@article{ZiemonsAuffrayBarbieretal.2005,
  author    = {Ziemons, Karl and Auffray, E. and Barbier, R. and Brandenburg, G. and Bruyndonckx, P.},
  title     = {The ClearPET™ project: Development of a 2nd generation high-performance small animal PET scanner},
  series = {Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment},
  volume    = {537},
  journal   = {Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment},
  number    = {1-2},
  issn      = {0168-9002},
  pages     = {307 -- 311},
  year      = {2005},
  abstract  = {Second generation high-performance PET scanners, called ClearPET™1, have been developed by working groups of the Crystal Clear Collaboration (CCC). High sensitivity and high spatial resolution for the ClearPET camera is achieved by using a phoswich arrangement combining two different types of lutetium-based scintillator materials: LSO from CTI and LuYAP:Ce from the CCC (ISTC project). In a first ClearPET prototype, phoswich arrangements of 8×8 crystals of 2×2×10 mm3 are coupled to multi-channel photomultiplier tubes (Hamamatsu R7600). A unit of four PMTs arranged in-line represents one of 20 sectors of the ring design. The opening diameter of the ring is 120 mm, the axial detector length is 110 mm.The PMT pulses are digitized by free-running ADCs and digital data processing determines the gamma energy, the phoswich layer and even the exact pulse starting time, which is subsequently used for coincidence detection. The gantry allows rotation of the detector modules around the field of view. Preliminary data shows a correct identification of the crystal layer about (98±1)\%. Typically the energy resolution is (23.3±0.5)\% for the luyap layer and (15.4±0.4)\% for the lso layer. early studies showed the timing resolution of 2 ns FWHM and 4.8 ns FWTM. the intrinsic spatial resolution ranges from 1.37 mm to 1.61 mm full-width of half-maximum (FWHM) with a mean of 1.48 mm FWHM. further improvements in image and energy resolution are expected when the system geometry is fully modeled.},
  language  = {en}
}
@inproceedings{KloockMorenoHuachupomaetal.2005,
  author    = {Kloock, Joachim P. and Moreno, Lia and Huachupoma, S. and Xu, J. and Wagner, Torsten and Bratov, A. and Doll, T. and Vlasov, Y. and Sch{\"o}ning, Michael Josef},
  title     = {Halbleiterbasierte Schwermetallsensorik auf der Basis von Chalkogenidgl{\"a}sern f{\"u}r zuk{\"u}nftige „Lab on Chip"-Anwendungen},
  series = {7. Dresdner Sensor-Symposium - Neue Herausforderungen und Anwendungen in der Sensortechnik},
  booktitle = {7. Dresdner Sensor-Symposium - Neue Herausforderungen und Anwendungen in der Sensortechnik},
  editor    = {Gerlach, Gerald},
  publisher = {TUDpress, Verl. der Wissenschaften},
  address   = {Dresden},
  isbn      = {3-938863-29-3},
  pages     = {221 -- 224},
  year      = {2005},
  language  = {de}
}
@article{GrajewskiHronTurek2005,
  author    = {Grajewski, Matthias and Hron, Jaroslav and Turek, Stefan},
  title     = {Dual weighted a posteriori error estimation for a new nonconforming linear finite element on quadrilaterals},
  series = {Applied Numerical Mathematics},
  volume    = {54},
  journal   = {Applied Numerical Mathematics},
  number    = {3-4},
  publisher = {Elsevier},
  address   = {Amsterdam},
  issn      = {0168-9274},
  doi       = {10.1016/j.apnum.2004.09.016},
  pages     = {504 -- 518},
  year      = {2005},
  abstract  = {After a short introduction of a new nonconforming linear finite element on quadrilaterals recently developed by Park, we derive a dual weighted residual-based a posteriori error estimator (in the sense of Becker and Rannacher) for this finite element. By computing a corresponding dual solution we estimate the error with respect to a given target error functional. The reliability and efficiency of this estimator is analyzed in several numerical experiments.},
  language  = {en}
}