1970
DOI: 10.1021/ac60290a014
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Physical basis of atomic absorption spectrometry. II. Influence of temperature gradients on spatial distribution of neutral atoms in the long pathlength cell

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Cited by 21 publications
(2 citation statements)
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References 20 publications
(17 reference statements)
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“…From the linear velocity of carrier in the discharge tube of 20 cm/ms at 3.8 Torr and 23 °C, the half-lives of the neutral cadmium and iron atoms, for example, can be calculated to be 0.6 and 0.05 ms, respectively. The half-lives of neutral atoms decrease in the order Cd > Zn > Mg > Co > Cu > Fe, quite similar to those observed in the long pathlength cell employed for flame atomic absorption (9).…”
Section: Resultssupporting
confidence: 69%
“…From the linear velocity of carrier in the discharge tube of 20 cm/ms at 3.8 Torr and 23 °C, the half-lives of the neutral cadmium and iron atoms, for example, can be calculated to be 0.6 and 0.05 ms, respectively. The half-lives of neutral atoms decrease in the order Cd > Zn > Mg > Co > Cu > Fe, quite similar to those observed in the long pathlength cell employed for flame atomic absorption (9).…”
Section: Resultssupporting
confidence: 69%
“…Source radiation from a hollow cathode lamp (HCL) passed through the absorption cell and then through focusing optics onto a spectrograph. Compared to conventional flame AAS, they were able to increase the sensitivity for some elements by about 2 orders of magnitude (2,3). Other work using this long * To whom correspondence should be sent.…”
Section: Introductionmentioning
confidence: 99%