E. Okutan et al. / Inorganic Chemistry Communications 49 (2014) 1–4
3
systems have been obtained (see Supporting information). The reso-
nances were observed as broad overlapped peaks rather than clear
ABC patterns. To obtain appropriate parameters simulation program
has been also used for the 31P NMR spectra of C60–fullerene derivatives
(2a–4a) (Fig. 2).
Fullerene nanomaterials exhibit extremely low fluorescence effi-
ciencies. Therefore, the synthesis of photoluminescent fullerene
nanomaterials for practical use in different applications is challenging
[9]. To investigate the photophysical properties of C60–phosphazene de-
photon counting (TCSPC) technique in CDCl3, excited at 390 nm. Our
values of the lifetimes were found to be 0.0051, 0.041 and 0.098 ns re-
spectively (see Supplementary data). These results indicate a strong
electronic interaction between phosphazene moiety and the fullerene.
Comparative TGA results of fullerene, synthesized phosphazene de-
rivatives with aromatic side groups (2–4) and all C60–phosphazene con-
jugates (2a–4a). As expected fullerene has no decomposition between
25 and 600 °C. Compound 2 has single step decomposition between
325 and 395 °C with the percent weight loss of 97.5% between 260
and 425 °C. Compound 2a has two step decompositions between 175
and 250 °C (10%) and 355–440 °C (37%) with total weight loss of 42%
at 600 °C. This weight loss is equal to the decomposition of the
phosphazene derivative bonded to the fullerene through pyrrolidino
group. The thermal stability of naphtoxy (3) and pyreneoxy (4)
substituted cyclophosphazenes is higher than the phenoxy substituted
phosphazene (2). Compound 3 starts to lose its functionalities at
370 °C up to 600 °C with a total weight loss of 72%. Compound 3a
shows one-step decomposition of one naphtoxy group and methyl
group between 130 and 180 °C (24%) with a total weight loss of 40%
at 600 °C. This decomposition can be attributed to the loss of naphtoxy
groups on phosphazene ring. Compound 4 has a first step 7% weight loss
170–205 °C and a second step decomposition from 390 to 450 °C with
weight loss of 51%. The pyreneoxy-substituted phosphazene–C60 deriv-
ative (4a) has a two-step decomposition between 130 and 235 °C (15%)
and 390–470 °C (18%). The char yield of the compound at 600 °C is 65%.
The C60 phosphazene derivatives (2a–4a) show better thermal stability
than the phosphazene compounds (2–4) due to the excellent thermal
stability of fullerene. The char yields of the derivatives increases with
the increasing size of the aromatic compounds on phosphazene because
of the higher π–π interaction between aromatic sides and fullerene
which makes derivative more stable.
rivatives, the absorbance and fluorescence emission of C60
–
phosphazene derivatives in chloroform were analyzed. The absorption
spectrum of phosphazene derivatives shows a broad shoulder with
peak maxima for 2a and 3a at 270 nm and 330 nm, and for 4a at 268,
278, 330 and 345 nm in chloroform. The UV–Vis absorption spectra
for pyrene phosphazene (4) and derivatives (C60–pyrene) 4a at almost
same concentration in chloroform are depicted. In fact, the observed ab-
sorption spectrum is close to a superposition of the spectra of typical 4a
and 4 compounds and is consistent with the UV–visible spectra of other
pyrene–fullerene derivatives [19]. The absorption at longer wave-
lengths beyond 400 nm is due entirely to the pyrene–C60 cage [20]. In
fluorescence emission spectra of the C60–phosphazene derivatives 2a–
4a in chloroform (excited at same wavelength, 390 nm), peaks were ob-
served at 448 nm. Pyrene excimer formation is a well-known phenom-
enon in organic solutions. In our previous work hexakis(pyrenyloxy)
cyclotriphosphazene exhibited an intramolecular excimer emission
arising from the non-covalent π–π and CH–π stacking interactions
among the pyrenyloxy moieties which were investigated by fluores-
cence spectroscopy [21]. Compound 4 exhibits a fluorescence maximum
near 448 nm, where most of the incident radiation is absorbed by the
pyrene phosphazene parts and not the fullerene which is coherent
with the previous results. Compound 4a shows a typical pyrene–
phosphazene emission spectrum but the intensity is reduced relative
to that of pyrene–phosphazene by a factor of ~10. Thus, the pyrene
phosphazene fluorescence is almost entirely quenched by the attached
fullerene moiety. The characteristic C60 fluorescence at ~700 nm is too
weak to be observed on our instrument. Fluorescence quantum yields
of compounds 2a–4a were determined by a standard procedure using
2-aminopyridine as standard (ΦF = 0.60). We observed that the quan-
tum yields of compounds 2a–4a are 0.12%, 0.75% and 0.82% respectively.
The lifetimes were also measured with the time correlated single
In this contribution we presented the synthesis of C60–phosphazene
derivatives with covalent linkage between both moieties by an 1,3-
dipolarcycloaddition of phosphazene derivatives having aldehyde
group and fullerene C60 in the presence of sarcosine. For this purpose
we have synthesized phosphazene derivatives which could serve as a
versatile template for designing more efficient donor–acceptor systems.
All compounds were fully characterized by standard spectroscopic tech-
niques. The photophysical behaviors of compounds were studied by
UV–Vis absorption and fluorescence spectroscopies. The fluorescence
Fig. 2. (A) Normal and (B) simulated 31P NMR spectra of compound 4a in CDCl3–CS2.