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Results for DC.creator="N." AND DC.creator="G." AND DC.creator="Alexandropoulos" in section 7.4.3 of volume C |
Compton scattering
International Tables for Crystallography (2006). Vol. C, Section 7.4.3, pp. 657-661 [ doi:10.1107/97809553602060000607 ]
... 4.184 4.478 4.690 4.878 5.051 5.208 5.348 5.781 5.930 7 N 1.08 2.858 4.097 4.792 5.182 5.437 5.635 5.809 5.968 6.113 ... state and a vacancy in the L (or M or N) shell and an electron in the continuum in the final ... 125137-1. Boeing Co. Bushuev, V. A. & Kuz'min, R. N. (1977). Inelastic scattering of X-ray and synchrotron ...
Plasmon, Raman, and resonant Raman scattering
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.4, pp. 660-661 [ doi:10.1107/97809553602060000607 ]
... state and a vacancy in the L (or M or N) shell and an electron in the continuum in the final ... Lett. 34, 372-376. Bushuev, V. A. & Kuz'min, R. N. (1977). Inelastic scattering of X-ray and synchrotron radiation ... Phys. Rev. B, 13, 2377-2380. Gavrila, M. & Tugulea, M. N. (1975). Compton scattering by L shell electrons. Rev. ...
Relativistic treatment of incoherent scattering
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.3, pp. 659-660 [ doi:10.1107/97809553602060000607 ]
... pocket calculator. Phys. Rev. A, 26, 3325-3333. Williams, B. G. (1977). Compton scattering. New York: McGraw-Hill. International Tables ...
Exact calculations
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.2.3, p. 659 [ doi:10.1107/97809553602060000607 ]
Exact calculations 7.4.3.2.3. Exact calculations The matrix elements of (7.4.3.4) can be evaluated exactly for the hydrogen atom. If one-electron wavefunctions in many-electron atoms are modelled by hydrogenic orbitals [with a suitable choice of the orbital exponent; see, for example, Slater (1937)], an analytical approach can be used, as ...
Thomas-Fermi model
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.2.2, p. 659 [ doi:10.1107/97809553602060000607 ]
Thomas-Fermi model 7.4.3.2.2. Thomas-Fermi model This statistical model of the atomic charge density (Thomas, 1927; Fermi, 1928) considerably simplifies the calculation of coherent and incoherent scattering factors since both can be written as universal functions of K and Z. Numerical values were first calculated by Bewilogua (1931); more recent ...
Semi-classical radiation theory
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.2.1, pp. 657-659 [ doi:10.1107/97809553602060000607 ]
... 4.184 4.478 4.690 4.878 5.051 5.208 5.348 5.781 5.930 7 N 1.08 2.858 4.097 4.792 5.182 5.437 5.635 5.809 5.968 6.113 ...
Non-relativistic calculations of the incoherent scattering cross section
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.2, pp. 657-659 [ doi:10.1107/97809553602060000607 ]
... 4.184 4.478 4.690 4.878 5.051 5.208 5.348 5.781 5.930 7 N 1.08 2.858 4.097 4.792 5.182 5.437 5.635 5.809 5.968 6.113 ...
Introduction
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.1, p. 657 [ doi:10.1107/97809553602060000607 ]
Introduction 7.4.3.1. Introduction In many diffraction studies, it is necessary to correct the intensities of the Bragg peaks for a variety of inelastic scattering processes. Compton scattering is only one of the incoherent processes although the term is often used loosely to include plasmon, Raman, and resonant Raman scattering, all of ...
Magnetic scattering
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.5, p. 661 [ doi:10.1107/97809553602060000607 ]
Magnetic scattering 7.4.3.5. Magnetic scattering Finally, and for completeness, it should be noted that the intensity of Compton scattering from a magnetic material with a net spin moment will, in principle, differ from that from a non-magnetic material. For unpolarized radiation, the effects are only discernible at photon energies greatly ...
International Tables for Crystallography (2006). Vol. C, Section 7.4.3, pp. 657-661 [ doi:10.1107/97809553602060000607 ]
... 4.184 4.478 4.690 4.878 5.051 5.208 5.348 5.781 5.930 7 N 1.08 2.858 4.097 4.792 5.182 5.437 5.635 5.809 5.968 6.113 ... state and a vacancy in the L (or M or N) shell and an electron in the continuum in the final ... 125137-1. Boeing Co. Bushuev, V. A. & Kuz'min, R. N. (1977). Inelastic scattering of X-ray and synchrotron ...
Plasmon, Raman, and resonant Raman scattering
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.4, pp. 660-661 [ doi:10.1107/97809553602060000607 ]
... state and a vacancy in the L (or M or N) shell and an electron in the continuum in the final ... Lett. 34, 372-376. Bushuev, V. A. & Kuz'min, R. N. (1977). Inelastic scattering of X-ray and synchrotron radiation ... Phys. Rev. B, 13, 2377-2380. Gavrila, M. & Tugulea, M. N. (1975). Compton scattering by L shell electrons. Rev. ...
Relativistic treatment of incoherent scattering
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.3, pp. 659-660 [ doi:10.1107/97809553602060000607 ]
... pocket calculator. Phys. Rev. A, 26, 3325-3333. Williams, B. G. (1977). Compton scattering. New York: McGraw-Hill. International Tables ...
Exact calculations
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.2.3, p. 659 [ doi:10.1107/97809553602060000607 ]
Exact calculations 7.4.3.2.3. Exact calculations The matrix elements of (7.4.3.4) can be evaluated exactly for the hydrogen atom. If one-electron wavefunctions in many-electron atoms are modelled by hydrogenic orbitals [with a suitable choice of the orbital exponent; see, for example, Slater (1937)], an analytical approach can be used, as ...
Thomas-Fermi model
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.2.2, p. 659 [ doi:10.1107/97809553602060000607 ]
Thomas-Fermi model 7.4.3.2.2. Thomas-Fermi model This statistical model of the atomic charge density (Thomas, 1927; Fermi, 1928) considerably simplifies the calculation of coherent and incoherent scattering factors since both can be written as universal functions of K and Z. Numerical values were first calculated by Bewilogua (1931); more recent ...
Semi-classical radiation theory
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.2.1, pp. 657-659 [ doi:10.1107/97809553602060000607 ]
... 4.184 4.478 4.690 4.878 5.051 5.208 5.348 5.781 5.930 7 N 1.08 2.858 4.097 4.792 5.182 5.437 5.635 5.809 5.968 6.113 ...
Non-relativistic calculations of the incoherent scattering cross section
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.2, pp. 657-659 [ doi:10.1107/97809553602060000607 ]
... 4.184 4.478 4.690 4.878 5.051 5.208 5.348 5.781 5.930 7 N 1.08 2.858 4.097 4.792 5.182 5.437 5.635 5.809 5.968 6.113 ...
Introduction
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.1, p. 657 [ doi:10.1107/97809553602060000607 ]
Introduction 7.4.3.1. Introduction In many diffraction studies, it is necessary to correct the intensities of the Bragg peaks for a variety of inelastic scattering processes. Compton scattering is only one of the incoherent processes although the term is often used loosely to include plasmon, Raman, and resonant Raman scattering, all of ...
Magnetic scattering
International Tables for Crystallography (2006). Vol. C, Section 7.4.3.5, p. 661 [ doi:10.1107/97809553602060000607 ]
Magnetic scattering 7.4.3.5. Magnetic scattering Finally, and for completeness, it should be noted that the intensity of Compton scattering from a magnetic material with a net spin moment will, in principle, differ from that from a non-magnetic material. For unpolarized radiation, the effects are only discernible at photon energies greatly ...
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