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At-edge minima in elastic photon scattering amplitudes for dilute aqueous ions
Institution:1. Department of Physics, University of Surrey, Guildford GU2 7XH, UK;2. School of Physics and Astronomy, University of Birmingham, B15 2TT, UK;3. Department of Nuclear Medicine, Radiotherapy and Oncology, School of Medical Sciences, Universiti Sains Malaysia, 16150 Kubang Kerian, Malaysia;4. Queen Elizabeth Medical Centre, University Hospital Birmingham, B15 2TH, UK;1. School of Physics, University of Melbourne, Victoria 3010, Australia;1. Department of Applied Sciences, College of Technological Studies, Public Authority for Applied Education and Training, Shuwaikh, P. O. Box: 42325, Code 70654, Kuwait;2. Department of Physics, Federal University of Agriculture Abeokuta, P. M. B. 2240, Abeokuta, Nigeria;1. Department of Mathematics and Physics, Roma Tre University, Via della Vasca Navale, 84, I-00146 Rome, Italy;2. Department of Nuclear Physics and Biophysics, Comenius University, Mlynska dolina F1, SK-84248 Bratislava, Slovakia;1. Department of Physics, University of Surrey, GuildfordGU2 7XH, UK;2. Department of Physics, College of Education and Science – Al Khurma, Taif University, Saudi Arabia;3. Department of Mathematics, Statistics and Physics Qatar University, Qatar;4. Crises Decision Support Program, Environment and Life Sciences Research Center, Kuwait Institute for Scientific Research, P.O. Box 24885, 13109 Safat, Kuwait;5. Department of Chemistry, University of Surrey, Guildford GU2 7XH, UK;6. Department of Physics, The University of Jordan, Amman, Jordan;7. Medical Physics Department, Cancer Centre, Prince Mohammed Medical City, P.O. Box: 2254, Sakaka Aljouf 42421, Saudi Arabia;8. Department of Physics, Taif University, Saudi Arabia;9. Sunway University, Institute for Healthcare Development, Jalan Universiti, 46150 PJ, Malaysia;1. Department of Physics, University of Surrey, Guildford GU2 7XH, UK;2. Department of Physics, College of Education and Science – Al Khurma, Taif University, Saudi Arabia;3. Department of Chemistry, University of Surrey, Guildford GU2 7XH, UK;4. Crises Decision Support Program, Environment and Life Sciences Research Center, Kuwait Institute for Scientific Research, P.O. Box 24885, 13109 Safat, Kuwait;5. Department of Physics, Taif University, Saudi Arabia;6. Department of Physics, The University of Jordan, Amman, Jordan;7. Department of Radiological Sciences, College of Applied Medical Sciences, King Saud University, P. O.Box 10219, Riyadh 11433, Saudi Arabia;8. Department of Mathematics, Statistics and Physics Qatar University, Qatar;9. Department of Physics, Princess Nourah Bint Abdulrahman University, Riyadh, Saudi Arabia;10. Sunway University, Institute for Healthcare Development, Jalan Universiti, 46150 PJ, Malaysia;1. Crises Decision Support Program, Environment and Life Sciences Research Center, Kuwait Institute for Scientific Research, P.O. Box 24885, 13109, Safat, Kuwait;2. Department of Civil and Environmental Engineering, Faculty of Engineering and Physical Sciences (FEPS), University of Surrey, Guildford, GU2 7XH, United Kingdom;3. Environmental Flow (EnFlo) Research Centre, FEPS, University of Surrey, Guildford, GU2 7XH, United Kingdom;4. Environment and Life Sciences Research Center, Kuwait Institute for Scientific Research, P.O. Box 24885, 13109, Safat, Kuwait
Abstract:Elastic photon scattering and absorption in the vicinity of core atomic orbital energies give rise to resonances in the elastic photon scattering cross-section. Of interest is whether a dilute-ion aqueous system provides an environment suitable for testing independent particle approximation (IPA) predictions. Predictions of the energy of these resonances have been determined for a Dirac–Slater exchange potential with a Latter tail. At BM28 (ESRF), tuneable X-rays were obtained at eV resolution using a 1 1 1 Si monochromator. From target systems including Cu2+ and Zn2+, the X-rays were scattered through high angle from an aqueous medium contained in a thin Perspex cell provided with 8 μm kaplan windows. An energy resolution of ∼500 eV from the HPGe detector was adequate to separate the elastic scattering signal from Kα radiation but not from Compton or Kβ contributions. The Compton contribution from the medium was removed assuming validity of the relativistic impulse approximation. The contribution due to Kβ fluorescence and the resonant X-ray Raman scattering process were handled by assuming the branching ratio for Kα and Kβ contributions to be constant and to be accurately described by fluorescent yields measured above edge. At ionic concentrations ranging from 0.01 to 0.1 mol/l, resonance structures accord with predictions of elastic scattering cross-sections calculated within IPA. Amplitudes calculated using modified form-factors and anomalous scatter factors computed from a Dirac–Slater exchange potential were convolved with a Lorentzian of several eV (FWHM).
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