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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

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