Far-infrared optical absorption due to surface phonon excitations in small metal particles

In this paper, the role played by the excitation of surface phonons in the far infrared optical absorption of small metallic spheres is explored. We find that for frequencies ranging between 100 cm^-3 and 200 cm^-1 this absorption mechanism is dominating over the ones coming from considering electronic excitations or the Joule heating.     

On the size dependence of the optical absorption due to small metal particles

The quantum mechanical theory of Kawbata and Kubo is used to calculate the position of the Mie optical absorption peak for small silver particles. The calculated position is close to that obtained with a classical model and does not explain the shift to long wavelength experimentally observed.     

Fano-like coupling of collective and particle-hole excitations in Li metal

The dynamic structure factor of Li with [110] and 0.88 a.u. <q< 1.03 a.u., as measured with 1 eV resolution by means of synchrotron radiation based inelastic X-ray scattering spectroscopy (IXSS), exhibits, in the energy loss range between 3 and 12 eV, a fine structure, which appears as a resonance around 4 eV and an antiresonance around 8 eV, when the difference between the experimental -spectra with [110] and [111] is considered. In order to find out the origin of this fine structure we have interpreted recent TLDA (time dependent local density approximation) calculations of the Li- [#!ref12!#], which were based on the inversion of the full dielectric matrix, by utilizing a simple two-plasmon-band model. In this way the fine structure can be traced back to a Fano-like coupling of the discrete collective excitations (both the regular plasmon and the so-called zone-boundary collective states (ZBCS's)) and the particle-hole excitation continuum, mediated by the off-diagonal elements of the dielectric matrix, , where (1,1,0). Received: 29 December 1998 / Accepted: 16 March 1998     

Changes in optical absorption in iron garnet films due to impurity incorporation

The incorporation of impurities in films of Bi-substituted iron garnets grown by liquid phase epitaxy has been studied by successively adding small amounts of SiO₂ and CaCO₃ to the melt before film growth. It is found that very small additions of CaCO₃ to the melt profoundly influences the optical absorption coefficient and the electrical properties. The impurity absorption ofn-type YIG doped with Si⁴⁺ and Pb²⁺ ions is investigated and its wavelength dependence compared to that ofp-type YIG. The optical transitions involved in the impurity absorption of iron garnets are discussed in terms of transition reaction, photon energy and dependence on the impurity concentration. Depending on the photon energy, one or several transitions may give rise to impurity absorption.     

Abnormal optical absorption of quenched Ag films due to surface roughness

The optical properties of rough Ag films quenched on substrates cooled to 150 K are studied by differential reflectivity during annealing to room temperature. An abnormal optical absorption at about 2.5 eV is assigned to surface roughness.     

Nonlinear absorption of ultrashort laser pulses in thin metal films

Self-consistent simulations of the ultrafast electron dynamics in thin metal films were performed. A regime of nonlinear oscillations was observed that corresponds to ballistic electrons bouncing back and forth against the films' surfaces. When an oscillatory laser field is applied to the film, the field energy is partially absorbed by the electron gas. Maximum absorption occurs when the period of the external field matches the period of the nonlinear oscillations, which, for sodium films, lies in the infrared range. Possible experimental implementations are discussed.     

Coherent control of the optical nonlinear and luminescence anisotropies in molecular thin films by multiphoton excitations

Photoinduced orientational distributions are implemented with one- and two-photon absorption interference in polymer films containing chromophores that exhibit luminescent and nonlinear properties. The odd- and even-order parameters of the final distribution are probed by simultaneous measurement of second-harmonic generation (SHG) and two-photon fluorescence (TPF). We show the possibility of engineering local SHG and TPF anisotropies by controlling the polarization states and intensities of the writing optical fields. Complex multipolar orders are modeled with an irreducible spherical tensor-based formalism jointly applied to the molecular polarizabilities and field tensors.     

The role of electron-hole pair excitations in the optical absorption of metals,particularly metal spheres

It is shown that electron-hole pair excitations can dominate the optical absorption of a small metal sphere over the entire frequency range up to the bulk plasma frequency. The limited size has the effect of giving more surface to volume, thereby giving a larger relative weight to the single particle excitations, predominantly produced in the surface region, as compared to the planar case where they make up for a smaller part of the total absorptance.     

从吸收比计算光学薄膜的消光系数

对于弱吸收薄腹,当薄膜和基底的折射率在一定数值范围内时,含有吸收比的公式可以用来计算薄膜的消光系数.该式不能用来计算已经没有干涉效应的厚的强吸收膜的消光系数.     

Magnetic order effect on optical absorption and photoconductivity in EuO thin films

The comparison of optical absorption with photoconductivity with left and right circularly polarized light versus temperature, shows similar behaviours. The transition responsible for photoconductivity has been assigned to a 4f-5d transition. Arguments are proposed to explain the relation between absorption which occurs between the 4f correlated levels and the 5d levels more delocalized and photoconductivity which has the same optical cause but whose electron is delocalized in a conduction band.     

基底对光学薄膜弱吸收测量的影响

对表面热透镜技术测量光学薄膜弱吸收低频调制时不同基底对测量的影响进行了理论分析。用Lambda—900分光光度计测量了K9和石英基底的Ti3O5单层膜的吸收值,将该组样品作为定标片;用表面热透镜装置分别测量了BK7和石英空白基底及HfO2,ZnO两组不同基底不同厚度单层膜样品的吸收。通过分析比较同一工艺条件下镀制的不同基底薄膜样品用与其同种和不同种基底定标片定标测量的结果,表明在低频测量时需要用与测量样品同种基底的定标片定标;不同厚度样品的测量结果表明,在不能严格满足热薄条件时,测量结果需引入修正值。     

基底对光学薄膜弱吸收测量的影响

 对表面热透镜技术测量光学薄膜弱吸收低频调制时不同基底对测量的影响进行了理论分析。用Lambda—900分光光度计测量了K9和石英基底的Ti₃O₅单层膜的吸收值,将该组样品作为定标片;用表面热透镜装置分别测量了BK7和石英空白基底及HfO₂,ZnO两组不同基底不同厚度单层膜样品的吸收。通过分析比较同一工艺条件下镀制的不同基底薄膜样品用与其同种和不同种基底定标片定标测量的结果,表明在低频测量时需要用与测量样品同种基底的定标片定标;不同厚度样品的测量结果表明,在不能严格满足热薄条件时,测量结果需引入修正值。     

Annealing-induced optical and sub-band-gap absorption parameters of Sn-doped CdSe thin films

Thin films of Sn-doped CdSe were prepared by thermal evaporation onto glass substrates in an argon gas atmosphere and annealed at different temperatures. Structural evaluation of the films was carried out using X-ray diffraction and their stoichiometry studied by energy-dispersive X-ray analysis. The films exhibit a preferred orientation along the hexagonal direction of CdSe. The optical transmittance of the films shows a red shift of the absorption edge with annealing. The fundamental absorption edge corresponds to a direct energy gap with a temperature coefficient of 3.34 × 10^?3 eV K^?1. The refractive index, optical conductivity and real and imaginary parts of the dielectric constants were found to increase after annealing. The sub-band gap absorption coefficient was evaluated using the constant photocurrent method. It varies exponentially with photon energy. The Urbach energy, the density of defect states, and the steepness of the density of localized states were evaluated from the sub-band-gap absorption.     

The effect of structural changes on the optical absorption of thin aluminium films

Experimental observations of the variations of optical absorption as a result of annealing thin, vapour-quenched aluminium films and also the dependence on film thickness, are discussed in relation to structural ordering in the films.     

Electromagnetic effect in enhanced infrared absorption of adsorbed molecules on thin metal films

The electric field strength within a homogeneous metal layer on a Ge hemi-cylindrical prism in the Kretschmann configuration has been calculated for infrared light using the Fresnel formula. To approximate the non-homogeneous island-like or porous nature of very thin metal films the dielectric constant of the metal layer was derived by the Bruggeman effective medium approximation. The dependence of the calculated intensity on the film thickness and the angle of incidence is in good agreement with the experimental observations of enhanced infrared absorption of adsorbed species. Combined with the observed short range effect of the enhancement this implies that the enhancement is due to actual high electric fields within the pores or between islands of the metal film which are proportional to the calculated effective field.