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BiBTeX citation export for MOPOTK003: Absorbed Dose Characteristics for Irradiation Experiments at AREAL 5 MeV Electron Linac

@inproceedings{khachatryan:ipac2022-mopotk003,
  author       = {V.G. Khachatryan and Z. Amirkhanyan and H. Davtyan and A. Grigoryan and B. Grigoryan and M. Ivanyan and V.H. Petrosyan and A. Vardanyan and A.S. Yeremyan},
% author       = {V.G. Khachatryan and Z. Amirkhanyan and H. Davtyan and A. Grigoryan and B. Grigoryan and M. Ivanyan and others},
% author       = {V.G. Khachatryan and others},
  title        = {{Absorbed Dose Characteristics for Irradiation Experiments at AREAL 5 MeV Electron Linac}},
  booktitle    = {Proc. IPAC'22},
% booktitle    = {Proc. 13th International Particle Accelerator Conference (IPAC'22)},
  pages        = {429--432},
  eid          = {MOPOTK003},
  language     = {english},
  keywords     = {electron, experiment, radiation, simulation, gun},
  venue        = {Bangkok, Thailand},
  series       = {International Particle Accelerator Conference},
  number       = {13},
  publisher    = {JACoW Publishing, Geneva, Switzerland},
  month        = {07},
  year         = {2022},
  issn         = {2673-5490},
  isbn         = {978-3-95450-227-1},
  doi          = {10.18429/JACoW-IPAC2022-MOPOTK003},
  url          = {https://jacow.org/ipac2022/papers/mopotk003.pdf},
  abstract     = {{Existing electron photogun facility at the CANDLE SRI currently can provide electron beam with the energy up to 5 MeV. The beam is being used as an irradiation source in the number of material science and life science experiments. Performed beam particle tracking simulations along with intensive application of the beam diagnostic instruments (bending magnet, YAG stations, Faraday cups) allow control of the experimental samples’ irradiation parameters, particularly exposure times for given dose as well as absorbed dose spatial distribution. Direct application of the electron beam for the irradiation experiments allows achievement of high absorbed dose. For the calculation of the irradiation parameters of the experimental samples’ particle transport simulation results should be combined with the beam current measurements by Faraday Cup (FC). Dose measurements and the comparison with numerical simulations using various initial parameters (Transverse size, divergence and energy spread) permit to pin down their actual values.}},
}