C O M M U N I C A T I O N S
Figure 1. MALDI-TOF MS spectra of quantum dots 1-3 (left to right), respectively. In the insets are the isotope-resolved patterns experimentally measured
(solid curves) with ones calculated (dotted curves) from the molecular structures of the quantum dots. In the spectra of 1 and 3, the small peaks marked by
asterisks are due to monochlorinated byproducts (M+34) in the last oxidation step.
nanographenes previously reported that contain fewer conjugated
carbon atoms.10a As a result, isotope-resolved MS with mild
ionization methods (e.g., MALDI-TOF) have been the only
applicable techniques for ensemble characterization of large
graphene nanostructures.10 Figure 1 shows the MALDI-TOF MS
results of 1-3, respectively. The comparison with spectra calculated
with the molecular formula of the quantum dots indicates the
elimination of the desired numbers of hydrogen atoms during the
oxidative condensation and the excellent size uniformity achieved
in the quantum dots. The structure of 1 was further confirmed with
infrared vibrational spectroscopy because of its high structural
symmetry and therefore the easy interpretation of the spectrum.8
As expected 1-3 have size- and shape-dependent optical
properties. Figure 2 shows their absorption spectra in dichlo-
romethane. Because of their larger sizes 1 and 3 have absorption
edges appearing at significantly longer wavelengths than 2. In
addition, all the spectra show R, p, and ꢀ bands in the order of
increasing energy from the absorption edges (e.g., marked by arrows
for 1 in Figure 2), a classic pattern observed in many polycyclic
aromatic hydrocarbons.11 The R and p transitions, which in 1 are
only weakly dipole-allowed due to the high molecular symmetry,
become significantly more pronounced in 2 as the symmetry reduces
(details in the Supporting Information), and the ꢀ transition that is
doubly degenerate in 1 appears as two separate bands in 2 or 3
since the reduced symmetry lifts the degeneracy.
both theoretical and experimental studies have shown that novel
electronic and magnetic properties may emerge as results of well-
defined edge structures in graphenes.5 Therefore the graphene
quantum dots may see a wide range of applications in optoelec-
tronics and molecular magnetism.
Acknowledgment. This work is supported by Indiana University
and the National Science Foundation (Grant 0747751).
Supporting Information Available: Detailed procedure for syn-
thesis and characterization of intermediates, IR spectra, and analysis
of UV-vis absorption bands of 1-3. This material is available free of
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Our work demonstrates the versatile synthesis of large, stable
colloidal graphene quantum dots with desired sizes and structures
enabled by a new solubilization strategy. Quantum dots 1 and 3
presented here, in particular, have large extinction coefficients
(Figure 2) in a wide spectral range from UV to near-infrared and,
thus, can serve as a new type of light harvesting media for
photovoltaics.8 We can further reduce the band gap of the graphenes
by increasing their sizes and tune their redox potentials by chemical
functionalization to tailor their properties for the devices. In addition,
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M.; Rader, H. J.; Mu¨llen, K. Macromol. Chem. Phys. 2001, 202, 215. (c)
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Figure 2. UV-vis absorption spectra of quantum dots 1-3 in solution.
Marked by arrows are the R, p, and ꢀ bands of 1, from right to left,
respectively.
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