Difference between revisions of "Absorption length"

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(Related forms)
(Related forms)
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| <math>\mu = \frac{\rho N_a}{m_a} \sigma</math>
 
| <math>\mu = \frac{\rho N_a}{m_a} \sigma</math>
 
|  
 
|  
|  
+
| <math>\mu = \frac{2 M_a \lambda}{m_a } \mathrm{Im}(\mathrm{SLD})</math>
 
|-
 
|-
 
| <math>\frac{\mu}{\rho} = \frac{1}{\rho\epsilon}</math>
 
| <math>\frac{\mu}{\rho} = \frac{1}{\rho\epsilon}</math>
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| <math>\frac{\mu}{\rho} = \frac{N_a}{m_a} \sigma</math>
 
| <math>\frac{\mu}{\rho} = \frac{N_a}{m_a} \sigma</math>
 
| <math>\frac{\mu}{\rho} = </math>
 
| <math>\frac{\mu}{\rho} = </math>
| <math>\frac{\mu}{\rho} = </math>
+
| <math>\frac{\mu}{\rho} = \frac{2 M_a \lambda}{\rho m_a } \mathrm{Im}(\mathrm{SLD})</math>
 
|-
 
|-
 
| <math>f_2 = \frac{m_a }{\rho N_a 2 r_e \lambda  \epsilon} </math>
 
| <math>f_2 = \frac{m_a }{\rho N_a 2 r_e \lambda  \epsilon} </math>
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|-
 
|-
 
|  
 
|  
|  
+
| <math>\mathrm{Im}(\mathrm{SLD}) = \frac{m_a }{2 M_a \lambda} \mu</math>
|  
+
| <math>\mathrm{Im}(\mathrm{SLD}) = \frac{\rho m_a }{2 M_a \lambda} \frac{\mu}{\rho}</math>
 
| <math>\mathrm{Im}(\mathrm{SLD}) = \frac{\rho N_a r_e }{M_a} f_2</math>
 
| <math>\mathrm{Im}(\mathrm{SLD}) = \frac{\rho N_a r_e }{M_a} f_2</math>
 
| <math>\mathrm{Im}(\mathrm{SLD}) = \frac{\rho N_a}{2 \lambda M_a}\sigma</math>
 
| <math>\mathrm{Im}(\mathrm{SLD}) = \frac{\rho N_a}{2 \lambda M_a}\sigma</math>

Revision as of 18:17, 6 June 2014

The absorption length or attenuation length in x-ray scattering is the distance over which the x-ray beam is absorbed. By convention, the absorption length ϵ is defined as the distance into a material where the beam flux has dropped to 1/e of its incident flux.

Absorption

The absorption follows a simple Beer-Lambert law:

The attenuation coefficient (or absorption coefficient) is simply the inverse of the absorption length;

Calculating

The absorption length arises from the imaginary part of the atomic scattering factor, f2. It is closely related to the absorption cross-section, and the mass absorption coefficient. Specifically, the atomic photoabsorption cross-section can be computed via:

Where λ is the x-ray wavelength, and re is the classical electron radius. The attenuation coefficient is given by:

where ρ is density, Na is the Avogadro constant, and ma is the atomic molar mass. Note that the mass attenuation coefficient is simply .

Related forms

As can be seen, there are many related quantities which express the material's absorption:

  • Absorption length , the distance over which the intensity falls to 1/e.
  • Attenuation coefficient , the characteristic inverse-distance for attenuation.
  • Mass attenuation coefficient , the density-scaled attenuation.
  • Absorptive atomic scattering factor , the intrinsic dissipative interaction of the material.
  • Atomic photoabsorption cross-section , the cross-section ('effective size') of the atom's x-ray absorption (capture) efficiency.
  • Imaginary refractive index , the resonant component of the refractive index.
  • Imaginary Scattering Length Density , the absorptive component of the scattering contrast.

See Also