A study on electromagnetic wave absorber for the collision-avoidance radar

In this paper, we designed and fabricated the EM wave absorber for eliminating false image and system-to-system interference in a collision-avoidance radar using Permalloy and CPE, the mixing ratio of which was Permalloy:CPE = 70:30 wt%. The EM wave absorption ability was simulated according to different thicknesses of the EM wave absorber using measured permittivity and permeability, and then the EM wave absorber was fabricated based on the simulated design. The simulated results agree well with the measured ones. As a result, we suggest Permalloy for use as a new EM wave absorber in W-band, and the fabricated EM wave absorber with the thickness of 1.4 mm has absorption ability more than 20 dB in frequency range of 76–77 GHz.     

The origin of reflection loss peaks in the double-layer electromagnetic wave absorber

We investigated the origin of reflection loss (RL) peaks of Co₂Z particle composite (t mm)/fake-shaped carbonyl iron (CI) particle composite (1.5 mm) double-layer absorbers backed by a perfect conductor in 0.1–18 GHz. The RL peak frequency in the low frequency region remains unvariable and the RL peak in the high frequency region moves to lower frequency with the increase of Co₂Z particle composite thickness. The investigation results indicated that the two RL peaks come from the quarter-wavelength cancellation at the interface from Co₂Z particle composite to CI particle composite and the interface from air to Co₂Z particle composite, respectively.     

Scattering of a plane electromagnetic wave by bodies of conical shape

Radiophysics and Quantum Electronics -     

Charged particle motion in a medium along an electromagnetic wave

The solution of the relativistic equation of motion is discussed for a charged particle interacting with an electromagnetic wave in a medium.     

Iron based carbon nanocomposites for electromagnetic wave absorber with wide bandwidth in GHz range

The electromagnetic wave absorption properties of resin compacts containing 40 vol. % composite powders of α-Fe/C(a), and Fe₃C/C(a) were characterized in a frequency range of 0.05–26.5 GHz, according to a conventional reflection/transmission technique. The real part (ε_r ^′) and the imaginary part (ε_r ^′′) of relative permittivity were constantly low in the 2–14 GHz (ε_r ^′= ∼12.4 and ε_r ^′′= ∼0.6) for α-Fe/C(a) resin composites, and in the 1–26.5 GHz (ε_r ^′= ∼9.6 and ε_r ^′′= ∼0.8) for Fe₃C/C(a) ones. The imaginary part (μ_r ^′′) of relative permeability exhibited wide peaks in the 1–9 GHz range for α-Fe/C(a), and in the 2–26.5 GHz range for Fe₃C/C(a) owing to their different magnetocrystalline anisotropy field values. Consequently, the resin compacts with 40 vol. % α-Fe/C(a), and Fe₃C/C(a) powders provided good electromagnetic wave absorption performances (reflection loss <-20 dB) in ranges of 4.3–8.2 GHz, and 9–26.5 GHz over absorber thicknesses of 1.8–3.3 mm, and 1.0–2.4 mm, respectively. PACS 76.50.+g; 61.46.+w; 75.50.Bb; 75.30.Gw; 75.20.En     

Scattering of a plane inhomogeneous electromagnetic wave by a spherical particle

We extend an analytical solution for the problem of diffraction of a plane wave by a spherical particle to the case of an inhomogeneous wave. Numerical examples showing a significant change in the scattered-wave structure compared with the case of diffraction of a homogeneous wave are presented. __________ Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Radiofizika, Vol. 49, No. 1, pp. 72–81, January 2006.     

Ponderomotive nongradient force acting on a relativistic particle crossing an inhomogeneous electromagnetic wave

The ponderomotive force acting on a relativistic charged particle crossing an inhomogeneous electromagnetic wave is investigated numerically and analytically. The initial velocity of the particle is perpendicular to the electric field vector of the wave and to the direction of its propagation. The wave has zero gradient in the direction of propagation and is inhomogeneous in both transverse directions. It is shown that the ponderomotive force acting on the particle is parallel to the wave vector. The magnitude of the force is determined not only by the extent of wave inhomogeneity in the direction of the translational motion of particle, but also by its inhomogeneity in the transverse direction. It is found that the trajectory of a particle is determined by the action of ponderomotive forces as well as by its drift in a nonuniform field.     

Bremsstrahlung of a neutral fermi particle in the field of a plane electromagnetic wave

The bremsstrahlung is considered from a neutral Fermi particle with anomalous magnetic and electric moments in the field of a screened Coulomb center and in the presence of a plane electromagnetic wave. The effect of the wave polarization on the scattering cross section and the behavior of the particle spin during the scattering process are considered. Cross sections are given for scattering of a particle at a Coulomb center in the presence of constant, crossed electric and magnetic fields which are equal in magnitude and also for a free particle. It is shown that the effect of the anomalous electric moment is often decisive.     

Thermal effects on laser-ablated particle velocities from thin film targets

The thermal history of the target surface on the plume dynamics was studied by high-speed streak photography. A thin aluminum layer was deposited on a thick substrate material. By choosing substrate materials with different thermal conductivity, it is possible to control the heat flux inside the target material, which in turn controls the particle ejection process. In all the experimental conditions tested, the plume was found to have two different velocity clouds. By a series of experiments with different substrate materials, their velocities were shown to depend on the substrate material. The heat conduction equation was solved to simulate the temperature history of the target materials. The result was discussed with those from streak photography and burn patterns, showing an appreciable dependence on the heat conductivity of the material.     

Effect of the field of a nonlinear electromagnetic wave on the shape of a soliton in a semiconductor superlattice

The effect of the electric component of the field of a high-frequency (HF) nonlinear electromagnetic (EM) wave on the propagation of a solitary EM wave (soliton) in a quantum semiconductor superlattice is studied. It is noted that in the collisionless approximation, the solution of the modified sine-Gordon equation corresponding to the amplification of an EM pulse that, with allowance made for interminiband electron transitions, transforms into a dissipative soliton is possible. The effect of electron collisions with irregularities of the crystal lattice on the soliton dynamics under the action of the field of a HF nonlinear wave is considered. The condition for an increase in the traveling time of the solitary wave is found.     

基于电磁谐振分离的宽带低雷达截面超材料吸波体

基于超材料的电磁谐振特性, 设计、制作了一种极化无关的宽带低雷达散射截面 (radar cross section, RCS)超材料吸波体. 通过场分布和反演法分析了其吸波机理, 利用波导法和空间波法测试了其吸波率和RCS特性. 理论分析表明: 在平面波的作用下, 该吸波体对某一吸波频率在不同的位置分别提供电谐振和磁谐振, 对不同的吸波频率, 利用不同的介质层提供主要的能量损耗, 从而有效减弱了电磁耦合, 保证了宽频带的强吸收特性. 实验结果表明: 设计的三层结构吸波体吸波率达90%以上的带宽是单层结构的4.25倍, RCS减缩10 dB以上的带宽为5.1%, 其单元尺寸为0.17λ, 厚度仅为0.015λ. 该吸波体的低RCS特性还具有极化无关、宽入射角的特点, 且通过改变吸波体的夹层结构可以实现工作带宽的灵活调节. 关键词： 超材料吸波体 雷达散射截面 宽带 电磁谐振     

On the radiation pressure effects of two-dimensional electromagnetic wave packets in fluids

Some characteristic properties of the two-dimensional wave packet propagation across an abrupt plasma-vacuum and dielectric fluid-vacuum boundary are deduced. The momentum left behind the wave packet is found. It is shown, that the momentum localisation and distribution is other and more complicated, than it has been supposed previously.The author thanks R.Klíma for numerous discussions.     

Current density distribution within a small metal particle in an electromagnetic wave field

The eddy current density distribution within a small conducting spherical particle is analyzed in the cases of specular, diffuse, and specular-diffuse interactions of electrons of a metal with the boundary of the sample. The situations with different sizes of particles and different frequencies of incident electromagnetic waves in the absence of the skin effect are considered.     

Anomalous transmission of electromagnetic wave through periodic arrays of subwavelength slits arranged on thin metal films

We study the optical properties of periodic structures, each of which consists of arrays of subwavelength slits in thick films that are placed directly against a continuous thin film. We find that the transmittance of the entire system including the thin film is higher than the transmittance of the isolated thin film alone. Our investigations are performed through numerical simulations with the Fourier modal method.     

Relativistic effects on electromagnetic wave propagation in a cold inhomogeneous electron plasma

We construct a method which permits to investigate the propagation of a travelling wave in different cases. We present the results we obtained in the case of an inhomogeneous plasma taking into account relativistic effects.     

Change in the energy of a charged particle moving in the field of a slow electromagnetic wave

A differential equation is obtained that describes the change in the energy of a charged particle in the field of a slow wave (with phase velocity not equal to unity) as a function of the distance traversed. Analysis of this equation yields the amplitude and period of the change in the particle's energy.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 2, pp. 97–102, February, 1981.     

Diffraction of electrons on the travelling electromagnetic wave

The quantum effect of diffraction scattering of the electron on the travelling electromagnetic wave in the presence of the third body has been found. As the third body, the refracting medium, the division bounds of different mediums or any inhomogenity of it, the atomic nucleus, screens, openings (giving diffraction emission) etc. may appear. The cause of this effect is physically connected with the real absorption and emission of non-vacuum quanta, the concrete mechanism of which is conditioned by the direct and inverse induced Cherenkov, transitional, bremsstrahlung, diffraction effects respectively. Owing to the real absorption-emission the scattering is inelastic, so the diffraction on the travelling wave is accompanied by the acceleration of electrons (one half decelerates).