Optical Fabry–Perot filter based on photonic band gap quasi-periodic one-dimensional multilayer according to the definite Rudin–Shapiro distribution

In this work, a new type of optical filter using photonic band gap materials has been suggested. Indeed, a combination of periodic H(LH)^J and Rudin–Shapiro quasi-periodic one-dimensional photonic multilayer systems (RSM) were used. SiO₂ (L) and TiO₂ (H) were chosen as two elementary layers with refractive indexes n_L = 1.45 and n_H = 2.30 respectively. The study configuration is H(LH)^J[RSM]^PH(LH)^J, which forms an effective Fabry–Perot filter (FPF), where J and P are respectively the repetition number of periodic and (RSM) stacks. We have numerically investigated by means of transfer-matrix approach the transmission properties in the visible spectral range of FPF system. We show that the number and position of resonator peaks are dependent on the (RSM) repetition number P and incidence angle of exciting light. The effect of these two parameters for producing an improved polychromatic filter with high finesse coefficient (F) and quality factor (Q) is studied in details.     

VUV spectroscopy of Ce<Superscript>3+</Superscript>-doped Na<Subscript>0.4</Subscript>Lu<Subscript>0.6</Subscript>F<Subscript>2.2</Subscript> single crystals

The short-wave transmission spectrum of Na_0.4Lu_0.6F_2.2 with the visible/ultraviolet transmission edge of 8 eV was studied. Absorption spectra of the 4f—5d transitions of the Ce³⁺ ion in the region of 4–8 eV were studied in Ce³⁺-doped Na_0.4Lu_0.6F_2.2 single crystals. Luminescence spectra in the ultraviolet and visible spectral regions, luminescence decay kinetics and reflection and luminescence excitation spectra in the visible/ultraviolet and ultraviolet regions (4–20 eV) were investigated at helium and room temperatures.     

Multilayer structures with optical characteristics controlled by a magnetic field

The consideration of the gyromagnetic properties of multilayer structures with one or more magnetically active components shows that the application of a magnetic field to such structures imparts magnetically controlled optical properties to them. The effect of a magnetic field on the reflection coefficient of the multilayer structures manifests itself in two phenomena: a shift of the maximum of the spectral curve of the resonant reflection coefficient and a change (increase or decrease) in the bandwidth of this curve. The more pronounced of these two effects is the change in the bandwidth of the spectral curve of the reflection coefficient. The orientation (transverse or longitudinal) of the magnetic field applied to the multilayer structure determines important specific features of these effects. Calculation performed for two types of multilayer structures (Y₃Fe₅O₁₂?Gd₃Ga₅O₁₂ and Y₃Fe₅O₁₂?SiO₂) shows the possibility of their practical use, for example, in fiber optics.     

Spectroscopic properties of Pr:KY(MoO4)2 crystal as a visible laser gain medium

A Pr³⁺-doped KY(MoO₄)₂ single crystal was grown by the Czochralski method. The polarized absorption and fluorescence spectra of the Pr³⁺:KY(MoO₄)₂ crystal were measured at room temperature. The stimulated emission cross-sections for the transitions from the ³P₀ multiplet were estimated from the fluorescence spectra. The fluorescence lifetime of the ³P₀ multiplet was estimated from the fluorescence decay curve at room temperature. The analysis of spectral properties shows that the Pr³⁺:KY(MoO₄)₂ crystal is a promising gain medium for visible lasers.     

Investigation on preparation and physical properties of nanocrystalline Si/SiO2 superlattices for Si-based light-emitting devices

Structures containing silicon nanocrystals (nc-Si) are very promising for Si-based light-emitting devices. Using a technology compatible with that of silicon, a broader wavelength range of the emitted photoluminescence (PL) was obtained with nc-Si/SiO₂ multilayer structures. The main characteristic of these structures is that both layers are light emitters. In this study we report results on a series of nc-Si/SiO₂ multilayer periods deposited on 200 nm thermal oxide SiO₂/Si substrate. Each period contains around 10 nm silicon thin films obtained by low-pressure chemical vapour deposition at T=625°C and 100 nmSiO₂ obtained by atmospheric pressure chemical vapour deposition T=400°C. Optical and microstructural properties of the multilayer structures have been studied by spectroscopic ellipsometry (using the Bruggemann effective medium approximation model for multilayer and multicomponent films), FTIR and UV–visible reflectance spectroscopy. IR spectroscopy revealed the presence of SiO_x structural entities in each nc-Si/SiO₂ interface. Investigation of the PL spectra (using continuous wave-CW 325 nm and pulsed 266 nm laser excitation) has shown several peaks at 1.7, 2, 2.3, 2.7, 3.2 and 3.7 eV, associated with the PL centres in SiO₂, nc-Si and Si–SiO₂ interface. Their contribution to the PL spectra depends on the number of layers in the stack.     

Electronic and electronic-vibrational phenomena in the new organic conductor ϰ-(ET)2[Hg(SCN)2Cl] with a metal-insulator transition

The reflection spectra and optical conductivity spectra of the new organic conductor ϰ-(ET)₂[Hg(SCN)₂Cl] with a metal-insulator transition in the spectral regions 700–5500 and 9000–40 000 cm⁻¹ have been studied in polarized light at 300 K. A comparisonis made between the spectra obtained and the corresponding spectra of related isostructural conductors based on the ET molecule, and also the properties of the crystal structure of the investigated compounds. An electronic transition between the ET molecules of the dimer (ET) ₂ ⁺ in the spectral region 700–5500 cm⁻¹ has been identified, as have the features of the electronic-vibrational structure arising as a consequence of the interaction of this transition with the completely symmetric intramolecular vibrations of the ET molecule. It is found that the conductor with the stronger dimer interaction between the ET molecules has the higher the transition temperature. Fiz. Tverd. Tela (St. Petersburg) 39, 1313–1319 (August 1997)     

Nanosized multilayer films with concurrent photochromism and electrochromism based on Dawson-type polyoxometalate

An inorganic-organic composite multilayer film constructed of poly(vinyl alcohol) (PVA) with Dawson-type phosphotungstate anion [P₂W₁₈O₆₂]⁶⁻ (P₂W₁₈) and poly(allylamine hydrochloride) (PAH) were fabricated on quartz, ITO, silicon and CaF₂ substrates by a layer-by-layer self-assembly method. The film was provided with concurrent photochromism and electrochromism. IR spectra showed that the structure of the PVA was fully maintained in the multilayer film. And their photochromic and electrochromic properties were investigated by UV-vis spectra, cyclic voltammetry (CV), chronoamperometry (CA) measurement and X-ray photoelectron spectra (XPS). Atomic force microscopy (AFM) was used to investigate the surface topography. This study provides a new route to explore the possibility of application to polyoxometalate-based hybrid inorganic-organic materials.     

Amplitude-phase reflectance spectra of amorphous silicon-based Bragg structures

Amplitude-phase spectra of light reflection from distributed Bragg reflectors and Fabry-Pérot microcavities based on a-Si: H/a-SiO_x: H thin films have been studied. The frequency dependence of the phase difference between the amplitude p-and s-light reflection coefficients within the photonic band gap is measured. The phase spectrum exhibits predominantly a monotonic, close-to-linear frequency behavior, except for spectral regions near the stop band edges and near the singularities related to the microcavity eigenmodes. The experimental spectra are compared with theoretical calculations based on the transfer matrix method and approximate analytical relations. A method based on analyzing amplitude-phase reflectance spectra is proposed for structural characterization of multilayer microcavity systems.     

Visible-light photochromism of phosphomolybdic acid and polyvinyl alcohol by inorganic-organic nanocomposite multilayer films

A novel visible-light photochromic inorganic-organic multilayer was constructed based on phosphomolybdic acid (PMoA) and polyvinyl alcohol (PVA) which was prepared using the layer-by-layer (LbL) assembly technique to form the multilayer film. The structures of the multilayer films were characterized via Fourier transform infrared spectra (FT-IR) and atomic force microscopy (AFM). The grown process, internal interaction, the surface topography and photochromic properties could be obviously studied through ultraviolet–visible (UV–vis) spectra and X-ray photoelectron spectra (XPS). The advantage of the structure and performance of the multilayer films prepared by layer-by-layer method could be found. It was suggested that the nearly linear growth process in peak-top absorbance in multilayer assembly. The PVA polymer substrate could disperse PMoA particles and changed the surface morphology. The polymer skeleton and PMoA particles were with strong interfacial interactions. The PMoA/PVA LbL film had wonderful visible light response. The oxygen acted a significant part during the bleaching process. According to XPS resoults, 51% of Mo⁶⁺ in the PMoA turned into Mo⁵⁺, obvious photoinduce oxidation and reduction reactions happened from PVA and PMoA through the proton transfer mechanism.     

Ultraviolet to far infrared optical properties of the one-dimensional conductor K2Pt(CN)4Br0·3. 3H2O

An experimental study of the optical properties of single crystals of the quasi-one-dimensional conductor K₂Pt(CN)₄Br_0·3, 3H₂O in the spectral range from 45,000 to 10 cm^?1 is presented.For light polarized perpendicular to the highly conducting direction the material behaves as a transparent dielectric, as evidenced by reflection and transmission spectra. The reflection spectrum measured with polarization parallel to the chain direction (E∥Z) shows, in addition to the previously reported ‘metal-like’ optical reflectance and plasma edge in the visible, deviations from free carrier type reflectance in the i.r. This was expected because the conductivity is thermally activated at low temperatures. The optical constants for E∥Z polarization have been determined by Kramers-Kronig analysis of the reflection spectrum and, at a few discrete wavelengths, from measurements of polarized reflectance under oblique incidence. The results are qualitatively consistent with various models of the electronic structure but do not distinguish between them.     

Luminescent and thermochromic properties of tellurium(IV) halide complexes with cesium

The spectral?luminescent and thermochromic properties of complex compounds of the composition Cs₂TeHal₆ (Hal = Cl, Br, I) are studied. The interrelation between the geometric structure and spectral–luminescent properties is studied using the example on complex compounds of tellurium(IV) halides with cesium. The Stokes shift and the luminescence intensity of Тe(IV) ions with island octahedral coordination are found to depend on the position of the A band in the luminescence excitation spectra, the diffuse reflection, and the energy of the luminescent ³P₁ → ¹S₀ transition of the tellurium(IV) ion. The maximum luminescence intensity and the minimum Stokes shift at 77 and 300 K are observed for Cs₂TeСl₆. The geometrical and electronic factors responsible for luminescence intensification in Te(IV) complexes under study are analyzed.     

GCLM缺陷光子晶体带隙结构及滤波特性

研究了以GCLM（the generalized Cantor-like multilayer）结构作为缺陷的光子晶体带隙结构和滤波特性.通过调整缺陷结构参量,可以得到通信波段1 300 nm~1 550 nm附近的窄带滤波窗口.滤波窗口透过率接近100%,而窗口以外的透过率在0.01以下.缺陷结构产生的Cantor分布,对光子晶体的透射特性产生很大影响,通过调整GCLM的结构,可以控制带隙的宽度及带隙中滤波窗口的数量和位置.和其他一维光子晶体相比,这种滤波特性能更好地应用在CWDM中.     

Spectral Ellipsometry of Multilayer ZnS/ZnSe Heterostructures

By the method of spectral ellipsometry with binary modulation of the polarization state the dispersions of the refractive index n, absorption coefficient k, and layer thickness in ZnS/ZnSe multilayer structures grown by the chemical gasphase deposition method from heteroorganic compounds on GaGaAssubstrates with ZnSe buffer layers have been determined. The efficiency of local ellipsometric measurements (with a light beam size less than 150 × 500 m) permitting mapping of the parameters of structures with A²B⁶ layers up to a few microns thick has been demonstrated. The optical properties of oxide layers formed on the zinc selenide surface have been investigated. Multilayer structures (ZnSe/ZnS) _n /ZnSe/GaAs with a pronounced exciton absorption and specific features in the reflection spectra coinciding in energy with exciton transitions, as well as Bragg mirrors with a reflection coefficient up to 99% in the blue region of the spectrum, have been studied.     

Spectra of $$ \mathcal{P}\mathcal{T} $$-symmetric Hamiltonians on tobogganic contours

A non-standard generalization of the Bender potentials x ²(ix ^ɛ) is suggested. The spectra are obtained numerically and some of their particular properties are discussed.     

Structural and optical properties of Fe-doped hydrogenated amorphous carbon films prepared from trans-2-butene by plasma enhanced metal organic chemical vapor deposition

Fe-doped hydrogenated amorphous carbon (a-C:H:Fe) films were deposited from a gas mixture of trans-2-butene/ferrocene/H₂ by plasma enhanced metal organic chemical vapor deposition. X-ray photoelectron spectroscopy, Fourier transform infrared spectra and Raman spectra were used to characterize the composition and the bonding structure of the a-C:H:Fe and a-C:H films. Optical properties were investigated by the UV–visible spectroscopy and the photoluminescence (PL) spectra. The Fe-doped films contain more aromatic structures and C=C bonds than the undoped films. The sp ² carbon content and sp ² clustering of the films increase, and aromatic-like rings’ structures become richer after Fe-doping. The Tauc optical gap of the a-C:H:Fe films become narrower by 0.3 eV relative to the value of the a-C:H films. The PL peak shifts from 2.35 eV of the a-C:H films to 1.95 eV of the a-C:H:Fe films, and the PL intensity of the a-C:H:Fe films is greatly enhanced. A deep level emission peak around 2.04 eV of the a-C:H:Fe films is observed.     

Nd3+ near UV and visible fluorescence in YAP:Nd

The present paper summarizes detailed investigations of Nd³⁺ fluorescence spectra in YAP:Nd laser crystal in the broad spectral range of 370–1100 nm at liquid nitrogen temperature. Especially, Nd³⁺ near UV and visible fluorescence spectra were studied for the first time in this crystal. The Nd³⁺ near UV and visible fluorescence spectra of this crystal consist of many narrow lines (up to 50). The Nd³⁺ near UV and visible fluorescence lines arise mainly from⁴D_3/2 and²P_3/2 Nd³⁺ terms (transitions from⁴D_3/2,²P_3/2 to lower lying Nd³⁺ levels are responsible for their appearance). At room temperature the fluorescence spectra consist of broad bands with narrow lines (mainly⁴D_3/2⁴F_3/2,⁴F_5/2 and²H_9/2 transitions).     

Interference phenomena of synchrotron radiation in TEY spectra for silicon‐on‐insulator structure

The general matrix theory of the photoelectron/fluorescence excitation in anisotropic multilayer films at the total reflection condition of X‐rays has been developed. In a particular case the theory has been applied to explain the oscillation structure of L_2,3 XANES spectra for a SiO₂/Si/SiO₂/c‐Si sample in the pre‐edge region which has been observed by a sample current technique at glancing angles of synchrotron radiation. Remarkably the phase of the oscillations is reversed by a ～2° angle variation. The observed spectral features are found to be a consequence of waveguide mode creation in the middle layer of strained Si, which changes the radiation field amplitude in the top SiO₂ layer. The fit of the data required the correction of the optical constants for Si and SiO₂ near the Si L_2,3‐edges.     

Ionization of hydrogen and deuterium atoms in thermal energy collisions with state-selected Ne(3s 3 P 2,3 P 0) metastable atoms

High resolution energy spectra of electrons and ions resulting from thermal energy collisions of hydrogen and deuterium atoms with state-selected metastable Ne(Ne(3s ³ P ₂,³ P ₀) atoms are reported. The electron spectra for Ne(³ P ₂)+H(D) are very broad: The high energy part due to formation of NeH⁺ (NeD⁺) bound states (associative ionization), amounts to about 30% of the ionizing events, whereas the dominant part of the spectrum including a prominent low-energy peak is due to Penning ionization out of a strongly-attractive entrance potential curve. Comparison of the spectra with quantum mechanical fit calculations yields fairly accurate information on this potential, in particular its well depthD _e [Ne(³ P ₂)?H,D]= 2.0(1) eV. The spectra for Ne(³ P ₀)+H, D are comparatively narrow with much lower cross sections than the one for the Ne(³ P ₂) state. The corresponding entrance channel is a weakly bound van der Waals molecule with a well depth below 0.1 eV. A perturbation calculation of the Ne(3s)+H(1s) potential energy curves at large distances explains the observed difference between the Ne(³ P ₂)+H(D) and Ne(³ P ₀)+H(D) systems. Symmetry arguments are given that the major contribution to the Ne(³ P ₂)+H(D) spectra is due to the² Σ potential.     

Synthesis and Characterization of a Biologically Active Lanthanum(III)–Catechin Complex and DNA Binding Spectroscopic Studies

A lanthanum(III) complex of catechin has been synthesized and characterized by elemental analysis, molar conductance, UV-Vis spectra, infrared spectra, thermal analysis, and ¹H NMR. The complex behaves as a nonelectrolyte in methanol solvent. The spectral and thermal properties of the complex are examined. A thermogravimetric (TGA) study showed the hydrated nature of the complex. ¹H NMR spectra of the lanthanum and the catechin (CT) ligands measured in CD₃OD-d₄ also show metal ligand coordination. The lanthanum–catechin complex shows bright luminescence in methanol solution. The interaction of the complex with calf thymus DNA has been investigated by absorption and emission spectroscopic measurements. Experimental spectral results suggest CT–DNA binding with catechin complex via an intercalative mode.     

The spestroscopy and structure of odd-A Fr isotopes withA=213–225

The remarkable features of the spectra of the odd-A Fr isotopes from²¹³Fr (with 126 neutrons) through²²⁵Fr (with 138 neutrons) serve as a sequence of examples for the application of a variety of nuclear models. As the shapes vary from spherical to spherical with strong octupole correlations to octupole-deformed, the corresponding symmetry breaking leads to increasingly complex spectra. Of considerable interest is the fact that the²¹⁹Fr 9/2⁻ ground state has the character of an h_9/2 shell model state while still having the rotational properties appropriate as a legitimate member of a reflection asymmetric K=1/2⁻ band. It is also possible to follow the expansion of the more degenerate shell model states into the less degenerate reflection asymmetric states. This results from dramatic decreasing in decoupling parameters with increasing mass number.