非常接近.这些结果有助于深入理解（Ga,Mn）As磁性起源的物理机制. 关键词： 自旋电子学 稀磁半导体 自发涨落谱     

Coupled Band Gap Solitons in One-Dimensional Alternating Heisenberg Ferromagnetic Chains

The dynamics of coupled band gap solitons in one-dimensional Heisenberg ferromagnetic chains with bond alternation is considered analytically. Using the method of multiple scales the nonlinear coupled-mode equations (i.e.Manakov equations) for the upper cutoff mode of acoustic band and the lower cutoff mode of optical band are derived under the quasi-discreteness approximation. Due to the cross-phase modulation the type of soliton excitations may be changed and the vibrating frequencies of these soliton excitations may locate within or outside the gap of magnon frequency bands.``     

Coupled Band Gap Solitons in One-Dimensional Alternating Heisenberg Ferromagnetic Chains

The dynamics of coupled band gap solitons in one-dimensional Heisenberg ferromagnetic chains with bond alternation is considered analytically. Using the method of multiple scales the nonlinear coupled-mode equations (i.e. Manakov equations) for the upper cutoff mode of acoustic band and the lower cutoff mode of optical band are derived under the quasi-discreteness approximation. Due to the cross-phase modulation the type of soliton excitations may be changed and the vibrating frequencies of these soliton excitations may locate within or outside the gap of magnon frequency bands.     

Frequency in Middle of Magnon Band Gap in a Layered Ferromagnetic Superlattice

The frequency in middle of magnon energy band in a five-layer ferromagnetic superlattice is studied by using the linear spin-wave approach and Green＇s function technique. It is found that four energy gaps and corresponding four frequencie in middle of energy gaps exist in the magnon band along Kx direction perpendicular to the superlattice plane. The spin quantum numbers and the interlayer exchange couplings all affect the four frequencies in middle of the energy gaps. When all interlayer exchange couplings are same, the effect of spin quantum numbers on the frequency wg1 in middle of the energy gap Δw12 is complicated, and the frequency wg1 depends on the match of spin quantum numbers in each layer. Meanwhile, the frequencies wg2, wg3, and wg4 in middle of other energy gaps increase monotonously with increasing spin quantum numbers. When the spin quantum numbers in each layer are same, the frequencies wg1, wg2, wg3, and wg4 all increase monotonously with increasing interlayer exchange couplings.     

Frequency in Middle of Magnon Band Gap in a Layered Ferromagnetic Superlattice

The frequency in middle of magnon energy band in a five-layer ferromagnetic superlattice is studied by using the linear spin-wave approach and Green's function technique. It is found that four energy gaps and corresponding four frequencie in middle of energy gaps exist in the magnon band along K_x direction perpendicular to the superlattice plane. The spin quantum numbersand the interlayer exchange couplings all affect the four frequencies in middle of the energy gaps. When all interlayer exchange couplings are same, the effect of spin quantum numbers on the frequency ω_g1 in middle of the energy gap Δω₁₂ is complicated, and the frequency ω_g1 depends on the match of spin quantum numbers in each layer. Meanwhile, the frequencies ω_g2, ω_g3, and ω_g4 in middle of other energy gaps increase monotonously with increasing spin quantum numbers. When the spin quantum numbersin each layer are same, the frequencies ω_g1, ω_g2, ω_g3, and ω_g4 all increasemonotonously with increasing interlayer exchange couplings.     

Magnon energy gap in a four-layer ferromagnetic superlattice

The magnon energy band in a four-layer ferromagnetic superlattice is studied by using the linear spin-wave approach and Green＇s function technique. It is found that three modulated energy gaps exist in the magnon energy band along Kx direction perpendicular to the superlattice plane. The spin quantum numbers and the interlayer exchange couplings all affect the three energy gaps. The magnon energy gaps of the four-layer ferromagnetic superlattice are different from those of the three-layer one. For the four-layer ferromagnetic superlattice, the disappearance of the magnon energy gaps △ω12, △ω23 and △ω34 all correlates with the symmetry of this system. The zero energy gap △ω23 correlates with the symmetry of interlayer exchange couplings, while the vanishing of the magnon energy gaps △ω12 and △ω34 corresponds to a translational symmetry of x-direction in the lattice. When the parameters of the system deviate from these symmetries, the three energy gaps will increase.     

Intrinsic Localized Spin-Wave Modes in an Anisotropic Ferromagnet with Dzyaloshinsky-Moriya Interaction

The existence and properties of intrinsic localized spin-wave modes in a ferromagnetic XXZ spin chain with Dzyaloshinsky-Moriya interaction are investigated analytically in the semiclassical limit. The model Hamiltonian is quantized by introducing the Dyson-Maleev transformation and the coherent state representation is chosen as the basic representation of the system. By making use of the method of multiple scales combined with a quasidiscreteness approximation, the equation of motion for the coherent-state amplitude is reduced to the nonlinear Schrödinger equation. It is shown that a bright intrinsic localized spin-wave mode whose eigenfrequency lies below the bottom of the magnon frequency band can exist in the ferromagnetic system. We also show that the system can produce a dark intrinsic localized spin-wave mode, i.e., nonpropagating kink, whose eigenfrequency is below the upper of the magnon frequency band. In addition, we find that the introduction of the Dzyaloshinsky-Moriya interaction changes wave numbers in the Brillouin-zone corresponding to the appearance of intrinsic localized spin-wave modes.     

High-frequency susceptibility of a superlattice with 2D inhomogeneities

We investigate the high-frequency susceptibility (Green function) of an initially sinusoidal 1D superlattice with 2D phase inhomogeneities that model the deformations of the interfaces between the superlattice layers. For waves propagating along the superlattice axis (the geometry of a photon or magnon crystal), we have found a peculiar behavior of the imaginary part of the Green function that consists in a significant difference between the peaks corresponding to the edges of the band gap in the wave spectrum. The peak corresponding to the lower-frequency band edge remains essentially unchanged as the root-mean-square fluctuation of the 2D inhomogeneities γ₂ increases, while the peak corresponding to the higher-frequency band edge broaden and decreases sharply in height until its complete disappearance with increasing γ₂. This behavior of the peaks corresponds to a band gap closure mechanism that differs from the traditional one characteristic of 1D and 3D inhomogeneities. These effects can be explained by a peculiarity of the energy conservation laws for the incident and scattered waves for 2D inhomogeneities in a 1D superlattice.     

光脉冲在一维负折射材料光子晶体中的传播

讨论了一维负折射光子晶体对光脉冲传播的影响.通过对光脉冲的透射场强的数值计算发现，频谱处于一维负折射率材料光子晶体禁带中的短脉冲通过光子晶体后基本保持形状不变，而对同样的短脉冲通过传统的一维光子晶体的透射脉冲则出现严重畸变.当考虑负折射率材料的色散时，讨论了位相时间随光脉冲载波频率的变化情况.     

Four-magnon relaxation in the itinerant electron ferromagnetics

The concept of an effective magnon Hamiltonian is used to study magnon relaxation inthe band model of ferromagnetism. The 4-magnon processes of electrostatic and magnetic dipolar origin in a narrow single band are discussed.     

Temperature evolution of spin-polaron in-gap states in undoped antiferromagnetic cuprates

The temperature evolution of in-gap states created by the spin polaron effect and located within the gap with charge transfer between the valence and conduction bands is studied for the case of strong electron correlations using the t-t′-t″-J model of antiferromagnetic undoped cuprates. The effect of temperature is taken into account by temperature renormalization of the magnon concentration, which is calculated using the Heisenberg model with inclusion of weak interlayer exchange and weak in-plane spin anisotropy, and by introducing a Lorentzian with a temperature-dependent half-width in the form corresponding to the marginal Fermi liquid model. With increasing temperature, the spectral weight of the in-gap state, which is proportional to the magnon concentration, grows leading to an increased intensity of the corresponding peak of the spectral function in all points of the Brillouin zone. At points (π/2, π/2) and (π, 0), the main peak is approached by the satellite peak related to the in-gap band and, at points (0, 0) and (π, π), the peaks move away from each other.