Neutron Scattering: Treatise on Materials Science and Technology, Vol. 15, Volume 15G. Kostorz Treatise on Materials Science and Technology, Volume 15: Neutron Scattering shows how neutron scattering methods can be used to obtain important information on materials. The book discusses the general principles of neutron scattering; the techniques used in neutron crystallography; and the applications of nuclear and magnetic scattering. The text also describes the measurement of phonons, their role in phase transformations, and their behavior in the presence of crystal defects; and quasi-elastic scattering, with its special merits in the study of microscopic dynamical phenomena in solids and liquids. Special materials problems in neutron devices are also considered. Materials scientists, solid state physicists, physical chemists, and metallurgists will find the book invaluable. |
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Results 1-5 of 49
Page xx
... Electron Microscopy C. S. Pande Metallurgy of A15 Conductors Thomas Luhman Superconductors for Power Transmission J. F. Bussiere Metallurgy of Niobium Surfaces M. Strongin, C. Varmazis, and A. Joshi Irradiation Effects in ...
... Electron Microscopy C. S. Pande Metallurgy of A15 Conductors Thomas Luhman Superconductors for Power Transmission J. F. Bussiere Metallurgy of Niobium Surfaces M. Strongin, C. Varmazis, and A. Joshi Irradiation Effects in ...
Page xxii
... electron wave-vector at Fermi surface L lattice vector static displacement, 36 Fourier transform of displacement, 37 M molecular weight of polymer and solvent, 387 magnetic structure factor, 110 magnetization density, 245 total magnetic ...
... electron wave-vector at Fermi surface L lattice vector static displacement, 36 Fourier transform of displacement, 37 M molecular weight of polymer and solvent, 387 magnetic structure factor, 110 magnetization density, 245 total magnetic ...
Page 3
... electrons volts: X = 0.286 E *. * To obtain velocity v, in meters per second from wavelength in angströms: tn = 3956//. B. Why Neutron Scattering? As can be seen from Table I, the range of wavelengths and energies covered by thermal ...
... electrons volts: X = 0.286 E *. * To obtain velocity v, in meters per second from wavelength in angströms: tn = 3956//. B. Why Neutron Scattering? As can be seen from Table I, the range of wavelengths and energies covered by thermal ...
Page 4
... electrons in an atom (in contrast to electromagnetic radiation) but rather varies in a nonmonotonic way from one element to another. Being a nuclear property, the scattering amplitudes may differ considerably for different isotopes of a ...
... electrons in an atom (in contrast to electromagnetic radiation) but rather varies in a nonmonotonic way from one element to another. Being a nuclear property, the scattering amplitudes may differ considerably for different isotopes of a ...
Page 13
... electron volts), they must be slowed down before they can be used for scattering experiments. This is achieved by a moderator, a medium which allows the neutrons to be thermalized. If thermalization is complete at temperature T, the ...
... electron volts), they must be slowed down before they can be used for scattering experiments. This is achieved by a moderator, a medium which allows the neutrons to be thermalized. If thermalization is complete at temperature T, the ...
Contents
1 | |
69 | |
Chapter 3 Phonons and Structural Phase Transitions | 131 |
Chapter 4 Phonons and Defects | 191 |
Chapter 5 SmallAngle Scattering and Its Applications to Materials Science | 227 |
Chapter 6 Diffusion Elastic Neutron Scattering from Nonmagnetic Materials | 291 |
Chapter 7 Magnetic Inhomogeneities | 337 |
Chapter 8 Polymer Conformation and Dynamics | 381 |
Chapter 9 Hydrogen in Metals | 423 |
Chapter 10 Materials Problems in Neutron Devices | 461 |
Index | 513 |
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Common terms and phrases
alloys amplitude antiferromagnetic atoms average Bragg peaks Bragg scattering calculated chain chapter by Kostorz Chem coherent collimation concentration cross section Crystallogr defect density dependence detector diffuse scattering direction dispersion curves displacements distribution domain elastic electron energy experimental ferroelectric ferromagnetic flux line Fourier transform frequency hydrides hydrogen impurity incoherent scattering inelastic scattering Institut Laue-Langevin intensity interaction isotope Kostorz and Lovesey Lett magnetic scattering materials matrix measurements metal mode molecules monochromator neutron beam neutron diffraction neutron SAS neutron scattering nuclear obtained orientation parameters particles peak phase phonon Phys plane polarized neutron polymer Proc quasi-elastic reactor reciprocal lattice reflection resolution sample scattering amplitude scattering cross section scattering length scattering vector Schelten Schmatz shown in Fig single crystal solid spin structure factor studies superconducting symmetry technique temperature theory thermal neutrons tion transition unit cell values wave vector wavelength width x-ray