refraction (original) (raw)

Definition: the change in the propagation direction when a wave comes from one medium into another one

Category: article belongs to category general optics general optics

Related: refractive indextotal internal reflectionvelocity of lightFresnel equationsprismschromatic dispersion

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DOI: 10.61835/vke Cite the article: BibTex BibLaTex plain textHTML Link to this page! LinkedIn

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Contents

What is Refraction?

Typical Cases Involving Refraction

Additional Remarks

Total Internal Reflection

Lossy Materials

Reflected Beam

Double Refraction

Negative Refraction and Superprism effects

Refraction of X-rays

Frequently Asked Questions

What is refraction?

What is Snell's law?

Why does light change direction when entering a different medium?

What are some common applications of refraction?

What is total internal reflection?

What is double refraction?

Summary:

This article provides a comprehensive introduction to the phenomenon of refraction, which is the change in the propagation direction of light when it passes from one medium to another. It explains the physical origin of refraction and presents Snell's law, which mathematically describes the relationship between the angles of incidence and refraction and the refractive indices of the media.

The text also covers various important applications, such as in optical lenses and prisms, and related phenomena including total internal reflection, double refraction in birefringent materials, and more exotic effects like negative refraction in metamaterials.

(This summary was generated with AI based on the article content and has been reviewed by the article’s author.)

What is Refraction?

When light, e.g. a laser beam, propagates from one transparent homogeneous medium into another, its propagation direction will generally change (see Figure 1). This phenomenon is called refraction.

Refraction can be understood by considering the conditions which the incoming and the transmitted waves need to fulfill at the boundary between the two media. Essentially, the tangential components of the wave vectors need to be identical, as otherwise the phase difference between the waves at the boundary would be position-dependent, and the wavefronts could not be continuous. As the magnitude of the wave vector depends on the refractive index of the medium, the said condition can in general only be fulfilled with different propagation directions. An exception is of course the case of normal incidence, where the wave vectors have no component along the surface.

refraction at an interface

Figure 1: Refraction at an interface between two media.

From the above considerations, one can easily derive Snell's law (the law of Snellius) for the angles: {n_1}\sin {\theta _1} = {n_2}\sin {\theta _2}$$

where ($n_1$) and ($n_2$) are the refractive indices of the two media. It is apparent that the larger angle to the normal direction must occur in the medium with the smaller refractive index.

As the refractive index of typical optical materials is between 1.4 and 2, refraction often causes substantial changes in propagation angle, which can be significantly different for different materials.

Figure 2 is an animated illustration of refraction. One can see that the wavelength is smaller on the right side (as a result of the reduced velocity of light), where the refractive index is larger. Also, the wavefronts are not interrupted at the interface, but only changed in direction. This is possible only with a modified angle of propagation.

animated illustration of refraction

Figure 2: An animated illustration of refraction. The wavefronts are shown as gray lines. The change in direction results from the reduced velocity of light in the right medium.

The amplitude transmission and reflection coefficients of the boundary are described by the Fresnel equations.

Typical Cases Involving Refraction

The phenomenon of refraction is very often encountered in general optics and other fields of photonics:

Total Internal Reflection

If the incident beam comes from the medium with the higher refractive index, and its angle of incidence is large, it may not be possible to fulfill Snell's law with any output angle, since the sine of the output angle can be at most 1. In that case, transmission is not possible — total internal reflection occurs.

Lossy Materials

Snell's law holds for lossless materials, i.e., with negligible absorption. Alternative equations for lossy materials can be derived, but such analysis involves complicated considerations. For example, simply working with complex refractive indices leads to complex angles, which raises questions of how to interpret such angles. Also, situations with non-normal incidence of a plane wave lead to waves in absorbing media which are no longer plane waves, since there is a transverse variation of the modulus of the complex amplitude.

Note, however, that substantial deviations from Snell's law are to be expected only in cases where the imaginary part of the refractive index becomes substantial — which is not the case in many cases of practical interest.

Reflected Beam

For the reflected beam, the angle to the surface normal is always the same as that of the incident beam (($\theta_1$)): its direction is not affected by refraction.

Double Refraction

For non-isotropic media, the refractive index can depend on the polarization direction of the light. Therefore, the refraction angle can be polarization-dependent. One obtains double refraction: different output beams for s and p polarization.

Negative Refraction and Superprism effects

Unusual phenomena such as negative refraction [3, 4] can occur with photonic metamaterials with a negative refractive index, at certain photonic metasurfaces, or with certain photonic crystals. Here, the refracted beam can be on the same side of the surface normal as the incident beam.

Another curious refraction phenomenon is the superprism effect [1, 2], where the refraction angle exhibits an unusually strong dependence of the propagation direction at the output on details like the input direction and the optical wavelength.

Refraction of X-rays

For electromagnetic radiation at very high frequencies, such as X-rays, refraction effects are far weaker than for light, since the refractive index is then close to 1.

Frequently Asked Questions

This FAQ section was generated with AI based on the article content and has been reviewed by the article’s author (RP).

What is refraction?

Refraction is the change in propagation direction that light experiences when moving from one transparent medium to another. This phenomenon is described by Snell's law.

What is Snell's law?

Snell's law is a formula relating the angles of incidence ($\theta_1$) and refraction ($\theta_2$) to the refractive indices ($n_1$) and ($n_2$) of the two media: ($n_1 \sin \theta_1 = n_2 \sin \theta_2$).

Why does light change direction when entering a different medium?

The direction change is necessary to maintain the continuity of wavefronts at the boundary. As the velocity of light and wavelength change with the medium's refractive index, the propagation angle must adjust to keep the phase relationship constant along the interface.

What are some common applications of refraction?

Refraction is a fundamental principle used in many optical components, including lenses for focusing or imaging light, and prisms for separating different wavelength components.

What is total internal reflection?

Total internal reflection occurs when light travels from a medium with a higher refractive index to one with a lower index at a sufficiently large angle of incidence. Beyond a certain critical angle, the light cannot be transmitted and is completely reflected.

What is double refraction?

Double refraction occurs in non-isotropic (or birefringent) materials, where the refractive index depends on the polarization of light. As a result, an incident light beam can be split into two beams with different polarizations, which are refracted at different angles.

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Bibliography

[1] H. Kosaka et al., “Superprism phenomena in photonic crystals”, Phys. Rev. B 58, R10096 (1998); doi:10.1103/PhysRevB.58.R10096
[2] H. Kosaka et al., “Superprism phenomena in photonic crystals: toward microscale lightwave circuits”, J. Lightwave Technol. 17 (11), 2032 (1999); doi:10.1109/50.802991
[3] S. Foteinopoulou, E. N. Economou and C. M. Soukoulis, “Refraction in media with a negative refractive index”, Phys. Rev. Lett. 90, 107402 (2003); doi:10.1103/PhysRevLett.90.107402
[4] E. Cubukcu et al., “Negative refraction by photonic crystals”, Nature 423, 604 (2003); doi:10.1038/423604b
[5] N. Yu, “Light propagation with phase discontinuities: Generalized laws of reflection and refraction”, Science 334 (6054), 333 (2011); doi:10.1126/science.1210713
[6] F. Aieta et al., “Out-of-plane reflection and refraction of light by anisotropic optical antenna metasurfaces with phase discontinuities”, Nano Lett. 12, 1702 (2012); doi:10.1021/nl300204s
[7] S. Larouche and D. R. Smith, “Reconciliation of generalized refraction with diffraction theory”, Opt. Lett. 37 (12), 2391 (2012); doi:10.1364/OL.37.002391

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