Specific features of the formation of optical waveguides in silicate glass at high energy and doze of electron irradiation

The formation of an optical waveguide in silicate glass that contains alkali-metal ions is experimentally studied under electron irradiation at an energy of 50 keV and a doze of 25–50 mC/cm². A gradient waveguide with a maximum variation in the refractive index of 0.01–0.04 is formed in the glass due to irradiation. It is demonstrated that a variation in the refractive index results from both field migration of alkalimetal ions to the region of negative space charge and structural modifications in the glass related to the destruction of glass structure by high-energy electrons.     

非聚焦电子束照射SiO2薄膜带电效应

采用考虑电子散射、俘获、输运和自洽场的三维数值模型, 模拟了低能非聚焦电子束照射接地SiO₂薄膜的带电效应. 结果表明, 由于电子的迁移和扩散, 电子会渡越散射区域产生负空间电荷分布. 空间电荷呈现在散射区域内为正, 区域外为负的交替分布特性. 对于薄膜负带电, 电子会输运至导电衬底形成泄漏电流, 其暂态过程随泄漏电流的增加趋于平衡. 而正带电暂态过程随返回二次电子的增多而趋于平衡. 在平衡态时, 负带电表面电位随薄膜厚度、陷阱密度的增大而降低, 随电子迁移率、薄膜介电常数的增大而升高;而正带电表面电位受它们影响较小.     

空间多能电子辐照聚合物充电过程的稳态特性

空间同步轨道上多能电子辐照聚合物的充电过程及其稳态特性是研究和抑制通信卫星静电放电的基础.在同步电子散射-输运微观模型的基础上,采用具有10—400 keV积分能谱分布的多能电子辐照聚酰亚胺样品,进行了多能电子辐照聚酰亚胺充电过程的数值模拟,获得了空间电荷密度、空间电位、空间电场分布和聚合物样品参数条件下的表面电位和最大场强.结果表明,多能电子与样品发生散射作用并沉积在样品内形成具有高密度的电荷区域分布,同时在迁移和扩散的作用下输运至样品底部形成样品电流;充电达到稳态、电子迁移率较小时(小于10-10cm2·V-1·s-1),表面电位绝对值和充电强度随电子迁移率的降低明显加强,捕获密度较大时(大于1014cm-3),表面电位绝对值和充电强度随捕获密度的增大明显加强;聚合物样品厚度对表面电位和充电强度的影响大于电子迁移率、捕获密度和相对介电常数的影响.研究结果对于揭示空间多能电子辐照聚合物的充电现象及微观机理、提高航天器故障机理研究水平具有重要科学意义和价值.     

低能电子束照射接地绝缘薄膜的负带电过程

为揭示低能电子束照射接地绝缘薄膜的负带电过程及其机理,建立了同时考虑电子散射与电子输运的计算模型,综合Monte Carlo方法和有限差分法进行了数值模拟,获得了内部空间电荷、泄漏电流和表面电位随电子束照射的演化规律.结果表明,入射电子因迁移、扩散效应会超越通常的散射区域产生负空间电荷分布,并经过一定的渡越时间后到达接地基板,形成泄漏电流,负带电暂态过程则随着泄漏电流的增加而趋于平衡.在平衡状态下,泄漏电流随电子束能量和电流而增大;薄膜净负电荷量和表面电位随膜厚而增加、随电子迁移率的增大而降低,随着电子束 关键词： 绝缘薄膜 电子束照射 带电效应 数值模拟     

The positive charging effect of dielectric films irradiated by a focused electron beam

Space charge and surface potential profiles are investigated with numerical simulation for dielectric films of SiO₂ positively charged by a focused electron beam. By combining the Monte Carlo method and the finite difference method, the simulation is preformed with a newly developed comprehensive two-dimensional model including electron scattering, charge transport and trapping. Results show that the space charge is distributed positively, like a semi-ellipsoid, within a high-density region of electrons and holes, but negatively outside the region due to electron diffusion along the radial and beam incident directions. Simultaneously, peak positions of the positive and negative space charge densities shift outwards or downwards with electron beam irradiation. The surface potential, along the radial direction, has a nearly flat-top around the center, abruptly decreases to negative values outside the high-density region and finally increases to zero gradually. Influences of electron beam and film parameters on the surface potential profile in the equilibrium state are also shown and analyzed. Furthermore, the variation of secondary electron signal of a large-scale integration sample positively charged in scanning electron microscopic observation is simulated and validated by experiment.     

Surface space charge potential in thin silver halides

An analysis is made of the surface space charge layer in thin silver halides. The proposed model takes into account that the surface sites have a binding energy different from the normal lattice sites. A well defined number of surface sites is introduced in the thin film space charge potential calculations. Numerical computations have been performed for pure films and films doped with divalent ions which are homogeneous distributed on normal lattice sites.     

Release of a diamond-like film on a nickel surface irradiated simultaneously with carbon ions and electrons

Nickel samples at temperatures of 300–1000°C have been irradiated simultaneously with 10-to 30-keV C⁺ ions and 1-to 5-keV electrons. The release of implanted carbon atoms on the surface of a sample with the formation of a transparent carbon film with the prevailing sp ³ hybridization has been observed. The thickness of the film is several tens of nanometers. The formation of films is attributed to the acceleration of the formation of carbon structures in samples irradiated by accelerated electrons.     

Anomalous optical constants of thin films

The explanation of anomalous optical constants in thin chemically distinct layers on substrates offered by Plumb is re-examined and extended. The model invokes the concept of the space charged boundary layer and treats the charge carrier population as a free-electron gas to derive the optical behaviour of thin surface films. The implication of the space charge means that the optical constants of a dielectric film on a metal will vary over a distance directly proportional to the dielectric constant of the film and inversly proportional to the concentration of the electrons at the metal/film interface. Similarly as the temperature increases this space charge region should extend to larger distances from the interface.     

Mechanism of electron beam poled SHG in 0.95GeS2·0.05In2S3 chalcogenide glasses

Utilizing the Maker fringe method, SHG was observed in the 0.95GeS₂·0.05In₂S₃ chalcogenide glass irradiated by the electron beam and the intensity of SH increases with the enhancement of beam current from 15 to 25 nA. According to Raman spectra of the as-prepared and the irradiated one, no distinct micro-structural transformation was found. In this work, the built-in charge model was founded to interpret the poling mechanism of electron beam irradiation, the emission of the secondary electrons and Auger electrons results in the formation of positive region and the absorbed electrons form negative region. The positive region was situated near the poling surface, and the negative region was much deeper than the positive region. Between the two opposite charged regions, a strong space-charge electrostatic field, E_dc, is created, which leads to the nonzero χ⁽²⁾ in the 0.95GeS₂·0.05In₂S₃ glass. The emission of backscattered electrons does no contribution to the formation of E_dc.     

Analyses of ion-exchanged glass optical waveguides by means of secondary ion mass spectroscopy: Condensation of impurity halide ions at the surface

We analyzed the chemical composition of K⁺-exchanged glass optical waveguides (OWGs) by secondary ion mass spectroscopy. Extensive condensation of impurity halide ions took place at the surface of the OWGs in the ion-exchanging and annealing processes. The condensation of Cl ions is likely a cause of the abnormal behavior observed for soda-lime glass OWGs; that is, a guided mode having appeared during the annealing did not disappear even after long annealing. Moreover, it was suggested that a space charge layer was formed at the OWG surfaces owing to the condensation of the halide ions.     

Interfacial electrostatic phenomena in polyimide Langmuir–Blodgett films in electron tunneling devices

Nanometric electrostatic space charges exist at the metal/molecular film interface due to the displacement of excessive electrons from metal to molecular films. As a result, surface potential is built across the films on metal. The distributions of the displaced electrons and the electronic density of states in films can be determined using the surface potential built. The current–voltage characteristic of tunneling device using polyimide Langmuir–Blodgett films is discussed with taking into account the space charge.     

Interaction of ions and electrons with nanoparticles in hydrocarbon combustion plasmas

The interaction of electrons and ions with a polydisperse ensemble of soot nanoparticles during the combustion of hydrocarbon fuels is studied. The dynamics of the particle charging is analyzed. It is shown that, in the initial stage, all the soot particles are charged negatively, the largest particles (100–150 nm) carrying up to 40–50 elementary charges. As time elapses, the negative charge is neutralized and the charge distribution becomes more symmetric. Finally, because of the interaction between ions (electrons) and soot particles, the total concentration of the positive ions becomes higher than that of the negative ones.     

TEM monitoring of silver nanoparticles formation on the surface of lead crystal glass

Silver nanoparticles have been formed on the surface of lead crystal glass by means of (i) ion-exchange of alkaline ions from the glass by Ag⁺ ions from a molten salts bath, and (ii) silica based sol-gel coatings containing silver. All experimental variables concerning both ion-exchange process and sol-gel coatings application were combined and studied as main parameters governing the reduction of Ag⁺ ions to Ag⁰ atoms and further aggregation to form nanosized colloids. The content of thermoreducing agents (arsenic or antimony oxides) in the lead crystal glass was essential to favour the reduction of silver ions to form nanoparticles. Optimal experimental conditions to be used for the obtaining of surface silver nanoparticles were determined. TEM was used as the principal characterisation technique for direct observation of the nanoparticles generated. The size of silver colloids varied in the 20-300 nm range for ion-exchanged samples and in the 10-80 nm range for sol-gel coated samples.     

Electrical characteristics of etched ion-tracks in polyimide filled with silver nanoparticles

Silicon ions, of energy 150?MeV and fluence ～10¹²?ions/cm², were used to register latent tracks in 40?µm thick polyimide samples. Different sizes of tracks were obtained by etching the ion irradiated polyimide samples, in chemical solutions, by varying the temperature and etching period. Silver nanoparticles were diffused into the etched tracks by immersing the polyimide samples in silver solution and then irradiating with 6.5?MeV electrons at different fluences varying from 1?×?10¹⁵ to 5?×?10¹⁵?cm^?2. Results of morphological and elemental analysis, carried out by Scanning Electron Microscopy and Energy Dispersive X-ray. Analysis revealed that the conical tracks could be fully filled with silver nanoparticles at electron fluence of 5?×?10¹⁵?cm^?2. The minimum d. c. resistance of an array of tracks, filled with silver nanoparticles and measured across the polyimide film, was orders of magnitude higher as compared to that of silver wires of equivalent sizes connected in parallel. In addition, these silver nanoparticles filled tracks exhibited rectifying I–V behavior and frequency dependent a. c. resistance, characteristic of metal–polymer nano-composites. Possible mechanisms have been discussed, which can justify the asymmetric current–voltage characteristics in such nano-composites.     

Ionic conductivity in epitaxial AgCl films

The space charge conductance and bulk conductivity of epitaxial {111} and {200} films of AgCl with thickness in the 1-μ range has been measured. Interstitial silver ions predominate in concentration within the space charge layer and in the bulk, but are present in concentration roughly $\text{1}\text{10}$ the concentration present in similar AgBr films. Values of the free energy change required for interstitial formation (0·56 eV) and vacancy formation (0·69 eV) were obtained for generation at the surface sites on a {111} film; similar values are reported for {200} films, although the value depends somewhat on the substrate. The concentration of ionic carriers present in the AgCl thin films is 100–1000 times greater than in bulk single crystals.     

Formation and characteristics of graded-index optical waveguides buried in glass

Low-loss optical waveguides have been prepared through thermally induced ion exchange, where sodium ions in glass are replaced by silver ions from an unstirred silver nitrate melt. The index distributions of the inhomogeneous guides produced in the glass are deduced by analysing the measured mode spectra with the WKB-method. The increase in the refractive index caused by the presence of the silver is found to have a nearly Gaussian form with a peak of about 0.082. The index profile is correlated to the two parameters of the preparation process, the diffusion time and the operating temperature. In a typical case (9 hrs and 221°C) the index takes on its maximum value 2.6 μm below the surface of the glass and one obtains an 8-mode guide with five modes buried within the glass and three modes extending to the air-glass interface.A single-mode guide is formed in less than 5 min. The measurements yield an activation energy for the diffusion of Ag⁺ in glass of 8.4·10⁴J/mole and a diffusion coefficient at 221°C of 0.67·10⁻¹² cm²/s, in good agreement with the experimental results reported by other authors. The present observations suggest that a potential gradient is set up in the glass when silver diffuses into it so that the silver ions drift into the glass with a velocity of about 0.3μm/hr.     

低能电子在外层导电屏蔽的玻璃锥管中的传输

采用新的具有常数锥角的玻璃锥管,并对玻璃锥管进行了外表面导电屏蔽,通过对电子穿越玻璃锥管的二维角分布随时间演化的观测,研究了低能电子与玻璃管相互作用的机制.发现电子穿越完全放电的玻璃锥管时穿透率先下降后平稳,整个过程中角分布中心发生微小移动,但角分布的半高宽几乎保持不变.这与我们之前发表的工作(2016 Acta Phys.Sin.65 204103)不同,这是由于对玻璃锥管进行外表面导电屏蔽会阻止外界不确定的快速充放电的影响,并形成了新的稳定放电通道,有利于实现电子的稳定穿透.电子的穿透率随倾角呈类似矩形的分布,透射电子的角分布中心伴随倾角的变化而移动,其穿透所容许的倾角与几何穿透一致.     

Effect of residual atmospheric pressure on the development of electrostatic discharges at the surface of protective glasses of solar cells

Electrostatic discharges obtained upon the irradiation of K-208 glass with 40-keV electrons at a flux density φ of 10¹⁰ to 2 × 10¹¹ cm^–2 s^–1 are studied. The residual pressure p _v in the vacuum chamber is varied from 5 × 10^–5 to 5 × 10^–3 Pa. Structural changes in the sample surfaces are studied by atomic-force microscopy. Depending on the pressure level, two types of discharges are observed in experiments at 3 × 10¹⁰ ≤ φ ≤ 1.2 × 10¹¹ cm^–2 s^–1: a microprojection at the glass–ionized-residual-atmosphere surface and a discharge which develops along the irradiated surface. It is found that at 5 × 10^–5 ≤ p _v ≤ 3 × 10^–4 Pa and 8 × 10¹⁰ ≤ φ ≤ 10¹¹ cm^–2 s^–1, discharges of the first type appear at the beginning of exposure; that is, an increase in microprojections is observed. Further, surface discharges propagate through these microprojections. At 10^–3 ≤ p _v ≤ 5 × 10^–3 Pa and 10¹⁰ ≤ φ ≤ 5 × 10¹⁰ cm^–2 s^–1, on the contrary, discharges of the second type are realized at the beginning. These discharges result in the appearance of channels with inhomogeneities on the glass, at which subsequently discharges of the first type occur. It is determined by calculations that in the region adjacent to the exposed glass surface, secondary electrons accelerated in a field of charge accumulated in the glass make the main contribution to the ionization of gases.     

Specific features of thermal dissolution of silver and gold thin films in silicate glass

It has been shown experimentally that the thermal dissolution of silver and gold thin films in silicate glass is accompanied by the formation of a monolayer of silver and gold micro- and nanocrystals, respectively, on the surface of the glass. These processes occur at temperatures well below the melting temperature of the metal. Microcrystals are formed predominantly at the edges of islands of the metal film, where there is a sufficient amount of the material for their growth. Silver and gold nanocrystals are formed in the case when atoms of the metal dissolved in the glass repeatedly emerge on the glass surface. Silver and gold dissolved in the glass exist not only in the form of atoms and ions but also in the form of charged and neutral molecular clusters.

     

Photon emission under bombardment of ruby by ions and electrons of medium energies

The characteristics of optical radiation produced under bombardment by ions (1–15 keV) and electrons (100–1000 eV) of a ruby surface are studied. Two broad bands with maxima at 330 and 450 nm attributed to defects of the crystal lattice are discovered in the spectral region of 200 to 800 nm. Characteristic radiation related to radiative relaxation of excited Cr³⁺ ions in the near-surface region of the crystal is observed. The dependence of the radiation intensity on the energy and current density of the bombarding particles is obtained experimentally. The degree of radiation polarization is determined.