4.8 Article

Er3+-Doped Anatase TiO2 Nanocrystals: Crystal-Field Levels, Excited-State Dynamics, Upconversion, and Defect Luminescence

期刊

SMALL
卷 7, 期 21, 页码 3046-3056

出版社

WILEY-BLACKWELL
DOI: 10.1002/smll.201100838

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资金

  1. Chinese Academy of Sciences (CAS) [KJCX2-YW-358]
  2. NSFC [10804106, 10974200, 51002151]
  3. MOST [2007CB936703, 2009AA03Z430, 2011AA03A407]
  4. NSF of Fujian Province for Distinguished Young Scholars [2009J06030, 2009J05138, 2010J05126]

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A comprehensive survey of electronic structure and optical properties of rare-earth ions embedded in semiconductor nanocrystals (NCs) is of vital importance for their potential applications in areas as diverse as luminescent bioprobes, lighting, and displays. Er3+-doped anatase TiO2 NCs, synthesized via a facile sol-gel solvothermal method, exhibit intense and well-resolved intra-4f emissions of Er3+. Crystal-field (CF) spectra of Er3+ in TiO2 NCs are systematically studied by means of high-resolution emission and excitation spectra at 10-300 K. The CF analysis of Er3+ assuming a site symmetry of C-2v yields a small root-mean-square deviation of 25.1 cm(-1) and reveals the relatively large CF strength (549 cm(-1)) of Er3+, thus verifying the rationality of the C-2v symmetry assignment of Er3+ in anatase TiO2 NCs. Based on a simplified thermalization model for the temperature-dependent photoluminescence (PL) dynamics from S-4(3/2), the intrinsic radiative luminescence lifetimes of S-4(3/2) and H-2(11/2) are experimentally determined to be 3.70 and 1.73 mu s, respectively. Green and red upconversion (UC) luminescence of Er3+ can be achieved upon laser excitation at 974.5 nm. The UC intensity of Er3+ in Yb/Er-codoped NCs is found to be about five times higher than that of Er-singly-doped counterparts as a result of efficient Yb3+ sensitization and energy transfer upconversion (ETU) evidenced by its distinct UC luminescence dynamics. Furthermore, the origin of defect luminescence is revealed based on the temperature-dependent PL spectra upon excitation above the TiO2 bandgap at 325 nm.

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