Difference between revisions of "Reflectivity"
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==Off-Specular Reflectivity== | ==Off-Specular Reflectivity== | ||
TBD | TBD | ||
+ | |||
+ | ==Mathematical form== | ||
+ | In its simplest form, the Fresnel reflectivity can be given by: | ||
+ | :<math> | ||
+ | R_F = \frac{k_z-\tilde{k}_z}{k_z+\tilde{k}_z} | ||
+ | </math> | ||
+ | Where: | ||
+ | :<math> | ||
+ | \tilde{k}_z = - \sqrt{ n^2 k^2_0 - |k_{\parallel}|^2 } | ||
+ | </math> | ||
+ | And ''n'' is the complex [[refractive index]] of the substrate. The idealized uncorrelated roughness can be characterized by a mean standard deviation of the height <math>\scriptstyle \sigma = \sqrt{ \left \langle h^2 \right \rangle }</math>: | ||
+ | :<math> | ||
+ | R_S = R_F e^{ -2 \sigma^2 k_z \tilde{k}_z } | ||
+ | </math> | ||
+ | For a substrate with a single continuous layer of thickness ''h'' (e.g. a uniform thin film), the reflectivity becomes: | ||
+ | :<math> | ||
+ | R_S = \frac{ r_{01} + r_{12} e^{ 2i \tilde{k}^1_z h } }{ 1 + r_{01} r_{12} e^{ 2i \tilde{k}^1_z h } } | ||
+ | </math> | ||
+ | where <math>\tilde{k}^j_z=-\sqrt(n^2_j k^2_0 - |k_{\parallel}|^2 }</math> is the perpendicular component of the wave-vector (in medium ''j''). The reflectivity coefficients are: | ||
+ | :<math> | ||
+ | f_{ij} = \frac{ \tilde{k}^i_z - \tilde{k}^j_z }{ \tilde{k}^i_z + \tilde{k}^j_z } | ||
+ | </math> | ||
+ | Where <math>\scriptstyle r_{01}</math> and <math>\scriptstyle r_{12}</math> for the [[vacuum]]-layer and layer-substrate interfaces, respectively. This is called the 'one-box model'. | ||
+ | |||
+ | ===Parratt formalism=== | ||
+ | TBD | ||
+ | |||
==See Also== | ==See Also== |
Revision as of 11:44, 28 January 2015
Reflectivity refers to the measurement of the intensity of reflection off of a flat interface. The term both describes the physical phenomenon, as well as the experimental technique.
X-ray Reflectivity (XRR or XR) and neutron reflectivity (NR) are techniques which measure the intensity of reflected radiation as a function of angle (where, by definition for specular reflectivity, the incident and exit angles are equal; ). A plot of reflectivity (R) versus angle yields the reflectivity curve. For XR and NR, the data is typically plotted as a function of the momentum transfer parallel to the film normal:
Off-Specular Reflectivity
TBD
Mathematical form
In its simplest form, the Fresnel reflectivity can be given by:
Where:
And n is the complex refractive index of the substrate. The idealized uncorrelated roughness can be characterized by a mean standard deviation of the height :
For a substrate with a single continuous layer of thickness h (e.g. a uniform thin film), the reflectivity becomes:
where Failed to parse (syntax error): {\displaystyle \tilde{k}^j_z=-\sqrt(n^2_j k^2_0 - |k_{\parallel}|^2 }} is the perpendicular component of the wave-vector (in medium j). The reflectivity coefficients are:
Where and for the vacuum-layer and layer-substrate interfaces, respectively. This is called the 'one-box model'.
Parratt formalism
TBD
See Also
- Fresnel plot
- Oscillations below the critical angle
- DWBA: A formalism for modeling GISAXS data, including reflection effects.