Page 36 - An Introduction to Analytical Atomic Spectrometry - L. Ebdon
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                                                          Figure 2.2
                                                    The hollow-cathode lamp.
            with the metal of interest. The lamp is contained within a glass envelope filled with an inert gas
            (usually Ne or Ar) at 1-5 Torr. A potential of about 500 V is applied between the electrodes and, at the
            pressures used, the discharge concentrates into the hollow cathode. Typically, currents of 2-30 mA are
            used. The filler gas becomes charged at the anode, and the ions produced are attracted to the cathode
            and accelerated by the field. The bombardment of these ions on the inner surface of the cathode causes
            metal atoms to sputter out of the cathode cup. Further collisions excite these metal atoms, and a simple,
            intense characteristic spectrum of the metal is produced. Marcus, and Kirkbright and Sargent (see
            Appendix C) describe this action and hollow-cathode lamps in more detail.

            The insulation helps to confine the discharge within the hollow cathode, thus reducing the possibility
            of self-absorption and the appearance of ion lines. Both of these effects can cause bending of calibration
            curves towards the concentration axis. A glass envelope is preferred for ease of construction, but a silica
            window must be used for ultraviolet light transmission. A graded seal between the window and
            envelope ensures excellent gas tightness and shelf-life. A moulded plastic base is used. The choice of
            filler gas depends on whether the emission lines of the gas lie close to useful resonance lines and on
            the relative ionization potentials of the filler gas and cathode materials. The ionization potential of
            neon is higher than that of argon, and the neon spectrum is also less rich in lines. Therefore, neon is
            more commonly used.

            Modern hollow-cathode lamps require only a very short warm-up period. Lifetimes are measured in
            ampere hours (usually they are in excess of 5 A h). A starting voltage of 500 V is useful, but operating
            voltages are in the range 150-300 V. In many instruments, the current supplied to the lamp is
            modulated. Hollow-cathode lamps may also be pulsed or
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