atoms (such as Ar, He, Xe) of high velocity. A later development was the use of a beam of
caesium (Csþ)ionsandthetermliquid secondary ion mass spectrometry(LSIMS) was
introduced to distinguish this from FAB–MS.Pseudomolecular ion speciesarise as either
protonated or deprotonated entities (MþH)þand (MH)respectively, which allows
15
27
32
41
42
43
28
29
58
% relative abundance
(b)
10
0
20 30 40 50 60
10
20
30
40
50
60
70
80
90
100
m/z
(a) CH 3 CH 2 CH 2 CH 3
CH 3 CH 2 CH 2 CH 3 ¬+.
+e–
CH 3 CH 2 CH 2. + CH 3.
CH 3 CH 2. + CH 3 CH 2 ¬+
¬+
CH 2 ¬+
CH¬+
C¬+
m/z=15
m/z = 29
CH 2 CH¬+
m/z= 27
CH 3 ¬+
m/z= 15
CH 2 ¬+
m/z= 14
CH 3 CH 2 ¬+
m/z= 29
CH 3 CHCH¬+
¬+
m/z= 41
m/z= 43
etc. etc.
CH 3 + CH 3 CH 2 CH 2
Fig. 9.3Fragmentation pathways inn-butane and the EI spectrum. The pathway for fragmentation of
n-butane is shown in (a) and the EI spectrum in (b). In the spectrum, the relative abundance is plotted
from 0 to 100% where the largest peak is set at 100% (base peak). Spectra represented in this way are
said to benormalised.
357 9.2 Ionisation