By R. M. Dagnall

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Prikl. Spektr. 11, 217 (1969). Β. V. L'vov, Spectrochim. Acta, 24B, 53 (1969). Β. V. L'vov, Atomno-Absorptsionny SpektraVny Analiz (Atomic Absorption Spectroscopy). Nauka: Moscow (1966). D. A. Katskov and Β. V. L'vov, Zh. Prikl. Spektr. 10, 867 (1969). D. A. Katskov, G. G. Lebedev and Β. V. L'vov, Zh. Prikl. Spektr. 10, 215 (1969). Β. V. L'vov and A. D. Khartsyzov, Zh. Analyt. , Mosk. 25, 1401 (1970). Β. V. L'vov and A. D. Khartsyzov, Zh. Analyt. , Mosk. 24,936 (1969). A. Walsh, Appl. Optics, 7,1259 (1968).

In practice, however, in the case of evaporation into the cuvette of samples deposited in solution form on the electrode face, one almost always has τί/τ2 < 1. Therefore, for the optimization of measurement conditions it is sufficient to satisfy condition 27. T Tc ri = 0-7sec Figure 5. Pulse records for various values of 23 T c ri Β. V. L'VOV As an example illustrating the effect of r c i r on the signal-to-noise ratio in atomic absorption measurements of the peak values of pulses, Figure 5 shows recordings of a series of pulses obtained at different values of T C IR (the other parameters remaining unchanged).

A. Walsh, Appl. Optics, 7,1259 (1968). Β. V. L'vov, Opt. i Spek. 19, 507 (1965). R. Woodriff, R. W. Stone and A. M. Held, Appl. Spectrosc. 22,408 (1968). A. Walsh, Proceedings of the Tenth International Spectroscopy Colloquium, pp 127-142. Spartan B o o k s : Washington (1963). G. G. Lebedev and Β. V. L'vov, Zav. Labor. 34,1139 (1968). Β. V. L'vov and A. D . Khartsyzov, Zh. Prikl. Spektr. 11, 9 (1969). Β. V. L'vov and A. D. Khartsyzov, Zh. Analyt. , Mosk. 2 4 , 799 (1969). N. P. Penkin, J. Quant.

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