Determination of radiative lifetimes in neutral nitrogen using short laser pulses from a distributed feedback dye laser

Radiative lifetimes were determined for two short-lived states in neutral nitrogen. Following photo-dissociation and two-photon excitation employing the same UV source, excitation to higher states was performed with a distributed feedback dye laser (DFDL). The lifetimes were found to be τ(2p ²4d ⁴ D _7/2)=17(3) ns and τ(2p ²5s ⁴ P _5/2)=22(3) ns.     

Energy transfer studies in binary dye solution mixtures: Acriflavine+Rhodamine 6G and Acriflavine+Rhodamine B

The effect of acceptor concentration on the energy transfer in Acriflavine (donar) plus Rhodamine 6G (Rh 6G) and Acriflavine plus Rhodamine B (Rh B) binary solution mixtures has been studied. The theoretical calculations are done to determine their lifetimes. Effect of these values on the total transfer efficiency at various acceptor concentrations have been studied to identify the appropriate energy transfer mechanism responsible for photon emissions, enhancement in lasing efficiency and dreading of the tenability of such mixed solutions. The energy transfer rate constants and critical transfer radius (R(0)) are calculated using Stern-Volmer plots and concentration dependence of radiative and non-radiative transfer efficiencies have also been determined. The experimental results indicate that dominant mechanism responsible for the efficient energy transfer in the binary mixtures is of non-radiative kind and is due to long-range dipole-dipole interaction.     

Energy transfer dye laser: Confirmation of energy transfer by reabsorption effect

The laser and fluorescence behavior was studied for the mixed dye system containing various concentrations of 3,3′-diethylthiacarbocyanine iodide and rhodamine 6G. A new way of confirming the occurrence of energy transfer is presented on the basis of the reabsorption effect.     

Comments on the energy transfer dye laser

Kinetic analysis of an energy transfer dye laser is presented. The laser gain function depends on the molecular parameters and on the concentrations of both the donor and acceptor. For the low signal limit the gain shows linear dependence on either the donor or the acceptor concentrations for a fixed donor-acceptor concentration ratio. This behavior has been confirmed experimentally.     

Distributed feedback multipeak laser emission in Rhodamine 6G doped organic-inorganic hybrids

Organic-inorganic hybrid materials were prepared from an ureasil precursor (ureapropyltriethoxysilane designated as UPTES) and acrylic acid modified zirconium (IV) n-propoxide. Thin films containing rhodamine 6G (Rh6G) were prepared by spin-coating on glass substrates with different Zr:Si molar ratios (Zr:Si = 75:25, 50:50 and 25:75). Refractive index, thickness, number of propagating modes and attenuation coefficient were measured at 543.5, 632.8 and 1550 nm wavelengths by the prism coupling technique. Distributed feedback (DFB) laser effect was observed and studied as a function of films thickness and refractive index.     

有机染料罗丹明B在复合催化剂TiO2-APS-PW11Ni作用下的光降解研究

利用自组装方式制备了多酸-有机胺-二氧化钛复合催化剂K5Ni(H2O)PW11O39-APS-TiO2(APS为(C2H5O)3SiCH2CH2CH2NH2的简称),简称为TiO2-APS-PW11Ni,通过红外(IR),紫外漫反射(UV/DRS)对其组成和结构进行了表征.并利用该催化剂光降解染料污染物罗丹明B(RB)水溶液,与纳米TiO2催化剂光降解进行对比,结果表明,染料罗丹明B在复合催化剂作用下的催化效果明显优于TiO2光催化效果,计算得降解半衰期分别为:T1/2(复合催化剂)＝6.5 min,T1/2(TiO2)＝21.2 min.     

Improving the conversion efficiency of an organic distributed feedback laser by varying solvents of the laser gain layer

Control experiments were performed to improve the slope conversion efficiency of the organic distributed feedback laser by varying the dissolution solvents of the laser gain layer, a conjugated polymer poly(2-methoxy-5-(2?-ethyl-hexyloxy)-1,4-phenylene-vinylene) (MEH-PPV) in this work. The distributed feedback configuration of the laser was prepared by holographic photopolymerisation of the polymer/liquid crystal (HPDLC) mixture. Experimental results showed that the tetrahydrofuran (THF) solvent cast laser gain layer had a lower lasing threshold (0.28 μJ/pulse) and a higher slope conversion efficiency (7.8%) than that of the xylene solvent cast laser gain layer (0.5 μJ/pulse, 4.9%). Thin film waveguide characterisation demonstrated that the THF-cast film possessed a smaller waveguide loss (5.3 cm^?1) and larger net gain (17.1 cm^?1) than the xylene-cast film (8.3 cm^?1, 15.7 cm^?1). Absorbance and photoluminescence spectra indicated that the THF-cast film showed brighter luminescence at 620 nm and larger absorbance at 532 nm, indicating that the interchain interactions of the MEH-PPV is different, which plays the vital role in improving the optical performance of our organic DFB lasers.     

Saturation spectroscopy of NH2 using a CW dye laser

Hyperfine structure in the electronic spectrum of NH₂ has been resolved using the technique of intermodulated fluorescence with CW dye laser excitation. From the observed spacings values for the ¹⁴N Fermi contact and dipole-dipole coupling terms have been estimated for both the ground state and the Π(0,10,0) vibrational level of the à ²A₁ excited electronic state.     

Difluoro-boron-triaza-anthracene: a laser dye in the blue region. Theoretical simulation of alternative difluoro-boron-diaza-aromatic systems

The synthesis, photophysical and laser properties of a difluoro-boron-triaza-anthracene (BTAA) compound are analyzed in the present paper. The molecular structure of this dye is an anthracene-like core with N atoms at 4a, 9 and 10a positions where two of them (4a and 10a) are linked through a BF(2)-bridge group. This structure is reminiscent of aza-BODIPY dye with an s-indacene core, BODIPY being one of the most commonly used laser dye family in the Vis region. The main absorption and emission bands of the new dye are localized in the blue part of the Vis region of the electromagnetic radiation, a spectral region practically unexploited by the BODIPY chromophore. Moreover, the new dye presents a higher laser efficiency and photostability than other commercial laser dyes operating in the same spectral region. In order to look for new molecular structures with potential laser emission covering the whole Vis spectral region, the spectroscopic properties of other different chromophoric systems based on BF(2)-linking aromatic groups are theoretically simulated by quantum mechanical calculations.     

Thermal lens spectrophotometry of nitrogen dioxide using an excimer-laser-pumped dye laser

A thermal lens spectrophotometer based on a pulsed dye laser pumped by an excimer laser was constructed. A thermal lens spectrum was measured for nitrogen dioxide by scanning the dye laser wavelength, which was well correlated with an absorption spectrum. A linear calibration graph was obtained in the nl 1^?1 range, the detection limit being 4 nl 1^?1, which is similar to the best value achieved by other laser spectrometric methods. The enhancement factor achieved was 16, which is much smaller than the theoretical value of 292 calculated by assuming an exciting laser with a single transverse mode (beam waist radius 0.12 mm). However, the observed enhancement factor agrees fairly well with the theoretical value of 17 calculated from the observed beam radius (0.5 mm) at the waist. Hence the observed small enhancement factor is ascribed to poor beam quality of the dye laser used. Pulsed thermal lens spectrophotometry is shown to be useful especially for the analysis of gaseous samples at elevated temperatures.     

A fragmentation study of the Rhodamine 610 cation using visible‐laser desorption ionization

The fragmentation of a potential visible matrix‐assisted laser desorption ionization: Rhodamine 610 was studied under 532 nm visible irradiation, as a function of anion counter ion. It was found that at a fixed fluence, the chloride salt produced fewer fragments than those formed with ClO₄^? or BF₄^?. Evidence presented suggests that the degree of fragmentation is inversely proportional to the strength of the contact ion pair in the solid state; that is, more energy is deposited into the radical cation which can lead to fragmentation when less energy is required to separate the ion pair. Similar results were found for salts of Rhodamine 6G. Copyright © 2010 John Wiley & Sons, Ltd.     

Concentration-dependent energy transfer studies in ternary dye mixture of Stilbene-420, Coumarin-540 and Nile Blue

The energy transfer studies in the case of ternary dye mixture [Stilbene-420 (donor)+Coumarin-540 (intermediator)+Nile Blue (acceptor)] have been done and discussed through optical gain characteristics at various acceptor concentrations under nitrogen laser excitation. The concentration of the other two dyes were kept constant. It is observed that the concentration of the acceptor dye plays a very critical role in energy transfer dye laser (ETDL) as small change in its concentration varies the intensity of the laser output in the red region by large amount. Also, the highest laser output in the red region is obtained when the concentration of the acceptor dye is slightly higher than that of the intermediator dye. The present studies are helpful in deciding the optimum concentration of the acceptor dye to be used in ternary dye mixture for maximum gain and tuning range. The ternary dye mixture under study provides an ETDL tuning range up to 700 nm.     

Photodynamic diagnosis in respiratory tract malignancy using an excimer dye laser system

Equipment has been developed for the early-stage diagnosis and treatment of cancer using an excimer dye laser. The excimer laser beam is obtained by exciting XeCl. A 405 nm beam tuned by DPS dye is used for tumour localization and a 630 nm beam obtained with a rhodamine B dye is used for treatment. The equipment was applied clinically on the basis of extensive experimental research. Effectiveness for cancer localization was examined in 11 cases: four were early stage (three lung cancer and one vocal cord cancer), four were stage I, two were stage III and one was stage IV. All cases were squamous cell carcinoma except for one case of adenocarcinoma. Fluorescence was recognized in all lesions and the equipment was effective for localization.     

The spectroscopic detection of molecular species using a scanning narrow-band dye laser

A continuously scanning, frequency doubled, tunable dye laser, pumped by a pulsed nitrogen laser, has been used to excite fluorescence of gaseous molecules. It was possible not only to scan continuously the fundamental wavelength, but also to scan the excitation wavelength when frequency doubled (270 – 325 nm) over a range exceeding 2 nm with a bandwidth of less than 0.01 nm.Insertion of an etalon into the dye laser cavity resulted in a narrowing of the laser output bandwidth to <0.002 nm in the fundamental and to 0.0005 nm in the ultraviolet (frequency-doubled) output. A simple technique has been devised for making almost linear, continuous scans of the narrow-band excitation wavelength over a range of 0.15 nm in the fundamental, or 0.08 nm in the second harmonic.The results are exemplified by studies of the laser-induced fluorescence of I₂, SO₂ and the OH free radical. However, laser induced fluorescence from the atmospherically-important ClO radical could not be detected under similar conditions, and possible reasons for this result are discussed.     

Optimization and mass transfer simulation of remazol brilliant blue R dye adsorption onto meranti wood based activated carbon

Remazol brilliant blue R dye (RBBR) brings toxicity to living organisms once it enters the environment. This study utilized response surface methodology (RSM) and Polymath software for optimization and mass transfer simulation purposes, respectively. RSM revealed that the optimum preparation conditions of meranti wood-based activated carbon (MWAC) were 441 W, 5.76 min, and 1.35 g/g for radiation power, radiation time, and KOH:char impregnation ratio (IR), respectively, which translated into 86.39 mg/g of RBBR uptakes and 31.94 % of MWAC’s yield. The simulation study predicted the mass transfer rate, r_m to be 112.20 to 1007.50 s^?1 and the adsorption rate, k₁ to be 3.96 to 4.34 h^?1. The developed model predicted the adsorption surface area, a_m to be 790.04 m²/g and this value is highly accurate as compared to the actual mesopores surface area of 825.58 m²/g. Mechanism analysis divulged that the interaction that occurred between RBBR molecules and MWAC’s surface were hydrogen bond (methylene and alkyne), dipole–dipole force (alkyl carbonate, terminal alkyne, and methoxy), and ion–dipole force (primary amine). The isotherm and kinetic studies found that the adsorption data obeyed the Freundlich model and pseudo-first-order (PFO) model the best, respectively. The Langmuir maximum adsorption capacity, Q_m was computed to be 327.33 mg/g. Thermodynamic parameters were calculated to be ?4.06 kJ mol^?1, 0.06 kJ mol^?1 K^?1, –22.69 kJ mol^?1, and 16.03 kJ mol^?1 for ΔH°, ΔS°, ΔG°, and E_a, respectively, which signified the adsorption process studied was exothermic, spontaneous and governed by physisorption.     

Colorimetric assay for lysozyme using Micrococcus luteus labeled with a blue dye, Remazol brilliant blue R, as a substrate.

Micrococcus luteus (M. lysodeikticus) labeled with Remazol brilliant blue R (blue ML) was prepared as a novel substrate for the colorimetric assay of lysozyme. The treatment of the labeled substrate with lysozyme resulted in the release of soluble blue products which can be easily measured spectrophotometrically at 600 nm. The blue color was most efficiently released at pH 7 and ionic strength of 0.2 on incubation with hen lysozyme at 40 degrees C. A new colorimetric method for the assay of lysozyme using this substrate was developed. The assay system gave a linear dose-response curve, and as little as 0.1 microgram of human lysozyme (1 microgram/ml, 100 microliters) can be detected. The present method is more convenient and reproducible than the conventional lysozyme assay with bacterial cells. Application of the system to the determination of lysozyme in human serum is described.     

Energy transfer from chemically attached rhodamine 101 to adsorbed methylene blue on microcrystalline cellulose particles

Rhodamine 101 (R101) was chemically attached onto microcrystalline cellulose and methylene blue (MB) was adsorbed to a sample bearing nearby 6 × 10^?7 mol R101 (g cellulose)^?1. The system was studied by reflectance and emission spectroscopy in the solid state. R101 shows no aggregation in these conditions and, while pure MB builds up dimers on cellulose even at 2 × 10^?8 mol g^?1, in the presence of R101 no evidence on selfaggregation or heteroaggregation is found up to around 10^?6 mol g^?1. No exciplex formation is found as well. The overall fluorescence quantum yield measured on thick layers, once re‐absorption effects are accounted for, amounts to 0.80 ± 0.07 for pure R101 and decreases steadily on increasing the concentration of MB. Results demonstrate the occurrence of radiative and nonradiative singlet energy transfer from R101 to MB. For thick layers of particles, the combined effect of both kinds of energy transfer amounts to nearly 80% at the highest acceptor concentration, while nonradiative transfer reaches 60% both for thin and optically thick layers. The dependence of nonradiative energy transfer efficiencies on the acceptor concentration is analyzed and the origin of departures from Förster behavior at low acceptor concentration is discussed.     

Photophysics of TICT states of 7-diethylamino-4-methyl coumarin dye by energy transfer techniques

Coumarin 1 exhibited dual amplified spontaneous emission (ASE) in certain solvents under nitrogen laser excitation. These emissions are known as normal and anomalous emissions. The anomalous emission corresponds to TICT state and it does not have a corresponding fluorescence peak. Energy transfer techniques have been used to study the photophysics of TICT states and the characteristics of dual ASE bands of the dye coumarin 1.