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== ルイヴィトンの新作長財布 ==
[[File:Fano-resonance-scs.png|thumb|right|Plot of scattering cross-section versus normalized energy for various values of the parameter q illustrating the asymmetric Fano line-shape.]]
In [[physics]], a '''Fano resonance''' is a type of resonant scattering phenomenon that gives rise to an asymmetric line-shape. Interference between a background and a resonant scattering process produces the asymmetric line-shape. It is named after Italian physicist [[Ugo Fano]] who gave a theoretical explanation for the scattering line-shape of inelastic scattering of electrons from helium.<ref>“ A. Bianconi  [http://arxiv.org/abs/cond-mat/0211452 Ugo Fano and shape resonances] in X-ray and Inner Shell Processes” AIP Conference Proceedings (2002): (19th Int. Conference Roma June 24–28, 2002) A. Bianconi arXiv: cond-mat/0211452 21 November 2002</ref><ref>[[Ugo Fano]] (1961) "Effects of Configuration Interaction on Intensities and Phase Shifts," Phys. Rev. '''124''', pp. 1866–1878 {{DOI|10.1103/PhysRev.124.1866}}</ref> However [[Ettore Majorana]] was the first to discover this phenomenon.<ref>Alessandra Vittorini-Orgeas, Antonio Bianconi [http://www.springerlink.com/content/j703124770742351/ "From Majorana Theory of Atomic Autoionization to Feshbach Resonances in High Temperature Superconductors"] Journal of Superconductivity and Novel Magnetism, 22, 215-221 (2009)</ref> Because it is a general [[wave]] phenomenon, examples can be found across many areas of physics and engineering.


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== History ==
The explanation of the Fano line-shape first appeared in the context of inelastic electron scattering by helium and [[autoionization]]. The incident electron doubly excites the atom to the <math>2s2p</math> state, a sort of [[shape resonance]]. The doubly excited atom spontaneously decays by ejecting one of the excited electrons. Fano showed that interference between the amplitude to simply scatter the incident electron and the amplitude to scatter via autoionization creates an asymmetric scattering line-shape around the autoionization energy with a line-width very close to the inverse of the autoionization lifetime.


== ヴィトン 財布 とは ==
== Explanation ==
The Fano resonance line-shape is due to [[Interference (wave propagation)|interference]] between two scattering amplitudes, one due to scattering within a continuum of states (the background process) and the second due to an excitation of a discrete state (the resonant process). The energy of the resonant state must lie in the energy range of the continuum (background) states for the effect to occur. Near the resonant energy, the background scattering amplitude typically varies slowly with energy while the resonant scattering amplitude changes both in magnitude and phase quickly. It is this variation that creates the asymmetric profile.


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For energies far from the resonant energy the background scattering process dominates. Within <math>2\Gamma_\mathrm{res}</math> of the resonant energy, the phase of the resonant scattering amplitude changes by <math>\pi</math>. It is this rapid variation in phase that creates the asymmetric line-shape.


== ビトン ブランド財布 ==
Fano showed that the total scattering cross-section <math>\sigma</math> assumes the following form,


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<math> \sigma \approx \frac{\left(q\Gamma_\mathrm{res}/2 + E - E_\mathrm{res}\right)^2}{\left(\Gamma_\mathrm{res}/2\right)^2 + \left(E-E_\mathrm{res}\right)^2}</math>
 
where <math>\Gamma_\mathrm{res}</math> describes the line width of the resonant energy and q, the Fano parameter, measures the ratio of resonant scattering to the direct (background) scattering amplitude. (This is consistent with the interpretation within the [[Feshbach–Fano partitioning]] theory.) In the case the direct scattering amplitude vanishes, the q parameter becomes infinite and the Fano formula boils down to the usual [[relativistic Breit–Wigner distribution|Breit–Wigner]] (Lorentzian) formula:
 
<math>\frac{\left(\Gamma_\mathrm{res}/2\right)^2}{\left(\Gamma_\mathrm{res}/2\right)^2 + \left(E-E_\mathrm{res}\right)^2}</math>
 
== Examples ==
Examples of Fano resonances can be found in atomic physics, nuclear physics, condensed matter physics, circuits, microwave engineering, nonlinear optics and nanophotonics.
 
==References==
 
{{Reflist}}
 
[[Category:Quantum mechanics]]
[[Category:Quantum field theory]]
[[Category:Scattering]]

Revision as of 03:34, 28 October 2013

File:Fano-resonance-scs.png
Plot of scattering cross-section versus normalized energy for various values of the parameter q illustrating the asymmetric Fano line-shape.

In physics, a Fano resonance is a type of resonant scattering phenomenon that gives rise to an asymmetric line-shape. Interference between a background and a resonant scattering process produces the asymmetric line-shape. It is named after Italian physicist Ugo Fano who gave a theoretical explanation for the scattering line-shape of inelastic scattering of electrons from helium.[1][2] However Ettore Majorana was the first to discover this phenomenon.[3] Because it is a general wave phenomenon, examples can be found across many areas of physics and engineering.

History

The explanation of the Fano line-shape first appeared in the context of inelastic electron scattering by helium and autoionization. The incident electron doubly excites the atom to the 2s2p state, a sort of shape resonance. The doubly excited atom spontaneously decays by ejecting one of the excited electrons. Fano showed that interference between the amplitude to simply scatter the incident electron and the amplitude to scatter via autoionization creates an asymmetric scattering line-shape around the autoionization energy with a line-width very close to the inverse of the autoionization lifetime.

Explanation

The Fano resonance line-shape is due to interference between two scattering amplitudes, one due to scattering within a continuum of states (the background process) and the second due to an excitation of a discrete state (the resonant process). The energy of the resonant state must lie in the energy range of the continuum (background) states for the effect to occur. Near the resonant energy, the background scattering amplitude typically varies slowly with energy while the resonant scattering amplitude changes both in magnitude and phase quickly. It is this variation that creates the asymmetric profile.

For energies far from the resonant energy the background scattering process dominates. Within 2Γres of the resonant energy, the phase of the resonant scattering amplitude changes by π. It is this rapid variation in phase that creates the asymmetric line-shape.

Fano showed that the total scattering cross-section σ assumes the following form,

σ≈(qΓres/2+E−Eres)2(Γres/2)2+(E−Eres)2

where Γres describes the line width of the resonant energy and q, the Fano parameter, measures the ratio of resonant scattering to the direct (background) scattering amplitude. (This is consistent with the interpretation within the Feshbach–Fano partitioning theory.) In the case the direct scattering amplitude vanishes, the q parameter becomes infinite and the Fano formula boils down to the usual Breit–Wigner (Lorentzian) formula:

(Γres/2)2(Γres/2)2+(E−Eres)2

Examples

Examples of Fano resonances can be found in atomic physics, nuclear physics, condensed matter physics, circuits, microwave engineering, nonlinear optics and nanophotonics.

References

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  1. ↑ “ A. Bianconi Ugo Fano and shape resonances in X-ray and Inner Shell Processes” AIP Conference Proceedings (2002): (19th Int. Conference Roma June 24–28, 2002) A. Bianconi arXiv: cond-mat/0211452 21 November 2002
  2. ↑ Ugo Fano (1961) "Effects of Configuration Interaction on Intensities and Phase Shifts," Phys. Rev. 124, pp. 1866–1878 Electronic Instrument Positions Staff (Standard ) Cameron from Clarence Creek, usually spends time with hobbies and interests which include knotting, property developers in singapore apartment For sale and boomerangs. Has enrolled in a world contiki journey. Is extremely thrilled specifically about visiting .
  3. ↑ Alessandra Vittorini-Orgeas, Antonio Bianconi "From Majorana Theory of Atomic Autoionization to Feshbach Resonances in High Temperature Superconductors" Journal of Superconductivity and Novel Magnetism, 22, 215-221 (2009)
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