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Figure 4. (a) UV-vis absorption (solid line) and fluorescence (dash line)
spectra of [8]CN (black), [9]CN (red), and [12]CN (blue). (b)
Luminescent photographs of [8]CN (yellow), [9]CN (green), and
[12]CN (blue) in THF under UV irradiation at λ = 365 nm.
pulsed laser system in degassed THF solutioDnOaIt: 1r0o.o10m39t/eCm7CpCe0ra7t3u7r0eD.
The fluorescence decay of [n]CNs followed first-order kinetics with a
lifetime (τ) = 5.3 ns for [8]CN, 1.7 ns for [9]CN, and 1.0 ns for [12]CN,
as measured by the single-photon counting method (Figure 5).
According to the equation kr = ΦF/τ,27 their radiation decay rate
constant (kr) could also be determined to be 4.2 × 107 s-1 for [8]CN,
2.0 × 108 s-1 for [9]CN, and 4.2 × 108 s-1 ns for [12]CN.
Table 1. Absorption and emission data for [n]CNsa
Conclusions
In conclusion, we developed a novel and efficient three-step
synthesis approach to achieve [8]-, [9]-, and [12]CNs nanorings based
on the platinum-mediated assembly of naphthalene units and
subsequent reductive elimination. This synthesis route provides a
good strategy to overcome the strain energy resulting from the
curved structure and successfully achieved the target molecules with
a relatively high yield. This method may open a new way for the
synthesis of [n]CNs from easily prepared starting materials 2 and 5
and facilitate their further utilization in bottom-up synthesis of
uniform CNTs. In addition, their photophysical properties in THF
were experimentally investigated, revealing their unique size-
dependent properties.
a Data obtained at room temperature in THF. b Maximum absorption.
Maximum emission upon excitation at 350 nm. Lifetime.
Fluorescence quantum yields.
c
d
e
The photophysical properties of the [8]-, [9]-, and [12]CNs in
THF were further investigated using UV-vis absorption spectroscopy,
steady-state fluorescence spectroscopy, and time-resolved
fluorescence decay. The absorption and emission spectra are shown
in Figure 4 and the data are summarized in Table 1. Interestingly,
unlike CPPs, which absorb UV-vis light at similar wavelength
regardless of their different sizes,12 the UV-vis absorption spectra of
the [8]-, [9]-, and [12]CNs clearly exhibit size-dependent properties:
The maximum absorption (λabs) were blue-shifted with an increase in
the size of the [n]CNs nanorings. This behavior is consistent with
reports by Itami and coworkers.23 The fluorescence emission
measurements were performed under an excitation at 350 nm, and
all [n]CNs emitted strong fluorescence in a variety of colors (yellow
for [8]CN, green for [9]CN, and blue for [12]CN) in THF solutions). The
fluorescence spectra also exhibit size-dependent properties. With
increasing size of [n]CNs, the maximum emission (λem) were
significantly blue-shifted. The λem peaks are 556 nm, 486 nm, and 463
nm for [8]-, [9]-, and [12]CNs, respectively. The fluorescence
quantum yields (ΦF) of [n]CNs were determined by using anthracene
in ethanol as the reference. The ΦF values are provided in Table 1
and the highest ΦF is 0.42 for [12]CN. Similarly, the ΦF values of
[n]CNs increased with increasing size.
This work was financially supported by the National Key Research
and Development Program of China (2017YFA0402800), the National
Natural Science Foundation of China (51772285, 21473170), and the
Fundamental Research Funds for the Central Universities.
Notes and references
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Figure 5. Luminescent decay profiles of (a) [8]CN, (b) [9]CN, and (c)
[12]CN in THF at 298 K.
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