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               162                                                                        Mass Spectrometry in Forensic Science
































































                      FIGURE 2 Fragmentation of molecules by electron impact. The analyte molecule (M) is bombarded with a beam
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                      of energetic electrons (e ), whereby it loses an electron to become a positively charged particle (M ), feasible for
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                      separation in a magnetic or oscillating electric field.
                 As  shown  schematically  in  Fig.  3  a  proton  donator  methane molecules to generate a stable population of sec-
               formed by EI of the reagent gas (e.g., methane) collides  ondary ions. These in turn react with the analyte gas, a
               in a gas phase with the target substance and then gives  process that results in a gas-phase acid–base proton trans-
               up its proton to the analyte. The reactions occur in two  fer from the secondary ions to the analytes. Since these
               steps. In the first one, the primary ions are formed from  are present in low concentrations as compared with the
               the methane fragments. At a sufficiently high pressure in  concentration of methane, the analytes only seldom col-
               the ionization cell, the primary ions collide with neutral  lide with the electrons, a situation that results in less
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