. . . "Onderi\u0161inov\u00E1, Z." . "luminescence; liquid phase epitaxy; garnets; Sc,Pr:LuAG; scintillator materials"@en . "Growth and emission properties of Sc, Pr, and Ce co-doped Lu3Al5O12 epitaxial layers for scintillators" . "NL - Nizozemsko" . "Ku\u010Dera, M." . "7"^^ . . . . "RIV/68378271:_____/11:00363964" . "Growth and emission properties of Sc, Pr, and Ce co-doped Lu3Al5O12 epitaxial layers for scintillators" . . . "1" . . "RIV/68378271:_____/11:00363964!RIV12-AV0-68378271" . . . "P(GA202/08/0893), P(KAN300100802), S, Z(AV0Z10100521), Z(MSM0021620834)" . "318" . "[D6C06E14FA5C]" . "Nikl, Martin" . . . . . "The effect of Sc, Pr, and Ce co-doping on the emission and scintillation properties of lutetium-aluminum epitaxial garnet layers, Lu3Al5O12, was studied. These garnet layers provide better emission and scintillation response compared to those without Sc co-doping and energy transfer from sensitizer Sc3+ to activator Pr3+ ions that was observed for small Sc doping levels consequently resulted in increased radioluminescence intensity and photoelectron yield."@en . . . . "Pr\u016F\u0161a, Petr" . . "The effect of Sc, Pr, and Ce co-doping on the emission and scintillation properties of lutetium-aluminum epitaxial garnet layers, Lu3Al5O12, was studied. These garnet layers provide better emission and scintillation response compared to those without Sc co-doping and energy transfer from sensitizer Sc3+ to activator Pr3+ ions that was observed for small Sc doping levels consequently resulted in increased radioluminescence intensity and photoelectron yield." . "5"^^ . "000289653900177" . "Journal of Crystal Growth" . "Mare\u0161, Ji\u0159\u00ED A." . "8"^^ . "Hanu\u0161, M." . . "Ku\u010Derkov\u00E1, Romana" . "201572" . . . . "10.1016/j.jcrysgro.2010.11.140" . "Nitsch, Karel" . . "Growth and emission properties of Sc, Pr, and Ce co-doped Lu3Al5O12 epitaxial layers for scintillators"@en . . . . "Growth and emission properties of Sc, Pr, and Ce co-doped Lu3Al5O12 epitaxial layers for scintillators"@en . . "0022-0248" .