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The '''Debye-Waller factor''' (DWF), named after [[Peter Debye]] and [[Ivar Waller]], is used in [[condensed matter physics]] to describe the attenuation of [[x-ray scattering]] or [[neutron scattering]] caused by thermal motion or quenched disorder. It has als been called the '''B factor''' or the '''temperature factor'''.
The '''Debye-Waller factor''' (DWF), named after [[Peter Debye]] and [[Ivar Waller]], is used in [[condensed matter physics]] to describe the attenuation of [[x-ray scattering]] or [[neutron scattering]] caused by thermal motion or quenched disorder. It has als been called the '''B factor''' or the '''temperature factor'''.


The DWF depends on ''q'', the absolute value of the [[scattering vector]] <math>\vec q</math>. For a given ''q'',
The DWF depends on ''q'', the absolute value of the [[scattering vector]] '''q'''. For a given ''q'',
DWF(''q'') gives the fraction of elastic scattering; 1-DWF(''q'') correspondingly the fraction of inelastic scattering. In [[diffraction]] studies, only the elastic scattering is useful; in crystals, it gives rise to distinct [[Bragg peak]]s. Inelastic scattering events are undesirable as they cause a diffuse background - unless the energies of scattered particles are analysed in which case they carry valuable information ([[inelastic neutron scattering]]).
DWF(''q'') gives the fraction of elastic scattering; 1-DWF(''q'') correspondingly the fraction of inelastic scattering. In [[diffraction]] studies, only the elastic scattering is useful; in crystals, it gives rise to distinct [[Bragg peak]]s. Inelastic scattering events are undesirable as they cause a diffuse background - unless the energies of scattered particles are analysed in which case they carry valuable information ([[inelastic neutron scattering]]).


Assuming [[harmonic oscillator|harmonicity]] of thermal motion in the material under study, the DWF takes the form
Assuming [[harmonic oscillator|harmonicity]] of thermal motion in the material under study, the DWF takes the form


:DWF<math>=\exp\left( -\langle [\vec q\vec u(0)]^2 \rangle \right) =
:DWF<math>=\exp\left( -\langle [\mathbf{q}\mathbf{u}(0)]^2 \rangle \right) =
\exp\left( -q^2 \langle \vec u(0)^2 \rangle / 3 \right)</math>
\exp\left( -q^2 \langle [\mathbf{u}(0)]^2 \rangle / 3 \right)</math>


where <math>\langle\ldots\rangle</math> denotes thermal averaging, and <math>\vec u(t)</math> is the displacement of a scattering center as function of time ''t''.
where <...> denotes thermal averaging, and '''q'''(''t'') is the displacement of a scattering center as function of time ''t''.


[[Category:Crystallography]]
[[Category:Crystallography]]

Revision as of 11:28, 29 January 2007

The Debye-Waller factor (DWF), named after Peter Debye and Ivar Waller, is used in condensed matter physics to describe the attenuation of x-ray scattering or neutron scattering caused by thermal motion or quenched disorder. It has als been called the B factor or the temperature factor.

The DWF depends on q, the absolute value of the scattering vector q. For a given q, DWF(q) gives the fraction of elastic scattering; 1-DWF(q) correspondingly the fraction of inelastic scattering. In diffraction studies, only the elastic scattering is useful; in crystals, it gives rise to distinct Bragg peaks. Inelastic scattering events are undesirable as they cause a diffuse background - unless the energies of scattered particles are analysed in which case they carry valuable information (inelastic neutron scattering).

Assuming harmonicity of thermal motion in the material under study, the DWF takes the form

DWF

where <...> denotes thermal averaging, and q(t) is the displacement of a scattering center as function of time t.