Page 347 - Tandem Techniques
P. 347

Page 331

            usually formed by the secondary ion process, such as (M+H)  and (M+Ag) , from thin layers of sample
                                                                                    +
                                                                      +
            deposited on a metal substrate such as silver. The use of other materials as a substrate, such as
            nitrocellulose, can improve the ionization efficiency for very high molecular weight samples. To
            employ this method of ionization in an LC/MS tandem instrument, the sample must be presented to the
            ionization source as a dry film on a solid carrier, and therefore requires the use of a transport interface.


            Fast Atom Bombardment (FAB)

            Fast atom bombardment spectrometry is an extension of the secondary ion mass spectrometry, and the
            principle of the ionization process is shown in Figure 9.1.



















                                                          Figure 9.1
                                           The Fast Atom Bombardment Ionization Source
            A beam of energetic particles is generated and directed onto the sample, which is carried as a thin film
            on a clean metal support. The secondary ions that are produced are extracted by a suitable ion optical
            arrangement into the mass spectrometer analyzer. The impact of an ion striking the surface produces an
            intense thermal spike. The energy from this thermal spike is then dissipated through the outer layers of
            the sample. In the original device developed by Barber [1], neutral atoms of argon and xenon were
            used, but eventually these were replaced by charged ions such as Ce  and Xe . If a dry sample is used,
                                                                                      +
                                                                             +
            the surface becomes damaged by the intense incident beam, and the yield of secondary ions rapidly
            decreases.
   342   343   344   345   346   347   348   349   350   351   352