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| Scattering is due to the polarization of species. The polarization can be summed from the behavior of individual resonances and damping factors (related to resonance bandwidth), which I have not yet been able to find. For mostly-isolated atoms in high vacuum, [[ | Beers line broadening ]] will not be relevant; the bandwidth $ \gamma $ is related to damping time, TBD | Scattering is due to the polarization of species. The polarization can be summed from the behavior of individual resonances and damping factors (related to resonance bandwidth), which I have not yet been able to find. For mostly-isolated atoms in high vacuum, [[ | Beers line broadening ]] will not be relevant; the bandwidth $ ~ \large \gamma ~ $ is related to damping time, TBD |
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| The scattering from a single resonator at frequency $ \omega $ is (from Feynman Lectures on Physics Chapter X page X) proportional to | The scattering from a single resonator at frequency $ ~ \large \omega ~ $ is (from Feynman Lectures on Physics Chapter X page X) proportional to |
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| $ \integral { \omega^4 \over { ( \omega^2 - {\omega_0}^2 )^2 - \gamma^2 omega^2 } ~ = ~ $ | $ { \Large \int{ \omega^4 \over { ( \omega^2 ~-~ \omega_0^2 )^2 ~-~ \gamma^2 \omega^2 } } } ~= \omega ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ $ $ {\Large - } ~~ { { \large \left( 2 \omega_0^4 ~-~ 2 \omega_0^2 \gamma \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~-~ 2 \gamma \right) ~+~ \gamma^3 \left( \gamma - \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } \right) \right) \tan^{-1} \left( { \Large { { \huge \omega } \over { \sqrt{ { \Large { \gamma \over 2 } } \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~-~ \gamma \right) ~-~ \omega_0^2 } } } } \right) } \over { \large \sqrt{ 2 } ~ \gamma \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } \sqrt{ \gamma \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~-~ \gamma \right) ~-~ 2 \omega_0^2 } } } $ $ {\Large + } ~~ { { \large \left( 2 \omega_0^4 ~+~ 2 \omega_0^2 \gamma \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2} ~+~ 2 \gamma \right) ~+~ \gamma^3 \left( \gamma + \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } \right) \right) \tan^{-1} \left( { \Large { { \huge \omega } \over { \sqrt{ { \Large { \gamma \over 2 } } \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~-~ \gamma \right) ~-~ \omega_0^2 } } } } \right) } \over { \large \sqrt{ 2 } ~ \gamma \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } \sqrt{ -~ \gamma \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~+~ \gamma \right) ~-~ 2 \omega_0^2 } } } $ |
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| $ \left( \left( \left( 2 {\omega_0}^4 - {\omega_0}^2 \gamma \left( \sqrt{ 4 {\omega_0}^2 + \gamma^2 } - 2 \gamma \right) + \gamma^3 \left( \gamma - \sqrt{ 4 {\omega_0}^2 + \gamma^2 } \right) \right $ |
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| $ atan( x \over \sqrt{ { 0.5 \gamma \left( \sqrt{ 4 {\omega_0}^2 + \gamma^2 } - \gamma \right) - {\omega_0}^2 } \right) $ $ \left( { \sqrt{2} \gamma \sqrt{ 4 {\omega_0}^2 + \gamma^2 } \sqrt{ \gamma \left{ \sqrt{ 4 {\omega_0}^2 + \gamma^2 } - 2 \gamma \right) - 2 {\omega_0}^2 } right) } right) $ |
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Rayleigh Scattering of Isolated Species
( Species == ions, atoms, molecules )
- See Polarization for the low wavenumber (frequency / speed of light ) approximation used for Rayleigh scattering.
Scattering is due to the polarization of species. The polarization can be summed from the behavior of individual resonances and damping factors (related to resonance bandwidth), which I have not yet been able to find. For mostly-isolated atoms in high vacuum, Beers line broadening will not be relevant; the bandwidth ~ \large \gamma ~ is related to damping time, TBD
note: perhaps I can get the relevant numbers from HITRAN, but many of the resonances (especially for tightly bound molecules and deep atomic orbitals) will be far into the ultraviolet, where HITRAN may not go. TBD
The scattering from a single resonator at frequency ~ \large \omega ~ is (from Feynman Lectures on Physics Chapter X page X) proportional to
{ \Large \int{ \omega^4 \over { ( \omega^2 ~-~ \omega_0^2 )^2 ~-~ \gamma^2 \omega^2 } } } ~= \omega ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ {\Large - } ~~ { { \large \left( 2 \omega_0^4 ~-~ 2 \omega_0^2 \gamma \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~-~ 2 \gamma \right) ~+~ \gamma^3 \left( \gamma - \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } \right) \right) \tan^{-1} \left( { \Large { { \huge \omega } \over { \sqrt{ { \Large { \gamma \over 2 } } \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~-~ \gamma \right) ~-~ \omega_0^2 } } } } \right) } \over { \large \sqrt{ 2 } ~ \gamma \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } \sqrt{ \gamma \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~-~ \gamma \right) ~-~ 2 \omega_0^2 } } } {\Large + } ~~ { { \large \left( 2 \omega_0^4 ~+~ 2 \omega_0^2 \gamma \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2} ~+~ 2 \gamma \right) ~+~ \gamma^3 \left( \gamma + \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } \right) \right) \tan^{-1} \left( { \Large { { \huge \omega } \over { \sqrt{ { \Large { \gamma \over 2 } } \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~-~ \gamma \right) ~-~ \omega_0^2 } } } } \right) } \over { \large \sqrt{ 2 } ~ \gamma \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } \sqrt{ -~ \gamma \left( \sqrt{ 4 \omega_0^2 ~+~ \gamma^2 } ~+~ \gamma \right) ~-~ 2 \omega_0^2 } } }