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For those molecules that can be vaporized without decomposition , EI
is often used to generate ions for mass analysis. As previously discussed,
however, ionization by electrons accelerated through a potential of
70 volts is a highly energetic or "hard" process and may lead to entensive
fragmentation that leaves very little or no trace of a molecular ion.
Because molecular mass and structure are not easily determined in the
absence of a molecular ion, lower energy or "soft" ionization techniques
have been developed based on chemical and desorption ionization.

In contrast to electron ionization, most applications of chemical ionization
(CI) produce ions by the relatively gentle process of proton transfer.
The sample molecules are exposed to a large excess of ionized reagent
gas. Transfer of a proton to a sample molecule M, from an ionized reagent
gas such as methane in the form of CH5+, yields
the [M+H]+ positive ion. For example, the mass spectrum of
ephedrine (top spectrum of Figure 11) shows no molecular ion at m/z
165 under electron ionization conditions. However, under positive CI
conditions (bottom spectrum of Figure 11), the protonated molecule at
m/z 166 and the important fragement ion corresponding to the loss of
water (18 Daltons) have significant intensity. In both spectra an intense
ion is seen at m/z 58 but note that the fragmentation patterns of protonated
molecules, [M+H]+, are not necessarily the same as the fragmentation
patterns of molecular ions, M+.

Negative ions can also be produced under chemical ionization conditions.
Transfer of a proton from M to other types of reagent gas or ions can
leave [M-H]-, a negatively charged sample ion. Addition of
an electron to M, a process facilitated by collisionally decreasing
the energy of electrons generated in the source, can yield an intense
M- ion. Such ions, often the only ion generated, can be used
to detect species by mass spectrometry with great sensitivity.
Desorption ionization is a term used by mass spectrometrists to decribe
the process by which a molecule is both evaporated from a surface and
ionized although the exact mechanism may not be understood. For the
first four desorption ionization methods listed below, samples are desorbed
and ionized by an impact process that involves bombardment of the sample
with high velocity atoms, ions, fission fragments, or photons of relatively
high energy. The impact deposits energy into the sample, either directly
or via the matrix, and leads to both sample molecule transfer into the
gas phase and ionization.
In field desorption, the sample is coated as a thin film onto a special
filament placed within a very high intensity electric field. In this
environment, ions created by field-induced removal of an electron from
the molecule are extracted into the mass spectrometer.

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