S. Wang et al. / International Journal of Mass Spectrometry 376 (2015) 6–12
9
of the single imaginary frequency (i211.75 cm−1) corresponds to
˚
extension of the N6 S5 bond (3.380 A) accompanied with oscilla-
˚
˚
INC is an interesting and important intermediate in the gas
phase chemistry, and various chemical reactions may occur either
in the ionic fragment alone or between the two partners prior to its
final separation [16,17,34]. Interestingly, the calculated electronic
excitation energy is negative (−0.6215 eV) for inc1, indicating that
inc1 can spontaneously undergo electron excitation along with
electron transfer to generate the triple inc1-t, consisting of a p-
tolylsulfinyl radical and an aniline radical cation. The triple inc1-t
lies 65.2 kJ mol−1 below the singlet one in free energy. The more
stability of inc1-t is attributed to the two stronger intramolecular
´
´
´
˚
˚
˚
hydrogen bonds (2.216 A and 2.216 A in inc1 versus 2.134 A and
´
˚
2.053 A in inc1-t) and the more p– conjugation of the N6 C7 bond
´
˚
´
˚
Fig. 2. The CID–MS spectra of (a) [9 + H]+, and (b) [10 + H]+.
(1.348 A in inc1 versus 1.328 A in inc1-t). Decomposition of inc1
and inc1-t affords the tosyl cation (a-1IP, m/z 155) and the aniline
radical cation (a-2IP, m/z 93), respectively.
Alternatively, the two partners in inc1 can undergo the cou-
pling reactions between the sulfonic group and the aniline ring,
and afford protonated toluenesulfinates (e.g. 1c), accompanied with
migration of the activated hydrogen (the ipso-H on the analinic
ring) to the sulfinyl O12. Due to the different coupling site (ortho,
meta, and para) at the aniline ring, there are three potential iso-
meric species of protonated toluenesulfinates (1c, 2c and 3c) via
the transition state of inc1-TS1, inc1-TS2 and inc1-TS3. As shown in
Fig. 4, all these transition states show a shortening O11–C distance
tion reactions (Scheme 2), DFT calculations have been preformed
at the B3LYP/6-311 + G(d,p) level of theory for fragmentation of the
typical [1 + H]+. Fig. 3 displays a potential energy diagram for the
dissociation reactions as presented in Scheme 2, and the details
structures of the corresponding species are available as Fig. 4 and
Supplementary Fig. 2S.
To begin the mechanistic investigation on the oxygen transfer
in fragmentation of [1 + H]+, we should first identify the original
tion sites for compound 1: (i) protonation at the sulfonamic N6 to
generate the ionic species a and (ii) at the tosyl O11 (or O12) to
afford b. The calculated free energy of a is 36.5 kJ mol−1 lower than
that of b, indicating a much more preferred protonation site of the
sulfonamide N atom [17]. The sulfonamide N is also reported by the
NMR investigation to be preferably protonated in solutions [30–33].
Noteworthy, inter-conversion between a and b is difficult to occur
via 1,3-proton transfer, due to a considerable energy barrier (a-TSb)
˚
˚
˚
(2.248 A in inc1-TS1, 1.706 A in inc1-TS2 and 2.699 A in inc1-TS3) in
structure. It should be noteworthy that this process involves migra-
tion of the tosyl O11 atom and reduction of the tosyl S5 atom. Also, a
can directly undergo an intramolecular tosyl oxygen transfer reac-
˚
tion (a-TS2) to afford 1c, via breakage of the N6 S5 bond (2.837 A)
˚
and coupling of the tosyl oxygen with the phenyl ring (1.931 A for
the O11–C8 distance).
The subsequent dissociation of 1c (2c or 3c) via the breakage of
the S5 O11 bond leads to completion of the tosyl oxygen transfer
to the aniline ring, and affords the product ions of the proton-
ated quino-imines (e.g. 1c-1IP, m/z 108) and the hydroxyaniline
radical cations (e.g. 1c-2IP, m/z 109) in two competing reaction
channels, respectively. Here, 1c was selected as an example to illus-
trate the two competing dissociation channels. The subsequent
charge-directed decomposition of 1c leads to an INC of inc2 via
the transition state 1c-TS1. Direct separation of inc2 affords the
protonated 6-iminocyclohexa-2,4-dienone (1c-1IP, m/z 108).
The mobile H8 in inc2 can also be effectively transferred to
of 133.7 kJ mol−1
Protonation at the sulfonamide N6 in a weakens the N6 S5
.
˚
bond, as indicated by the lengthened bond length (1.635 A in
˚
b versus 2.073 A in a). Cleavage of the N6 S5 bond in a, upon
complex (INC) consisting of a tosyl cation and a neutral aniline,
which surmounts an energy barrier of 98.4 kJ mol−1 via the transi-
tion state of a-TS1. As for the optimized structure of a-TS1 (Fig. 3),
which has not been obtained previously [17], the vibrational mode
,
which results in formation of another ion–neutral complex (inc3).
Analogous to inc1, the triple state (inc3-t) of inc3 is thermo-
dynamically more stable than the corresponding singlet one by
63.5 kJ mol−1. As shown in Fig. 4, there are two intramolecular
hydrogen bonds in both inc3 and inc3-t, with the types of N H. . .O
negative one (−2.3467 eV), and thus inc3 is spontaneously con-
verted to the triple state one along with electron transfer between
the two partners of the INC. Decomposition of inc3-t results in the
2-aminophenol radical cation (1c-2IP, m/z 109).
As shown in Fig. 3, the energy barrier of the four tosyl trans-
fer processes follows the order of 2c-TS1 (128.9 kJ mol−1) ∼ a-TS2
(128.1 kJ mol−1) > 1c-TS3 (77.8 kJ mol−1) ∼ 3c-TS1 (75.8 kJ mol−1).
migration in the CID process, rather than a direct transfer (via
a-TS2). The order of prior site for most for the tosyl oxygen trans-
fer is ortho ∼ para > meta site in the anilinic ring. Analysis of the
potential energy diagram in Fig. 3 indicated that the INC-mediated
Fig. 3. The potential energy diagram for the oxygen transfer in dissociation of
[1 + H]+.