A series of GdVO4: Sm 3+ , Eu 3+ reddish-orange-emitting nanophosphors were successfully prepared by a simple one-step hydrothermal method. X-ray diffraction (XRD), field emission scanning electron microscope (FESEM), energy-dispersive X-ray spectrometer (EDS), transmission electron microscope (TEM), photoluminescence (PL) spectra, fluorescence lifetime, PL quantum-efficiency (QE) and vibrating sample magnetometer (VSM) were utilized to characterize the as-prepared samples. The results
10show that the individual Sm 3+ or Eu 3+ ions activated GdVO4 phosphors exhibit excellent emission properties in their respective regions and the bright blue light from VO4 3group can be observed under the excitation of ultraviolet (313 nm). The emission intensity of Sm 3+ singly activated GdVO4 phosphors reaches the maximum when the content of Sm 3+ is 0.025, of which the critical distance (RSm-Sm) is calculated to be 18.42 Å. Strong reddish-orange emissions can be seen in Sm 3+ and Eu 3+ ions co-doped 15 GdVO4 phosphors under ultraviolet light irradiation. In addition, the energy transfer phenomenon from Sm 3+ to Eu 3+ ions is clearly observed in GdVO4: Sm 3+ , Eu 3+ , which is confirmed to be an electric quadrupole-quadrupole interaction and the energy transfer efficiency can reach a maximum at 92.5%. More significantly, the color becomes more saturated with the increasing of Eu 3+ or Sm 3+ ions content. Moreover, the as-prepared samples exhibit paramagnetic properties at room temperature. This type of 20 multifunctional reddish-orange-emitting nanophosphor has promising applications in the fields of UV/n-UV WLEDs and biomedical science. 65 transfer from Sm 3+ ions to Eu 3+ ions. Moreover, Ln 3+ ions doped GdVO4 nanocrystals can function as multifunctional materials for their promising applications in biomedical field ascribed to the high magnetic moment and isotropic electronic ground state 8 S7/2 of Gd 3+ ions. So it is highly valuable to prepare GdVO4: Sm 3+ , 65 the latter is O 2--V 5+ CT, which corresponds to the transitions from the 1 A2( 1 T1) ground state and to 1 A1( 1 E) and 1 E( 1 T2) excited state of VO4 3group in the view of molecular orbital theory 35 . Furthermore, there are some weak absorption peaks resulting from f-f transitions within the 4f 6 configuration of the Eu 3+ ions 70 from the 7 F0 ground state to the 5 D4 (363 nm), 5 G3 (377 nm), 5 L7 (384 nm), 5 L6 (396 nm), 5 D3 (418 nm), 5 D2 (467 nm) excited states can be discovered. It can be clearly found that the f-f transitions of Eu 3+ from 350 nm to 470 nm match well with the n-