Epitaxial Growth of LuAG:Ce and LuAG:Ce,Pr Films and Their Scintillation Properties

We performed the growth by Liquid Phase Epitaxy (LPE) of Ce and Ce-Pr doped Lu<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> (LuAG) Single Crystalline Films (SCFs) onto LuAG and Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> (YAG) substrates. The structural properties of LuAG:Ce and LuAG:Ce,Pr SCFs were examined by X-ray diffraction. The optical properties of the SCFs were studied through cathodoluminescence (CL) spectra, scintillation Light Yield (LY), decay kinetic under <inline-formula> <tex-math notation="LaTeX">$\alpha $ </tex-math></inline-formula>–particle (Pu<sup>239</sup>) excitation, X-ray excited luminescence, thermostimulated luminescence (TSL) and afterglow measurements. The SCFs grown on LuAG substrates displayed good surface quality and structural perfection, whereas the SCFs grown on YAG substrates showed a rough surface and poorer crystalline quality, due to a large lattice mismatch between the film and the substrate (0.82%). Under <inline-formula> <tex-math notation="LaTeX">$\alpha $ </tex-math></inline-formula>-particle excitation, the LY of LuAG:Ce SCF exceeded by 2 times that of the best YAG:Ce SCF sample used as reference. Under X-ray excitation, the LuAG:Ce SCF with optimized Ce concentration showed LY close (77%) to a reference YAG:Ce Single Crystal (SC) scintillator. The afterglow of LuAG:Ce and LuAG:Ce,Pr SCFs was lower (by 1 decade) than that of the tested reference LuAG:Ce SC. However there is not a complete suppression of the afterglow at room temperature (RT), despite the fact that the SCFs present much lower concentration of antisite and vacancy type defects than their SC counterparts. This can be explained by the presence in the films of other trap centers responsible for TSL above RT.

[1]  A. Vedda,et al.  The antisite LuAl defect‐related trap in Lu3Al5O12:Ce single crystal , 2005 .

[2]  W. Marsden I and J , 2012 .

[3]  Y. Zorenko,et al.  High‐perfomance Ce‐doped multicomponent garnet single crystalline film scintillators , 2015 .

[4]  N. G. Einspruch,et al.  ELECTRONIC EFFECT IN THE ELASTIC CONSTANT C′ OF SILICON , 1963 .

[5]  M. Nikl,et al.  Scintillation and optical properties of YAG:Ce films grown by liquid phase epitaxy , 2007 .

[6]  M. Kuklja Defects in yttrium aluminium perovskite and garnet crystals: atomistic study , 2000 .

[7]  J. Tous,et al.  The α-particle excited scintillation response of the liquid phase epitaxy grown LuAG:Ce thin films , 2008 .

[8]  Thierry Martin,et al.  A novel epitaxially grown LSO-based thin-film scintillator for micro-imaging using hard synchrotron radiation. , 2010, Journal of synchrotron radiation.

[9]  R. Stephenson A and V , 1962, The British journal of ophthalmology.

[10]  M. Nikl,et al.  Growth and properties of epitaxial Ce-doped YAG and LuAG films for scintillators , 2010 .

[11]  V. Mikhailin,et al.  Luminescence of excitons and antisite defects in the phosphors based on garnet compounds , 2004 .

[12]  A. Vedda,et al.  Lu3Al5O12-based materials for high 2D-resolution scintillation detectors , 2009 .

[13]  A. Rack,et al.  LSO-Based Single Crystal Film Scintillator for Synchrotron-Based Hard X-Ray Micro-Imaging , 2009, IEEE Transactions on Nuclear Science.

[14]  P. Bilski,et al.  Peculiarities of luminescent and scintillation properties of YAG:Ce phosphor prepared in different crystalline forms , 2012 .

[15]  P. Bilski,et al.  Growth and luminescent properties of scintillators based on the single crystalline films of (Lu,Gd)3(Al,Ga)5O12:Ce garnets , 2016 .

[16]  M. Nikl,et al.  Ce-doped YAG and LuAG Epitaxial Films for Scintillation Detectors , 2008, IEEE Transactions on Nuclear Science.

[17]  E. Giess,et al.  Liquid phase epitaxial growth of magnetic garnet films by isothermal dipping in a horizontal plane with axial rotation , 1972 .

[18]  T. Martin,et al.  Recent developments in X-ray imaging with micrometer spatial resolution. , 2006, Journal of synchrotron radiation.

[19]  A. Vedda,et al.  Single crystalline film scintillators based on Ce- and Pr-doped aluminium garnets , 2007 .

[20]  Mark Voorneveld,et al.  Preparation , 2018, Games Econ. Behav..

[21]  J. Tous,et al.  Scintillation efficiency and X-ray imaging with the RE-Doped LuAG thin films grown by liquid phase epitaxy , 2012 .

[23]  M. Shone The technology of YIG film growth , 1985 .

[24]  M. Nikl,et al.  Scintillation properties of LuAG:Ce single crystalline films grown by LPE method , 2010 .

[25]  P. Bilski,et al.  Growth and luminescent properties of scintillators based on the single crystalline films of Lu3−xGdxAl5O12:Ce garnet , 2015 .

[26]  Martin Nikl,et al.  LuAG:Pr, LuAG:La, and LuAP:Ce thin film scintillators for visualisation of x-ray images , 2009 .

[27]  I. Konstankevych,et al.  New scintillation detectors based on oxide single crystal films for biological microtomography , 2003 .

[28]  P. Görnert,et al.  Study of the liquid phase epitaxy process of garnet layers by induced striations , 1977 .

[29]  A. Mandowski,et al.  Luminescence of F+ and F centers in AI2O3-Y2O3 oxide compounds , 2010 .

[30]  A. Meijerink,et al.  Luminescence and energy transfer in Lu3Al5O12 scintillators co-doped with Ce3+ and Pr3+ , 2013 .

[31]  A. Vedda,et al.  Luminescence of dimer lead centers in aluminium perovskites and garnets , 2009 .

[32]  H. Levinstein,et al.  Growth of High‐Quality Garnet Thin Films from Supercooled Melts , 1971 .

[33]  M. Nikl,et al.  Growth and emission properties of Sc, Pr, and Ce co-doped Lu3Al5O12 epitaxial layers for scintillators , 2011 .

[34]  M. I. Timoshechkin,et al.  Spectroscopic study of stoichiometry deviation in crystals with garnet structure , 1977 .

[35]  Y. Zorenko,et al.  Preparation, Luminescence Properties, and Application of Scintillators Based on Lu3Al5O12:Ce Single‐Crystal Films , 2002 .