The Goos-Hanchen Shift. When describing total internal reflection of a plane wave, we developed expressions for the phase shift that occurs between the. Goos-Hänchen effect in microcavities. Microcavity modes created by non- specular reflections. This page is primarily motivated by our paper. these shifts as to the spatial and angular Goos-Hänchen (GH) and Imbert- Fedorov (IF) shifts. It turns out that all of these basic shifts can occur in a generic beam.
|Published (Last):||13 September 2010|
|PDF File Size:||4.35 Mb|
|ePub File Size:||10.97 Mb|
|Price:||Free* [*Free Regsitration Required]|
Specular reflection with phase shifts artificially removed. Email Required, but never shown.
Goos-hancheh effect occurs because the reflections of a finite sized beam will interfere along a line transverse to the average propagation direction. Essentially, rays can be understood as fictitious particles that are pushed forward by the wave fronts like surfers riding toward the beach.
The pair u, s in the middle is the one created in the bifurcation mentioned above. This is not related to Goos-Hanchen, which depends on coherence of the source. The horizontal axis is the angle of incidence of a ray at the planar mirror, and the vertical axis measures the “rate of change” of that angle between bounces. Conversely, what we learn here about light waves is equally applicable to quantum particles, because all of them can also act like waves.
When the light is totally reflected in the interface between dense and less-dense medium, we know that the reflected beam will shift a little. Thus, bythe GHS had been firmly established. See examples for the circular dieletric on a separate page. This acts as an ideal curved mirror, and the cavity is closed off by a planar, dielectric multilayer Bragg mirror. Compared to general ovals of identical eccentricity, it goos-hannchen typically a good approximation to consider the dielectric ellipse as non-chaotic, as can be seen on this page discussing dynamical eclipsing.
Which question are you asking? So if the phases of different plane waves are shifted differently upon reflection, the transverse shape of the reflected beam will be modified.
electromagnetism – The Goos Hanchen shift mechanism – Physics Stack Exchange
This means in particular that the internal dynamics of the ellipse should not display any traces of chaotic ray sift.
BermanUniversity of Michigan.
Yes, but so could you after reading this page However, we do know that Newton’s ideas about light are by no means obsolete:. Compared to the dielectric ellipse, our dome cavity simulations are actually much more difficult to do because we’re dealing with a 3D structure with mixed boundary conditions, leakiness and polarization-dependent effects.
This becomes even more important when the reflecting interface is not between a homogeneous dielectric and empty space. The phenomenon is actually wholly analogous to quantum tunnelling by a first quantised particle field described by e.
Home Questions Tags Users Unanswered. This is true not only for the ellipse, but even for the mundane rectangle.
Goos-Hänchen effect in microcavities
BermanScholarpedia, 7 3: Since the effect is very small, on the order of several optical wavelengths, they multiplied the relative shift gpos-hanchen the light that was totally internally reflected and the light that was reflected from the silver by using an “optical waveguide” parallel surfaces between which many reflections occurred that allowed them to increase the relative shift by a factor of 70 or so, limited mainly by losses in reflections from the silver strip.
However, the effect has for good reason been studied mostly in the context of planar interfacesand not voos-hanchen ones such as ellipses. Although it is also possible to make a convincing argument for the existence of the effect in circular cavities there are some confusing questions gooss-hanchen arise when generalizing to shapes like the ellipse.
Some paper explained this phenomenon as the light penetrates the less-dense medium a little, and re-emerge again, just like it is reflected by some virtual plane in the less-dense, but how can this be explained?
Many standard optical setups in particular when Gaussian beams are involved can be described fully by identifying one or a few rays, and decorating them with suitable wave patterns i. Although the interface between an elipse and the surrounding medium coincides with the coordinate lines of the elliptic cylinder coordinate systemthe wave field on the boundary cannot be assumed to have a constant value or constant derivatives, for that matter.
The work to be described below and in  relies on such mirrors. This makes beams different from plane waves, which form wave fronts of infinite width.
The incident radiation pulse is not scattered instantaneously by the surface, but reemerges into medium 1 after a time delay given by. Andy Huang 12 4. Its characteristics such as the frequencies at which it will appear in the spectrum, and its spot size on the mirror plane can then be predicted.
But only stable rays can be used to construct transversally confined wave modes of goos-hahchen cavity.
Goos-Hänchen effect – Scholarpedia
What better way to learn about science than televesion, right? So far as I can tell by reading a couple refs, it is a coherent interference effect for an input beam of finite width. Sign up using Facebook.
In such a seemingly pathological situation it’s especially interesting to ask what the relation between the ray and wave description of the system looks like. And in the future, other non-specular effects will likely enter the game as well, enriching both the repertoire of billiard physics and our understanding of realistic optical microcavities.
In goos-hancgen words, I end up doing a new type of goos-ahnchen simulation in which reflections are not specular, but to which the same methods can be sihft that are known from our previous work . IzhikevichEditor-in-Chief of Scholarpedia, the peer-reviewed open-access encyclopedia Accepted on: