The spectral and kinetic characteristics of YAG:Ce,Tb powders (with Tb 3+ concentration varying up to 100%, relative to Y) using cathode-ray and UV excitations were determined. The energy diagram of YAG:Ce,Tb was constructed and energy transfer processes in the compound were studied. The most effective resonance energy transfer takes place at Tb 3+ concentrations of 20%. There is no evidence of Ce 3+ →Tb 3+ energy back transfer for (Y,Tb)AG:Ce even in high resolution spectra. The optimal Tb 3+ content for maximum light output of YAG:Ce,Tb was determined to be 20% and for lowest afterglow 100%.Oxide materials based on garnet structure crystals are promising candidates for scintillator applications. 1 The garnets have good chemical and radiation stability, exhibit excellent mechanical properties, and show efficient luminescence when doped with lanthanide ions. Among other candidates, the Ce 3+ -doped Y 3 Al 5 O 12 (YAG:Ce) scintillator possesses sufficient luminous efficiency, short decay time (∼65 ns), and appropriate density (4.55 g/cm 3 ) comparable to that of CsI (Tl) crystals (4.51 g/cm 3 ). 2 Moreover, the emission located at 550 nm matches well to the Si photoelectric diode detecting range. The long wavelength emission for interconfigurational 5d-4f transitions of Ce 3+ ion in YAG is caused by large crystal field splitting of 5d orbitals. 3 At present, Ce 3+ -doped YAG is the most widely used phosphor in white light LEDs. The combination of (In,Ga)N blue emission and YAG:Ce yellow emission results in bright white light sources. 4 The light yield of YAG:Ce scintillator is less than its theoretical limit, which can be estimated to be 60 000 photons/MeV. 5 However, experimental studies report lower values of ∼ 25 000 photons/MeV. 6 The discrepancy may be related to native host lattice defects (vacancies, anti-sites, dislocations) which trap electrons and holes, thus decreasing the efficiency of energy transfer from matrix to activator or even leading to non-radiative recombination. 6,7 In addition to low efficiency, some afterglow is also observed, which likewise points to a role of defects in the garnets. To compete with trapping by defects, a higher activator concentration may be used; however, this usually leads to concentration quenching.Improving the emission properties of YAG:Ce phosphor can be achieved by incorporation of a co-dopant, in particular Tb 3+ . In some Ce 3+ ,Tb 3+ double doped silicates and perovskites, energy transfer from Ce 3+ to Tb 3+ occurs. 8 Ce 3+ to Tb 3+ energy transfer is also widely applied in phosphors for high quality fluorescent lamps. In order to get efficient Tb 3+ →Ce 3+ transfer it is necessary that the lowest d (5d 1 ) state of Ce 3+ is located at slightly lower energy than the excited 5 D 4 level of Tb 3+ . It is known that the energy of the 5d 1 state of Ce 3+ decreases with reduction of center symmetry, shortening of the Ce-anion distance and reduction in coordination number (also leading to shorter Ce-anion distances). 9 These conditions are partially fulfilled in the ...