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tion[10] and atmospheric pressure chemical ionization
(APCI).[11]
A certain degree of oxidation is also observed for these
compounds, but no signal corresponding to a reduced species
is detected. Molecules with a variety of functional types were
also subjected to LTP and their product ions were analyzed by
mass spectrometry (Table S1 in the Supporting Information).
Similar to the results shown in Figure 2, reduction by
dihydrogenation was observed for arenes but not for other
types of compounds, even those having functional groups
susceptible to reduction. It is also remarkable that under the
LTP conditions, the reduction of benzene stops after the
addition of two hydrogen atoms to form cyclohexadiene
products (C6H8), in spite of the fact that complete hydro-
genation is thermodynamically more favorable once the
aromatic system is destroyed.[12]
Figure 3. LTP mass spectra of benzene with: A) a discharge chamber
containing a silicon wafer surface exposed to the plasma, and B) a
À
discharge chamber containing an Si H-modified silicon wafer exposed
to the plasma.
To elucidate the reaction mechanism, efforts were
directed at finding the source of the added hydrogen.
Hydrogen atoms from benzene, trace molecules in the
environment, and adsorbate on the discharge surfaces are
all possible contributors to the reduction. The possibility of
benzene itself acting as the hydrogen source was precluded by
analyzing the LTP mass spectrum of hexadeuterobenzene
(C6D6, Mr = 84). If hydrogen was provided from benzene, the
reduction product ions should appear at m/z 88 (addition of
two deuterium atoms). However, the base signal occurs at
m/z 85 with ions at m/z 86 and 84 of much lower abundances,
but no signal at m/z 88 (Figure S2 in the Supporting informa-
tion). The observation of abundant ions of m/z 85 is most
likely due to back exchange of deuterium to hydrogen from
hydrogen was the terminating group.[14] The corresponding
mass spectrum of benzene after LTP treatment is shown in
Figure 3B. As expected, the intensity of the MC ions of
+
benzene (m/z 78) decreases significantly, while ions corre-
+
sponding to the reduction product [M+2H]C (m/z 80)
become the base signal. The above results indicate that
benzene reduction involves hydrogen atoms covalently bound
to the discharge surface.
A surface-assisted benzene reduction pathway is pro-
posed, as shown in Scheme 1. The efficient diffusion of
electrons from the plasma to the surface means the discharge
surface is negatively charged.[15] Electrons with low binding
energies (ca. 1 eV) are adsorbed onto the discharge surface
and can diffuse across it or recombine with positively charged
entities. In the first step of the reduction, the adsorbed
benzene molecule is proposed to capture an adsorbed
electron in its vicinity on the discharge surface, thereby
giving rise to an adsorbed benzene radical anion intermediate.
The proposed next step for the reduction of benzene involves
charge neutralization by reaction of the benzene radical anion
with a positively charged group on the surface, which provides
a hydrogen atom for the first proton addition step. One
+
the initially formed dihydrogenation product ([C6D6+2H]C )
at m/z 86. The possibility of hydrogen arising from chemicals
in the surrounding environment such as water and methanol
(a common solvent) is highly unlikely. This is evident from the
fact that after feeding deuterated water or methanol into the
plasma system during the LTP treatment of benzene, the
dominant signal was still at m/z 80 (Figure S3 in the Support-
ing Information). The chance that surface physisorbed water
may contribute was also ruled out by using properly baked
discharge surfaces.
Based on the above results, the only remaining hydrogen
source is the discharge surface, which is made of glass. Since
glass is terminated by silicon-bound OH groups,[13] it can
potentially provide hydrogen atoms for reduction. To test this
possibility, two thin sections of silicon wafer were inserted
into the discharge chamber to cover the glass slides which
comprise the surfaces at the top and bottom of the chamber.
In this case, the glass slides still functioned as a dielectric
barrier to maintain a stable plasma, but it is the silicon wafer
with a surface terminated with silicon atoms that is exposed to
the plasma. The corresponding LTP mass spectrum of
benzene is shown in Figure 3A. The base signal is now the
molecular ion of benzene at m/z 78, with the reduction
product at m/z 80 appearing in relatively lower abundance.
Since the entire area of the discharge chamber was not
covered by silicon, the exposed glass surface might contribute
to the observation of ions at m/z 80. To confirm the role of
covalently bound surface hydrogen atoms in the reduction of
benzene, the silicon wafer surface was modified so that
possible donating entity in the case of the glass surface is
+
À
(···Si OC···H) . The addition of a second electron followed by
another proton will form the cyclohexadiene product, which
could be collected as such or ionized in the plasma to yield the
+
observed [M+2H]C ions. GC/MS analysis of the benzene
reduction products showed 1,4-cyclohexadiene as the major
reduction product, in a yield 2.5 times greater than that of the
co-product 1,3-cyclohexadiene. It is likely that some 1,3-
cyclohexadiene is formed from 1,4-cyclohexadiene as a result
of isomerization promoted by its greater stability.[16] The
Scheme 1. Mechanism for the surface-assisted reduction of benzene in
an LTP. Benzene molecules are adsorbed (ads.) on the discharge
surface during reduction and this is followed by desorption of the
reduction products into the gas phase.
2018
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2009, 48, 2017 –2019