• DocumentCode
    758396
  • Title

    Effects of \\hbox {Ca}^{2+} Co-Doping on the Scintillation Properties of LSO:Ce

  • Author

    Spurrier, Merry A. ; Szupryczynski, Piotr ; Yang, Kan ; Carey, A. Andrew ; Melcher, Charles L.

  • Author_Institution
    Scintillation Mater. Res. Center, Tennessee Univ., Knoxville, TN
  • Volume
    55
  • Issue
    3
  • fYear
    2008
  • fDate
    6/1/2008 12:00:00 AM
  • Firstpage
    1178
  • Lastpage
    1182
  • Abstract
    In addition to desirable physical properties including a density of 7.4 g/cm3 , an effective atomic number of 66, and no hygroscopicity, Lu2SiO5:Ce has well-known scintillation properties of ~30 900 photons/MeV, an emission peak near 420 nm, and a decay time of ~43 ns. These scintillation properties are achieved with Ce doping concentrations roughly in the range of 0.05 to 0.5 atomic percent relative to Lu. These properties make Lu2SiO5:Ce a widely used scintillator in positron emission tomography, in particular. We have found that both the light output and decay time may be improved by a combination of optimized crystal growth atmosphere and co-doping with divalent cations such as Ca. Scintillation light output of ~38 800 photons/MeV has been achieved as well as scintillation decay time as short as 31 ns with no long components. The relationship between growth conditions, dopant concentration, decay time, and light output is well defined, thus allowing one to reliably "tune" the crystal to the desired combination of light output and decay time. Possible explanations of the underlying mechanism are being explored and include compensation of oxygen vacancies, alteration of the relative occupancies of the cerium lattice sites, and suppression of trapping centers. In addition to higher count-rate capability and better coincidence timing, the improved decay time is expected to be particularly advantageous for time-of-flight positron emission tomography. Also, phoswich detectors comprising "standard" LSO (~43 ns decay time) and "fast" LSO (~31 ns decay time) become an attractive alternative to typical phoswich designs that often suffer from problems of mismatched light outputs and indices of refraction or the absorption of one scintillator\´s light by the other.
  • Keywords
    calcium; cerium; crystal growth; doping profiles; lutetium compounds; positron emission tomography; refractive index; scintillation; solid scintillation detectors; vacancies (crystal); LSO:Ce; Lu2SiO5:Ce,Ca; crystal growth; doping concentrations; oxygen vacancies; phoswich designs; phoswich detectors; physical properties; refraction index; scintillation light output; scintillation properties; time-of-flight positron emission tomography; trapping centers; Absorption; Atmosphere; Biomedical imaging; Doping; Lattices; Molecular imaging; Photonic crystals; Positron emission tomography; Temperature measurement; Zirconium; $hbox {Lu}_{2}hbox {SiO}_{5}$; crystal growth; decay time; light output; scintillators;
  • fLanguage
    English
  • Journal_Title
    Nuclear Science, IEEE Transactions on
  • Publisher
    ieee
  • ISSN
    0018-9499
  • Type

    jour

  • DOI
    10.1109/TNS.2007.913486
  • Filename
    4545214