H. Zhu et al. / Materials Research Bulletin 44 (2009) 2033–2039
2039
Fig. 9. (a) UV–vis adsorption spectrum of the In2S3 flowers. (b) PL emission spectra of the above sample (excited by 335 nm).
flowery nanostructures was inhibited and spherical particles with
coarse surfaces came into being in a broad size range. Besides, the
poor crystalinity of them was also detected. When the urea
concentration was increased, enough OHÀ anions were supplied.
These anions may bind on the surface to direct the flowers
fabrication with thinner flakes to a certain extent. For the anions
supply, if NaOH and NH3ÁH2O were selected, due to the local
supersaturation, heterogeneous nucleation occurred and resulted
in flowers in wide size range. When HETA was chosen, uniform
spheres formed due to the homogeneous nucleation. However, due
to the different coordination ability, these spheres linked together
and failed to transform into flowery structures. Similar explanation
was also applicable for the cysteine supply.
final structure and composition control. Urea induced precursor-
decomposition associated with ripening mechanism was proposed
to interpret their shape evolutions. These In2S3 novel architectures
showed a quantum confinement effect in absorption spectra and
exhibited a strong blue emission, which allowed to be utilized as
promising materials for quantum electronic.
Acknowledgements
This work was supported by the National Natural Science
Foundation of China (No. 90713022), the National Key Basic
Research Development Project of China (No. 2007CB714500) and
the Project of Chinese Academy of Sciences (No. KJCX2. Y. W. H09).
3.5. Optical properties of the flowery In2S3
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As a promising semiconductor, its optical properties were also
studied at room temperature. Fig. 9a represented the UV–vis
absorption spectrum of the as-prepared In2S3 microflowers.
Besides a weak broad absorption at 508 nm, a strong peak located
at 291 nm was observed, which obviously revealed their blue shift
compared with the reported data of 620.6 nm for bulk In2S3
materials [16,21]. The flower petals exhibited a thickness of about
20 nm, which was smaller than the Bohr exaction radius of In2S3
(33.8 nm). Consequently, this blue shift phenomenon of the
absorption may be interpreted by the quantum confinement
effect. In addition, we also carried out photoluminescence (PL)
studies to investigate the optical properties of the stacked In2S3
flowers. This hierarchical superstructures showed good lumines-
cence compared with the non-luminescent behavior of bulk In2S3.
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observed as shown in Fig. 9b. The blue luminescence at 484, 420
and 454 nm can be attributed to the presence of several deep trap
states or defects in the structure. The weak green luminescence at
533 nm may be an emission from the indium interstitial sites,
which corresponded to the report of Chen et al. [11].
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