PENG Hong-shang, SONG Hong-wei, CHEN Bao-jiu, WANG Ji-wei, L&#220; Shao-zhe, HUANG Shi-hua. Remarkable Spectral Difference between Nanocrystalline Y<sub>2</sub>O<sub>3</sub>:Eu<sup>3+</sup> and Bulk Ones[J]. Chinese Journal of Luminescence, 2003,24(5): 531-534
PENG Hong-shang, SONG Hong-wei, CHEN Bao-jiu, WANG Ji-wei, L&#220; Shao-zhe, HUANG Shi-hua. Remarkable Spectral Difference between Nanocrystalline Y<sub>2</sub>O<sub>3</sub>:Eu<sup>3+</sup> and Bulk Ones[J]. Chinese Journal of Luminescence, 2003,24(5): 531-534DOI:
Remarkable Spectral Difference between Nanocrystalline Y2O3:Eu3+ and Bulk Ones
spectral difference between nanocrystalline yttria doped with europium (Y
2
O
3
:Eu
3+
) and the bulk ones was reported. Besides a 580.6nm line similar to that in the bulk Y
2
O
3
:Eu
3+
a new broad excitation line at 579.9nm was observed in the excitation spectra of nanocrystals (NCs). The 579.9nm peak relative to the 580.6nm one decreases a little as temperature increases. The fluorescent lifetime excited by 579.9nm line became slightly shorter than that of the 580.6nm line. We suggest that in nanocrystalline Y
2
O
3
:Eu
3+
the broader 579.9nm excitation peak originates from the luminescence of Eu
3+
ions near the surface
and the 580.6nm one from the internal Eu
3+
ions. The surface to volume ratio is quite small (1%) in the micrometer particles
while it increases significantly as the particle size decreases to several nanometers. This will lead the surface effects to be effective. As well known
the energies of electrons in 4f states of rare earth ions are affected by the crystal field. In nanocrystals
rare earth ions near the particle surface are at the sites microscopically inequivalent with those close to the center. Their energy levels may shift
and the degenerated spectral lines in the bulk sample may split. Due to the appearance of numerous surface defects the crystal field in the surface of nanoparticles degenerates and the emission of 5D
o
7
Fj
shifts. Because the local environments surrounding Eu
3+
ions near the surface are more disordered and surface defects may act as nonradiative transition channels
the width of the 579.9nm line is broader and the fluorescent lifetime becomes shorter.