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.     

Atomiser, source, inductively coupled plasmas, in atomic fluorescence spectrometry (ASIA). Some recent work

The dual-plasma atomic fluorescence/atomic emission spectrometer (ASIA spectrometer) is described and the detection limits for several elements in both the fluorescence and the emission mode are presented and compared directly. The detection limits for the non-refractory elements are, in general, better in fluorescence than emission While for the refractory elements the converse is true, but all are in the ng ml⁻¹ range. Growth curves for a refractory and a non-refractory element are presented and evaluated.     

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.     

Atomic and ionic fluorescence spectrometry with pulsed dye laser excitation in the inductively-coupled plasma

The atomic and ionic fluorescences of iron, tin, barium and indium excited by flash-lamp-and nitrogen laser-pumped pulsed dye lasers in the inductively-coupled plasma (ICP) are studied. Noise sources are investigated and detection limits are compared to the techniques of ICP-emission and laser-excited atomic fluorescence spectrometry.     

Studies in atomic-fluorescence spectroscopy--VIII. Atomic fluorescence and atomic absorption of thallium and mercury with electrodeless discharge tubes as sources

Atomic-fluorescence measurements, with microwave-excited electrodeless discharge tubes as sources of excitation, are described for thallium and mercury. The limits of detection by atomic fluorescence are 0.12 ppm for thallium and 0.08 ppm for mercury; the corresponding limits by atomic absorption (using the same instrument and source) are 6 and 10 times as great. The preparation, operation and spectral characteristics of thallium and mercury discharge tubes are described and comparisons are made with a thallium hollow cathode lamp and thallium and mercury spectral discharge lamps.     

Detection limits and error estimation in analysis

Summary The results of theoretical calculations of the standard deviation in atomic spectrometry and analytical chemistry are discussed. Methods for the estimation of random errors and detection limits are proposed.     

An unusual systematic behaviour of detection limits for elements from 55Cs to 73Ta

A representative database for detection limits for all elements from ⁵⁵Cs to ⁷³Ta reveals that these limits are governed by a systematic zigzag pattern, according to which the odd atomic number elements have systematically lower detection limits than the even atomic number neighbour elements. This is true even when the actual detection limits vary by several orders of magnitude. We propose that such a systematic pattern be used as a requisite analytical criterion to evaluate the detection limit data, and any departure from this pattern be looked on with caution to check the analytical technique for any interference or matrix effect problems.Electronic Supplementary Material Supplementary material is available for this article if you access the article at . A link in the frame on the left on that page takes you directly to the supplementary material.     

Atomic spectrometry and flow injection analysis: a synergic combination

The combination of flow-injection techniques with atomic spectrometry (flame atomic absorption and emission spectrometry and inductively-coupled plasma/atomic emission spectrometry) is reviewed, with particular reference to the more recent contributions. The considerable growth in the number of directly couple pre-concentration and matrix isolation is noted, together with the increasing number of reports of indirect methods for metals, inorganic anions and even drug molecules. Many developments are motivated by a desire to increase the performance of the spectrometry over that obtained with conventional methods of sample introduction. Conflicting statements concerning the possible benefits of reduced uptake rate, of air compensation and of peak-area measurement are examined critically. The conflicting requirements of obtaining freedom from stable-compound interferences coupled with god detection limits are discussed, as are means of obtaining the best detection limits. Modifications to nebuliser and spray-chamber design are suggested for maximising peak height (to obtain detection limits) and for working with reduced uptake rates (to reduce stable-compound interferences in flame-based spectrometries). The single well-stirred tank model is used to model nebuliser response and results are presented for the flow-injection behaviour of a Philips Scientific SP9 instrument under conditions of low flow rate which show reasonable agreement with the model. With the instrument, the best detection limits are obtained on the basis of peak-height measurements at the flow rate producing maximum signal-to-noise ratio.     

X-ray fluorescence spectrometry with synchrotron radiation

X-ray fluorescence spectrometry (x.r.f.) can be done through excitation with synchrotron radiation. This permits multi-element determinations in the trace region with improved detection limits compared to conventional x.r.f. Detection limits are evaluated and compared with theoretically calculated values. For a beam diameter of 0.5 mm and a sample of 1 mg cm^?2, absolute detection limits are between 0.1 and 0.4 pg. The dependence of the detection limit on the atomic number is reduced, when white synchrotron radiation is used for excitation instead of monochromatic radiation. The optimum of the limit of detection on the Z-scale can be shifted to higher atomic numbers and improved through filtration of the primary radiation by aluminium absorbers. Preparation of samples on different polymeric films is discussed in relation to blank values.     

小功率空气冷却电感耦合等离子体发射光谱的研究 Ⅱ.碱金属和碱土金属分析特性

本文测定了碱金属、碱土金属九个元素48条谱线在空气冷却ICP中的信背比和检出限,并同全氩ICP的检出限进行了比较。本工作还测绘了各元素灵敏线与9个常见共存元素的光谱重叠扫描图,以了解可能存在的光谱干扰。     

The atomic absorption spectrometric determination of arsenic and selenium in mineral waters by electrothermal atomization

A procedure for the determination of arsenic and selenium in mineral waters based on electrothermal atomic absorption spectrometry is described. Because of matrix effects and the inadequate detection limits for direct determinations, both elements are separated from the macrocomponents by co-precipitation in hydrated iron(III) oxide. The precipitate is dissolved in 0.2 M sulphuric acid for injection. The detection limits are 0.2 and 0.5 μg l^?1 for arsenic and selenium, respectively.     

Determination of cadmium,zinc, and lead by non-dispersive atomic fluorescence spectrometry with a new graphite furnace atomizer

A new graphite furnace atomizer has been developed and applied to the determination of cadmium, zinc, and lead by non-dispersive atomic fluorescence spectrometry. A solar-blind photomultiplier, a lock-in amplifier, and microwave-excited electrodeless discharge lamps are used. The detection limits for cadmium, zinc, and lead in the non-dispersive atomic fluorescence mode are 1·10^?13g, 2·10^?13g, and 2·10^?11g, respectively, which are 20-, 10-, and 2-fold better than those in the atomic absorption mode. The analytical working curves are linear over about three decades of concentration from the detection limits.     

Is odd-even effect reflected in detection limits?

It is observed for the first time from an extensive compilation that the detection limit ratios for odd/even atomic number neighbour elements are generally less than 1 for nearly all-stable elements of the periodic table (most are even less than 0.5), which is very similar to the odd-even effect in cosmic abundances. This systematic behaviour of detection limits can be explained by a simple relationship with physicochemical and environmental-geological factors. We propose that such a behaviour should be used in future as a fundamental criterion to evaluate the highly variable detection limit data for all chemical elements by a given analytical technique and the estimation of detection limits should be based on at least 30 or more measurements.     

Laser atomic absorption spectrometry of excited Hg in a discharge applying sum frequency mixing of two diode lasers (preliminary results)

Wavelength modulation diode laser atomic absorption spectrometry is applied to the detection of atomic mercury. Transitions from metastable energy levels highly populated in a radio-frequency discharge are induced with laser diodes by use of nonlinear techniques. The wavelength of one strong transition at 365.119 nm with a high oscillator strength is obtained by sum frequency generation of two diode lasers. The cold vapor technique is used to transfer ionic into atomic mercury. The mercury in the vapor phase is transported by an argon stream into the discharge tube. From the time-dependent absorption signals detection limits of 100 ng/L are achieved at this state of research.     

Laser atomic absorption spectrometry of excited Hg in a discharge applying sum frequency mixing of two diode lasers (preliminary results)

Wavelength modulation diode laser atomic absorption spectrometry is applied to the detection of atomic mercury. Transitions from metastable energy levels highly populated in a radio-frequency discharge are induced with laser diodes by use of nonlinear techniques. The wavelength of one strong transition at 365.119 nm with a high oscillator strength is obtained by sum frequency generation of two diode lasers. The cold vapor technique is used to transfer ionic into atomic mercury. The mercury in the vapor phase is transported by an argon stream into the discharge tube. From the time-dependent absorption signals detection limits of 100 ng/L are achieved at this state of research.     

Comparison of electrothermal atomization diode laser Zeeman- and wavelength-modulated atomic absorption and coherent forward scattering spectrometry

Atomic absorption and coherent forward scattering spectrometry by using a near-infrared diode laser with and without Zeeman and wavelength modulation were carried out with graphite furnace electrothermal atomization. Analytical curves and limits of detection were compared. The magnetic field was modulated with 50 Hz, and the wavelength of the diode laser with 10 kHz. Coherent forward scattering was measured with crossed and slightly uncrossed polarizers. The results show that the detection limits of atomic absorption spectrometry are roughly the same as those of coherent forward scattering spectrometry with crossed polarizers. According to the theory with bright flicker noise limited laser sources the detection limits and linear ranges obtained with coherent forward scattering spectrometry with slightly uncrossed polarizers are significantly better than those obtained with crossed polarizers and with atomic absorption spectrometry. This is due to the fact that employing approaches of polarization spectroscopy reduce laser intensity fluctuations to their signal carried fractions.     

Analytical Potentials and Features of Atomic Emission Analysis Using Electron-Impact Excitation of Atoms in Helium under Atmospheric Pressure

A device is described for the atomic emission analysis of vaporous samples using electron-impact excitation in helium under atmospheric pressure. The device consists of a cathode atomizer with a test sample applied onto it and the anode located at 1–3 mm from the cathode. The electrons emitted by the cathode upon heating are accelerated by applying a constant voltage to the electrodes. The mechanism for the formation of a non-self-sustained gas discharge between the cathode and anode is considered and the properties of the discharge are compared to those of the known discharges used in atomic emission spectrometry. The influence of atomization temperature and helium pressure on the analytical and background signals was studied. It is shown that, under certain conditions, the analytical signal increases with helium pressure. The relative detection limits attained for a number of elements are from tenths to dozens of nanogram per liter; this is two or three orders of magnitude lower than those in inductively coupled plasma atomic emission spectrometry and of the same order of magnitude as detection limits in inductively coupled plasma mass spectrometry.     

Comparison of line and continuous sources in atomic absorption spectrophotometry

Expressions are given for the absorption signal (absorbance or fraction absorbed) in atomic absorption spectrophotometry with a line source and a continuous source, respectively. A theoretical and experimental comparison is made between the shape of the working curves, the magnitude of the signals, and the limits of detection in both cases. The significance of the spectral bandwidth of the monochromator and the absorption line profile is discussed. With a good medium-dispersion monochromator, a continuous source offers several distinct advantages and yields detection limits which are approximately the same as those obtained with a hollow-cathode discharge tube.     

The determination of arsenic and selenium in coal by continuous flow hydride-generation atomic absorption spectrometry and atomic fluorescence spectrometry

Concentrated perchloric acid is used to digest coal for subsequent determination of arsenic and selenium by hydride-generation atomic absorption and fluorescence spectrometry. Arsenic and selenium are removed from potentially interfering metal ions by coprecipitation with lanthanum hydroxide. The detection limits, 58 and 36 ng g^?1 by atomic absorption and 25 and 10 ng g^?1 by atomic fluorescence, for arsenic and selenium in coal, respectively, are adequate for the normal levels of these metals.     

Effects of sample matrix on detection limits in analytical inductively coupled plasma-Fourier transform spectrometry

The feasibility of making analytical atomic spectrometry measurements by inductively coupled plasma-Fourier transform spectrometry (ICP-FTS) is demonstrated. Analytical working curves and detection limits are presented for Al, Ni, Fe and Ca. The effects of sample matrix composition on detection limits for analytical ICP-FTS are investigated. It is shown that a multiplex disadvantage may occur in the case of a spectral bandpass encompassing stroog emission lines of a matrix element. A “worse case” example of this problem is presented. Possible approaches to overcoming the multiplex disadvantage in analytical ICP-FTS and some ideal criteria for ICP-FTS instrumentation are presented.