高分子固溶态染料激光材料的光学性质（Ⅰ）

引入极性交联剂(Ⅰ)改性的MMA-MA共聚物作基质,通过研究激光染料Rh6G在不同组成的基质中的吸收光谱、荧光特性和激光能量转换效率的关系,获得含Rh6G的固溶态材料。对材料的光学均匀性作了探讨,材料的激光输出特性达到同条件下的Rh6G乙醇溶液水平,显示了染料在固溶态中激光运转的可能性。     

Capacitive Discharge Graphite Furnace Laser-Excited Atomic Fluorescence of Thallium

For the first time, an anisotropic graphite furnace heated by capacitive discharge was used for laser-excited atomic fluorescence spectrometry. A detection limit of 5 fg for thallium was obtained with a laser repetition rate of 500 Hz and a peak integration time of 80 ms. The use of a capacitive discharge furnace allows for a shorter integration time, which in turn should allow for integration of less background noise, and improved detection limits. Theoretically, the magnitude of the shot noise should be proportional to the square root of the integration time, and inversely proportional to the square root of the laser repetition rate. Experimental data illustrated the effect of laser repetition rate, but were inconclusive with respect to integration time. The linear dynamic range of the calibration curve was six orders of magnitude, which was comparable to that normally obtained for laser-excited atomic fluorescence in modern commercial graphite furnaces. Thallium was accurately determined in NIST biological samples at levels one to two orders of magnitude below the detection limit of electrothermal atomic absorption spectrometry, with an analytical precision between 8 and 20%. The interference effects of calcium, sodium chloride, and potassium chloride on the thallium signal were investigated and shown to be similar to both laser-excited atomic fluorescence in a conventional furnace and capacitive discharge furnace atomic absorption results reported in the literature.     

Sub-picogram detection of lead by non-flame atomic fluorescence spectrometry with dye laser excitation

The frequency-doubled radiation of flashlamp-pumped dye laser has been compared with the radiation of an eleotrodeless discharge lamp (EDL) and a hollow cathode lamp (HCL) as excitation light sources in non-flame atomic fluorescence spectrometric (AFS) measurements. Detection limits and linear ranges of the analytical working curves have been studied. The aqueous Pb sample solutions used in this study were atomized in an electrically heated graphite rod. Direct line fluorescence at 405.8 nm has been observed. The limit of detection obtained with the laser as excitation source is about one order of magnitude lower than the detection limits obtained with the EDL and HCL. The absolute limit of detection of 0.2 pg is the lowest reported value to date attained in any atomic spectrometric method. The ultraviolet laser irradiance was found to be high enough to approach saturation conditions. As a result selfabsorption of the exciting laser beam is reduced and the linear range of the analytical working curve is extended to higher analyte concentrations.     

Laser-excited ionic fluorescence spectrometry of rare-earth elements in the inductively-coupled plasma

A pulsed tunable dye laser pumped with an excimer laser is used to excite ionic fluorescence of the rare earth elements in the inductively-coupled plasma. Because several fluorescence lines were observed after laser excitation, it was possible to draw partial energy-level diagrams for most of the rare earths. Non-resonance fluorescence lines were used for all measurements in order to minimize spectral interferences. Detection limits at given excitation wavelengths are reported for each element. Laser-excited ionic fluorescence eliminates the problem of spectral interferences which has been associated with the determination of the rare earths by atomic emission spectrometry in the inductively-coupled plasma.     

Construction and performance of a time-multiplex multiple-slit flame atomic fluorescence spectrometer for multi-element analysis

The design and performance characteristics of a new multi-element flame atomic fluorescence spectrometer are presented. Radiation from four hollow-cathode tubes is directed onto an unsheathed air—hydrogen flame. The resulting atomic fluorescence is viewed by a special monochromator with a separate exit slit for each element. The light exiting from all slits is directed to a single photomultiplier tube. The fluorescence signals from different elements are distinguished by a time multiplex approach. Single-element detection limits for ten elements and multi-element detection limits for four elements are presented. The degradation of detection limits by flame background emission noise and effect of flame composition on performance are discussed. Better than 1% precision is obtained for moderate analyte concentrations.     

Laser induced double-resonance ionic fluorescence in an inductively coupled plasma

Two pulsed dye lasers pumped by an excimer laser are simultaneously directed into the analytical zone of an inductively coupled argon plasma. When the two beams are tuned to the appropriate ionic transitions, highly excited ionic levels can be efficiently populated in saturated conditions, the resulting fluorescence being then spectrally isolated with a monochromator and measured. A theoretical outline of this technique, variously called double-resonance fluorescence or two-step fluorescence, is given. The experimental results obtained with the alkaline-earth metals Ca, Sr, Ba and Mg show that the technique does provide excellent sensitivity, freedom from scattering problems and unprecedented spectral selectivity. The laser characteristics, the time overlap between the pulses and the spectral characteristics of the transitions used are discussed. Finally, ionic fluorescence in the plasma is the most suitable analytical application of such double-resonance technique since its use in flame atomic fluorescence suffers from the strong depletion of the excited levels due to collisionally assisted ionization.     

Application of laser-excited atomic fluorescence spectrometry to the determination of iron

A frequency-doubled, flashlamp-pumped tunable dye laser is used to excite the Stokes direct-line atomic fluorescence transition of iron (296.7 nm/373.5 nm). Limits of detection are determined with single (0.6 ng/ml) and multipass (0.2 ng/ml) and with a l s time constant (a 0.06 ng/ml limit detection is obtained with an 8 s time constant). Noise sources limiting precision at both low (background flame emission shot and flicker noise) and high concentrations (laser pulse to pulse variability) concentrations are investigated and the technique is used for the determination of iron in simulated fresh water NBS SRM-1643), unalloyed copper (NBS SRM-394) and fly ash (NBS SRM-1633).     

Atomic absorption spectrometry and other instrumental methods for quantitative measurements of arsenic

Progress in instrumental methods for quantification of arsenic during the past decade is reviewed. Particular emphasis is placed on atomic absorption spectrometry, where major progress has been made in flame methods in conjunction with hydride generation procedures and in electrothermal methods with the graphite furnace. Specific materials in which arsenic is quantified by atomic absorption techniques are also listed. Progress in the application of neutron activation—γ-spectrometry, emission spectrometry, electrometric methods, x-ray procedures and atomic fluorescence spectrometry is also reviewed. The limits of detection and time requirements of all the techniques are compared.     

Studies in atomic fluorescence spectrometry: Part II. Interference effects in the determination of tin with various premixed flames

The interference effects are reported for 27 elements, 6 acids and 4 organic liquids on the atomic fluorescence determination of tin with argon-hydrogen, argon-oxygen-hydrogen and argon-separated air-acetylene flames. The addition of1000 p.p.m. iron (III) eliminates most interferences from the elements but not from the acids. The basic trends in the interference effects in the argon-hydrogen flame for the atomic absorption and atomic fluorescence determinations of tin are similar. The detection limit, for an 18.2-s time constant, in the argon-oxygen-hydrogen and argon-hydrogen flames is 0.006 p.p.m. and in the air-acetylene flame it is 0.05 p.p.m. These detection limits are significantly better than previously reported limits. Analytical curves in all three flames studied are linear between the detection limits and 250 p.p.m.     

Atomic Absorption Spectrometry with an Alternating Current Plasma as an Atomization Source

Abstract

The utilization of an alternating current plasma as an atomization source for atomic absorption spectrometry is described. The analytical performance of this technique has been characterized for the determination of 11 elements. The detection limits (3[sgrave]) were found to be comparable to those determined with existing plasma sources. The accuracy of the method has also been assessed by comparison with flame and graphite furnace atomic absorption spectrometric methods.     

Atomic fluorescence and atomic emission measurements with an image dissector echelle spectrometer

This paper deals with the investigation of an image dissector echelle spectrometer as an analytical instrument for flame atomic fluorescence spectrometry and for flame atomic emission spectroscopy. The fluorescence was induced by high-pressure xenon arc lamps, which emitted continuum spectra and had higher power ratings, i.e. 1.6 and 2.5 kW, than those normally used for the same purpose. The experimental set-up included two different types of premix burners and one type of total consumption burner. A spherical reflector was applied to improve the utilization of the fluorescence radiation. Two different coatings were tested. None gave the expected enhancement.Detection limits and growth curves were measured for 8 different elements (Ca, Co, Cu, Fe, K, Mg, Na and Ni) in a non-separated air/acetylene flame. The attained detection limits were found to be equally good or somewhat better in flame atomic fluorescence excited with continuum sources than previously reported in the literature, i.e. using similar flames. In flame atomic emission spectroscopy better detection limits have been reported before.     

Comparison of the helium/oxygen/acetylene and air/acetylene flames as atom sources for continuum-source atomic fluorescence spectrometry

The helium/oxygen/acetylene flame is compared to the more widely used air/acetylene flame for its utility as an atom cell for atomic fluorescence spectrometry. Nearly identical experimental arrangements were used for both flames in order to make the comparison valid. With a continuum source used for excitation, fluorescence detection limits in the helium/oxygen/acetylene flame were between 13 and 60 times better (lower) than those determined for the same eight elements in the air/acetylene flame. The improved detection limits are attributable mainly to the higher temperature, increased thermal conductivity and lower quenching in the helium flame. Fluorescence background spectra were obtained for both flames over the wavelength range 185–650 nm, and showed the helium flame to have slightly smaller background fluctuations, but a much larger background because of the more favorable fluorescence conditions in the flame.     

A demountable boosted-output spectral lamp for atomic absorption and fluorescence measurements

A demountable boosted-output spectral lamp is described that permits easy exchange of the cathode, which is in the form of a disc pressed from the appropriate powder or machined from rod. The new lamp overcomes to a large extent the major disadvantage of the conventional boosted hollow-cathode lamp, namely the interaction of the sputtering and boosting discharges. In flame atomic absorption spectrometry it yields calibration curves more nearly linear than those obtained with commercial hollow-cathode lamps. In non-dispersive flame atomic fluorescence it permits the attainment of detection limits rather better than those obtained with other high-intensity light sources.     

Determination of boron in blood,urine and bone by electrothermal atomic absorption spectrometry using zirconium and citric acid as modifiers

A comparative study of various potential chemical modifiers (Au, Ba, Be, Ca, Cr, Ir, La, Lu, Mg, Ni, Pd, Pt, Rh, Ru, Sr, V, W, and Zr), and different ‘coating’ treatments (Zr, W, and W+Rh) of the pyrolytic graphite platform of a longitudinally heated graphite tube atomizer for thermal stabilization and determination of boron was undertaken. The use of Au, Ba, Be, Cr, Ir, Pt, Rh, Ru, Sr and V as modifiers, and of W+Rh coating produced erratic, and noisy signals, while the addition of La, Ni and Pd as modifiers, and the W coating had positive effects, but with too high background absorption signals, rendering their use unsuitable for boron determination even in aqueous solutions. The atomic absorption signal for boron was increased and stabilized when the platform was coated with Zr, and by the addition of Ca, Mg, Lu, W or Zr as modifiers. Only the addition of 10 μg of Zr as a modifier onto Zr-treated platforms allowed the use of a higher pyrolysis temperature without analyte losses. The memory effect was minimized by incorporating a cleaning step with 10 μl of 50 g l⁻¹ NH₄F HF after every three boron measurements. The addition of 10 μl of 15 g l⁻¹ citric acid together with Zr onto Zr-treated platforms significantly improved the characteristic mass to m₀=282 pg, which is adequate for biological samples such as urine and bone, although the sensitivity was still inadequate for the determination of boron in blood of subjects without supplementary diet. Under optimized conditions, the detection limit (3σ) was 60 μg l⁻¹. The amount of boron found in whole blood, urine and femur head samples from patients with osteoporosis was in agreement with values previously reported in the literature.     

Characterization of ground state analyte neutral atoms and ions in the inductively coupled plasma using atomic fluorescence spectrometry

A nitrogen pumped dye laser source atomic fluorescence system that can be used to spatially map the distribution of ground state neutral atom and ion species in the inductively coupled plasma is described. Complete maps of neutral atom and ion species (Ca and Sr) were measured with this system. Measurements are presented (15 point radial profiles) for five heights (9,13,19,25 and 31 mm above the load coil), five powers (0.5,0.75,1.0,1.25 and 1.5 kW), and three carrier gas flow rates (1,0.85 and 0.651/min). The results are extensively discussed and compared with atomic absorption data and other fluorescence data in the literature.     

Determination of copper,iron and zinc in spirituous beverages by total reflection X-ray fluorescence spectrometry

The concentration of copper in traditional homemade alcoholic distillates produced in Venezuela (Cocuy de Penca) were determined by total reflection X-ray fluorescence (TXRF) using vanadium as internal standard. The results were compared to those obtained by flame atomic absorption spectrometry (FAAS). Three preparative methods of addition of vanadium were compared: classical internal standard addition, ‘layer on layer’ internal standard addition and in situ addition of internal standard. The TXRF procedures were accurate and the precision was comparable to that obtained by the FAAS technique. Copper levels were above the maximum allowed limits for similar beverages. Zinc and iron in commercial and homemade distilled beverages were also analyzed by TXRF with in situ addition of internal standard demonstrating the usefulness of this technique for trace metal determination in distillates.     

Combined furnace—flame non-dispersive atomic fluorescence spectrometry for direct simultaneous multi-element analysis of air filters

Furnace volatilization followed by atomization in the flame of a non-dispersive atomic fluorescence spectrometer is used for the direct, simultaneous, multi-element determination of Zn, Cd, Pb and Fe on air filter papers. Standardization is done by using blank filter papers impregnated with standard metal solutions. The results agree well with those obtained by a standard atomic absorption procedure.     

Improvements in derivative-corrected nitrous oxide-acetylene flame emission spectrometry

The use of repetitive optical scanning in the derivative mode has been thoroughly evaluated for flame emission spectrometry with a nitrous oxide-acetylene flame. Most of the detection limits obtained were the best reported for flame emission spectrometry. A comparison has been made between atomic absorption and inductively coupled plasma spectrometry. The flame emission technique was found to be complementary to and highly competitive with both techniques.     

Evaluation of the analytical capabilities of frequency modulated sources in multielement non-dispersive flame atomic fluorescence spectrometry

Frequency modulated sources of Cd and Zn are used to produce modulated atomic fluorescence signals (at two different frequencies) in a non-dispersive flame atomic fluorescence spectrometer. To reduce the flame background level, a chlorine filter, a separated air—acetylene flame, and a solar blind photomultiplier are used. Even so, there is shown experimentally and theoretically to be a multiplex disadvantage, as compared to the conventional single slit scanning dispersive spectrometer, as a result of the flame background photon noise and an additional multiplex disadvantage at high concentrations of an interference, e.g. in the measurement of Zn (213.9 nm), Cd (228.8nm) results in a reduced S/N for Zn when the Cd signal level becomes comparable with the flame background signal level. Little future for multiplexed techniques in atomic flame spectrometry in the u.v.- Visible is predicted.     

The use of a dye laser for the detection of sub-picogram amounts of lead and iron by atomic fluorescence spectrometry

The frequency-doubled radiation of a dye laser excited by the second harmonic radiation of a YAG:Nd³⁺ laser has been used as light source in graphite-tube atomic fluorescence analysis. Detection limits and linear ranges of the analytical curves for two elements, Pb and Fe, were studied. Direct-line fluorescence at 373.5 mn for Fe and at 405.8 nm for Pb was observed. The limits of detection, obtained using linear extrapolation to the background level, were 25 pg/ml for Fe and 2.5 pg/ml for Pb. This corresponds to an absolute detection limit of 0.75 pg for Fe and 0.075 pg for Pb. In the case of Pb, saturation was reached at an intensity of the exciting radiation of about 20 kW/cm², but in the case of Fe, linearity was maintained up to 300 kW/cm².