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basic medium yielded the dianionic dithiocarbimate ligands as
potassium salts (Scheme 2).
[STDC1]2ꢀ and [ReN(STDC1)2]2ꢀ also support the assignments
made for the experimental IR spectra (ESI). The shapes and energies
for the frontier orbitals for the [STDC1]2ꢀ and [ReN(STDC1)2]2ꢀ
(DFT-calculated, Fig. 6) are also given. These are of interest to
explore in the context of the fact that UV–Vis spectroscopy of the
Re(V) compound could be observed experimentally and showed
strong absorption bands in the 250–350 nm region of the spec-
trum. Encouraged by these calculations the involvement of such
frontier orbitals in the transitions responsible for fluorescence
emission spectra was also evaluated. Whilst for the simple com-
plexes bearing the [SDTC1]–[SDTC3] anionic ligands the fluores-
cence was rather weak, the fluorescence emission spectrum of
the potassium salt of the SDTC4 free ligand was observed (Fig. 2
and ESI). Interestingly, the fluorescence emission quenching upon
metallation with Re(V) and the formation of the [ReN(SDTC4)2]2ꢀ
complex dianion occurred in CH3CN solutions (ESI). This loss of flu-
orescence emission may well be as a result of non-radiative path-
ways due to the dynamic equilibria between canonical forms A/B
(shown in Scheme 1) of the coordinating ligand becoming involved
in solutions. Also, the presence of traces of paramagnetic rhenium
species forming in aerated solution during the analysis could not
be fully discounted at first, therefore the kinetic stability tests in
aqueous environment were carried out: spectroscopic evaluations
of compounds of this class showed a remarkable kinetic stability in
water media (Fig. 3B). The complex [ReN(SDTC2)2]2ꢀ proved to be
stable in CH3CN:H2O with the UV–Vis spectra showing little
change over this period. Taking the shape and energies of
HOMO-LUMO calculated by DFT for SDTC1 and [ReN(SDTC1)2]2ꢀ
in the simplified gas phase models (using a wide variety of basis
sets and conditions, ESI), it is feasible to assume that these frontiers
orbitals are involved in the observed electronic absorption bands
and in the occurrence of fluorescence [51]. The higher energy gap
between the HOMO and LUMO orbitals in the complex compared
to the ligand can indicate that the metal-to-ligand charge transfer
associated to the fluorescence process is not as favored resulting
in a quenching of the fluorescence intensity. Furthermore, the stabil-
ity study of the tolyl complex, [ReN(SDTC2)2]2ꢀ monitored in an
organic solvent (CH3CN) in the presence of water over a period of
6 h was also conducted showing promising kinetic stability compat-
ible with its intended pre-clinical aims. Longer term we are inter-
ested in setting the foundations for the Re(V) radiochemistry
labelling which requires aqueous conditions. As such, prior to
engaging in extensive ‘hot’ experiments using 186/188Re we have
been establishing the ‘cold’ chemistry protocols hereby, and fluores-
cence spectroscopy proved to be a helpful tool in assessing the nec-
essary compatibility and kinetic stability in aqueous solutions.
A significant fluorescence emission was observed for the dian-
ionic ligand with the naphthyl backbone (denoted SDTC4) with
excitation and emission in the UV region of the spectrum (Fig. 1).
Interestingly, the excitation and emission spectra also showed
peaks of lower intensity in the NIR region (650–700 nm). The fluo-
rescence emission in this region is especially attractive for biomed-
ical imaging as interference from tissue autofluorescence in vitro
and in vivo substantially decreases in the NIR.
The reaction of the ligands with rhenium nitride precursors
results in bis-substitution of the dithiocarbimate ligand, and in
the formation of a dianionic rhenium(V) complex of the type
[ReN(SS)2]2ꢀ (Scheme 3).
The desired complexes featuring the [ReN]2+ (Re(V)) core were
obtained either from the [ReNCl2(PPh3)2] or [ReNCl2(PPhMe2)3]
by refluxing in methanol with the ligands and adding PPh4Br to
generate the counter-ion. The negative ESI TOF mass spectra
obtained for the [ReN(SDTC3)2]2ꢀ complex show peaks for the pro-
tonated complex, [M+H]ꢀ, but also for the dianionic species, m/z
corresponding to [M]2ꢀ. The ESI TOF results obtained for the com-
plex [ReN(SDTC4)2]2ꢀ, however, only showed the dianionic species
[M]2ꢀ (see ESI).
Furthermore, the UV–vis spectra of the prepared rhenium com-
plexes are summarized in Fig. 3(A) as well as the corresponding
stability test in aqueous media for [ReN(SDTC4)2][PPh4]2 is given
in Fig. 3(B). The absorption maxima is maintained at ca. 270–
280 nm and in the case of SDTC4, the bands above 300 nm are
not observed in the complex.
Interestingly, a search in the literature confirmed that the
reported X-ray crystal structures for rhenium nitride complexes
with bidentate S-donor ligands are scarce (vide infra). Among these,
only a handful display a square pyramidal geometry like the com-
pounds described herein. Other examples including those with
additional phosphine ligands and adopting a pseudo-octahedral
geometry [40–42] or multimetallic complexes [43–49] are outside
the scope of this discussion and consequently not included here.
The closest examples to the complexes prepared in this work
are depicted in Fig. 4. In all examples, the Re-N nitride distances
are practically identical while the Re-S distances vary more with
the type of ligands. The dithiolate derivative, II [15], presents the
shorter Re-S distances followed by the complexes containing
dithiocarbimate ligands, I [50] and [ReN(SDTC1)2][PPh4]2. The
longer distances found are consistent with the likely occurrence
of the canonical form B in Scheme 1. The complex with dithioimi-
dophosphinato ligands, IV [19], presents the longest Re-S distances
with values around 2.4 Å (Fig. 4). The ORTEP representation of the
[ReN(SDTC1)2][PPh4]2 complex acquired using synchrotron X-ray
radiation is represented in Fig. 5 and a summary of the most rep-
resentative structural parameters is listed in Table 1.
3. Conclusions and outlook
Additionally we carried out investigation by DFT calculations on
the binding of the anionic ligands to the [ReN]2+ core. For the
model ligand SDTC1, and the corresponding dianionic complex,
gas phase DFT optimizations using a variety of basis sets under
Gaussian platforms were employed. In each case, as expected for
these bonding models, there are delocalized bonding throughout
which appeared to be favored for both the experimental structure
and the model compounds. The optimized (Fig. 6, Table 2 and ESI)
geometries are in agreement with the findings from X-ray diffrac-
tion studies on [ReN(SDTC1)2][PPh4]2 and other literature data
[15,19,50] and Figs. 4 and 5.
Key structural data for the experimental structure, species mod-
elled as well as the partial charge distributions estimated are also
given in the Supporting Information.
Molecular parameters are in agreement with those resulting
from the X-ray structural data and the calculated IR spectra
The synthesis of new ligands and their [ReN]2+ core-tagged
complexes was described herein. The characterization data in solu-
tion and in the solid state as well as the crystal structure of the
metal complex [ReN(SDTC1)2](PPh4)2 are given. This compound is
representative of the series and incorporates the phenyl sulfon-
amide backbone: its geometry was discussed and compared to
DFT level gas-phase calculations. Additional highlights are the fact
that the free dianionic ligand SDTC4 isolated as a potassium salt is
fluorescent in wet solvents, however, it is clear that quenching has
taken place upon its coordination to the Re(V) centre. New coordi-
nation chemistry of Re(V) in wet organic solvents was developed
hereby and opens up the possibility of generating complexes
including the [S(O)2N] moiety known for playing a role in the
selective reductive trapping of related compounds in hypoxic cells
and tissues: further work in this context is currently in progress in
our laboratories.