Codoping with Li + is an efficient method to enhance the photoluminescence of Bi 3+ -Yb 3+ doped Y 2 O 3 phosphors. It suggests a kind of potential method which may be used to improve the solar cell efficiency. OCIS codes: (250.0250) Optoelectronics; (250.5230) Photoluminescence
IntroductionIn single-junction crystalline silicon (c-Si) solar cell, the major energy loss in the conversion of solar energy to electric energy is due to the intrinsic spectral mismatch: low-energy photons cannot be absorbed by the solar cells (subbandgap transmission loss) while high-energy photons cannot be used efficiently (lattice thermalization loss).[1] A promising way to reduce the spectra mismatch losses is to adapt the solar spectrum to better match the solar cell.[2] Thus, shifting of the incident solar spectrum via downconversion using luminescent materials could allow a solar cell to operate at a higher efficiency.[3] Downconversion is to split one higher energy photon to obtain two photons with a smaller energy.[4] It has been calculated that in an ideal case, the energy conversion efficiency of a solar cell can be enhanced from 29% to 38.6% via spectrum shifting. [5] Recently, much attention has been paid to downconversion materials through the energy transfer (ET) between Yb 3+ and other rare-earth ions, such as ion couples of Tb 3+ -Yb 3+ , Tm 3+ -Yb 3+ , Pr 3+ -Yb 3+ , Ce 3+ -Yb 3+ and Er 3+ -Yb 3+ .[6] The Yb 3+ has a relatively simple electronic structure of two energy-level manifolds: the 2 F 7/2 ground state and 2 F 5/2 excited state around 1000 nm in near-infrared (NIR) region, which is located just above the band gap of Si (~1100 nm).[7] However, rare-earth ions as donors feature narrow adsorption line width and low absorption cross-sections for UV-visible photons, resulting in lower direct excitation efficiency and weak NIR emission of Yb 3+ .[8] On this occasion, metal ions with broadband and spin-allowed absorption in the UV-blue region of interest might be an excellent broadband sensitizer for Yb 3+ . So the combination of transition-metal Bi 3+ and Yb 3+ codoped Y 2 O 3 for NIR downconversion luminescence has been exploited, and best ratio is 1% Bi 3+ , 2% Yb 3+ codoped Y 2 O 3 .[5] Bi 3+ have 6s 2 electronic configuration, and the 6s 2 →6s6p transition is also an allowed electric-dipole transition. The emission of Bi 3+ in Y 2 O 3 takes place mainly around 500 nm (the energy is just twice that of the 2 F 7/2 → 2 F 5/2 transition of Yb 3+ ), which suggests the possibility of efficient cooperative energy transfer from Bi 3+ to Yb 3+ .[9] On this basis, dopant of Li + in Y 2 O 3 : 1% Bi 3+ , 2% Yb 3+ sample may be further improving luminescence intensity. Li + with small radius can substitution of larger sized Bi 3+ to enhance downconversion emissions intensities of Y 2 O 3 : 1% Bi 3+ , 2% Yb 3+ due to the distortion of crystal field symmetry of Bi 3+ . [10] In this paper, we reported that codoping x% Li + (x = 0, 1, 3, 5, 7 and 10) in Y 2 O 3 : 1% Bi 3+ , 2% Yb 3+ downconversion powder phosphors are synthesized...