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be emitted by the lamp. If we want to determine Cu in our AAS experiment, the lamp cathode

               must be a copper cylinder; if we want to determine gold, the cathode must be a gold cylinder,

               and so on. The cathode and an inert anode are sealed in a glass cylinder filled with Ar or Ne at
               low pressure (the “filler gas”). A window of quartz or glass is sealed onto the end of the lamp; a

               quartz  window  is  used  if  UV  wavelengths  must  be  transmitted.  Most  HCLs  have  quartz
               windows, because most elements have emission and absorption lines in the UV. Glass can be

               used for some elements, such as sodium, where all the strong absorption lines are in the visible

               region of the spectrum. The HCL emits narrow, intense lines from the element that forms the
               cathode.

                       Applying a high voltage across the anode and  cathode creates this emission spectrum.
               Atoms of the filler gas become ionized at the anode and are attracted and accelerated toward the

               cathode. The fast-moving ions strike the surface of the cathode and physically dislodge some of
               the surface metal atoms (a process called “sputtering”).




















                       The displaced atoms are excited by collision with electrons and emit the characteristic

               atomic emission spectrum of the metal used to make the cathode. The process is shown in Fig.
               The emitted atomic lines are extremely narrow. Unlike continuum radiation, the narrow emission

               lines  from  the  HCL  can  be  absorbed  almost  completely  by  unexcited  atoms.  Using  this  light

               source, atomic absorption is easily detected and measured.
                       Narrow  line  sources  such  as  the  HCL  provide  not  only  high  sensitivity,  but  also

               specificity. If only Cu atomic emission lines are produced by the Cu HCL, there are few species
               other than Cu atoms that can absorb these lines. Therefore, there are few spectral interferences in

               AAS.

                       The emitted spectrum consists of all the emission lines of the metal cathode, including
               many lines that are not resonance absorption lines, but these other lines do not interfere in the

               analysis. Each hollow cathode emits the spectrum of metal used in the cathode. For this reason, a
               different  HCL  must  be  used  for  each  different  element  to  be  determined.  This  is  an

               inconvenience in practice and is the primary factor that makes AAS a technique for determining

               only one element at a time. The handicap is more than offset, however, by the advantage of the
               narrowness of the spectral lines and the specificity that results from these narrow lines.


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