We have recently observed large cross sections (sigma = 1.8 x 10(-15)
cm2) for electron induced dissociation (EID) of physisorbed cyclohexan
e in multilayers on Pt(111) surfaces. This is a general phenomenon for
hydrocarbon multilayers and for other physisorbed hydrocarbon species
at monolayer or submonolayer coverages. While it is certainly not new
to identify electron induced effects in adsorbed layers, the large EI
D cross sections reported here and their implications for physisorbed
hydrocarbons is not generally appreciated. Two consequences of this ch
emistry are discussed. First, these EID cross sections are so large th
at serious artifacts in temperature programmed desorption (TPD) can be
caused even in the-short time it takes to perform a TPD experiment us
ing a conventional quadrupole mass spectrometer (QMS) which can bombar
d the sample with electron fluxes in the muA regime. This problem in T
PD can be overcome by utilizing a biased grid between the sample and t
he QMS ionizer region to stop low energy electrons. However, the secon
dary electron emission inherent in many electron spectroscopies (XPS,
UPS, AES, etc.) may cause similar effects that are difficult to elimin
ate. Secondly, the large difference in EID cross sections between phys
isorbed and chemisorbed species has the exciting consequence that well
-defined, complex hydrocarbon surface intermediates, e.g., cyclohexyl,
can be prepared cleanly on reactive metal surfaces for chemistry stud
ies.