COMMUNICATION
cific examples of cyclic thiouronium [Tf2N] ionic liquids
were not reported, being the object of this investigation.
The approach revealed to be general and allowed for the
synthesis of a variety of cyclic thiouronium imides by vary-
ing either the alkylating agent or the starting thione struc-
ture.
More in detail, the 1-alkyl-3-methylimidazolyl-2-thiones
were obtained by reacting the respective 1,3-dialkylimidazo-
lium halide salts with sulfur, under basic condition in reflux-
ing methanol. Subsequently, the thiones were alkylated with
alkyl iodides. The obtained iodide were not isolated, but di-
rectly extracted with water followed by metathesis with
alkyl substituents at the cation caused the suppression of
a clear melting temperature, and only glass transitions were
observable (rows 4,6,7 in Table 1). Moreover, comparing the
melting point of 2a (glass transition at À788C) with the one
of [C6mim]ACTHUNGTRENNUNG
the cyclic thiouronium head group decreases the tendency
for crystallization. To assess the thermal stability of the pre-
pared cyclic thiouronium salts, a TG analysis at 10 KminÀ1
heating ramp was carried out. Despite the fact that this
method tends to overestimate the thermal stability and is
not able to distinguish between thermal decomposition and
ionic liquid evaporation,[18] the obtained data indicate suffi-
cient thermal stability for most typical IL applications.
As mentioned at the beginning, XPS was employed for
electronic structure characterization of the thiouronium ILs,
particularly of IL 1a. XPS has been found to be an extreme-
ly powerful tool for studying ILs under well-defined ultra-
high vacuum conditions,[19] and we applied this methodology
to evaluate the core-level binding energy shifts that reflect
differences in electronic structure. The aim of this study was
to understand to which extent the sulfur of the thio-alkyl
moiety is involved in the delocalization of the positive
charge originally present on the imidazolium core. For the
purpose of this study, we compared the ILs shown in
Scheme 2.
LiACHTUNGTRENNUNG[Tf2N]. The final thiouronium [Tf2N] salts were obtained
in yield ranging from 62% for 1d to 95% for 2a (see the
Supporting Information). They were all room temperature
ionic liquids. A number of key properties is summarized in
Table 1. For comparison, also the properties of the related
and well known ILs 1-methyl-3-ethylimidazolium [Tf2N]
Table 1. Physicochemical data of selected cyclic thiouronium imide ILs
in comparison to [C2mim]ACTHNUGTREN[NUNG Tf2N] and [C2C1mim]ACHTGNUTRENNUNG
Ionic liquid
m.p.
[8C]
Decomposition
Density[b]
[gcmÀ3
point[a] [8C]
G
N
]
A
R
À17[c]
439
441
368
310
282
320
314
36
77
114
81
88
121
184
1.52[c]
1.48[c]
1.52
1.44
1.44
E
ACHTUNGTRENNUNG
25[c]
1a
1b
1c
1d
2a
À13
3 is a structural isomer of 1a, containing the sulfur atom
as part of a thioether group within the 1-alkyl side chain,
and [C2mim]ACTHNUGTRENUNG[Tf2N] (4) can be considered as the parent com-
pound of 1a, with the C2 position remaining unsubstituted.
In Figure 1, the C 1 s, N 1 s, and S 2p1/2, 3/2 XP spectra of ILs
1a, 3, and 4 are shown. All three compounds contain the
À84[d]
11
À85[d]
1.32
1.39
À78[d]
[a] Off-set temperature, heating rate 10 KminÀ1. [b] At 208C. [c] Data ac-
cording to Ref. [16]. [d] Glass transition.
([C2mim]
ACHTUNGTRENNUNG[Tf2N]) and 1,2-di-
methyl-3-ethylimidazolium
[Tf2N] ([C2C1mim]
reported.
ACHTUNGTRENNUNG[Tf2N]) are
The methyl substituted thio-
uronium IL 1a has a higher vis-
cosity compared with its 1,3-di-
alkylimidazolium counterpart
(rows 1 and 3 in Table 1). In
fact, [C2mim]ACHTUNGTRENNUNG[Tf2N] has a viscos-
ity of 36 MPas at 208C, versus
a viscosity of 114 MPas mea-
Scheme 2. Structures and marked atoms of the ionic liquid used for XPS-investigations.
sured for 1a. Interestingly, by
attaching a C3 alkyl chain to
the thiouronium sulfur atom (ILs 1b and 1c) the viscosity
drops and was comparable to the methyl substituted salt
and even for the octyl substituent the viscosity remains as
low as 121 MPas. Remarkably, the introduction of the thio-
alkyl moiety had only a minor effect on the melting points
of the resulting ILs. In sharp contrast to the increase in
melting point induced by methylating the C2-position of the
imidazolium cation (see entries 1 and 2 in Table 1), the at-
tachment of the S-CH3 group in the same position causes
almost no change in melting point. Elongating one of the
[Tf2N]À anion, giving rise to Canion, Nanion, and Sanion peaks at
identical binding energies (BE) of 292.7, 399.3 and 168.8 eV
(S 2p3/2), respectively. These values serve as internal BE ref-
erence with 0.1 eV accuracy over the whole BE range
(within each region, cation- and anion-derived BEs, for ex-
ample, Nimid relative to Nanion, can be derived within 0.03 eV
accuracy). The most remarkable finding is the BE of sulfur
attached in 2-position of thiouronum 1a: its BE is shifted by
1.0 eV towards higher BE as compared to the thioether S 2p
signal of the IL 3 cation. This difference is very large for an
Chem. Eur. J. 2012, 18, 8288 – 8291
ꢃ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
8289