RP Photonics logo
VL logo part of the
Virtual
Library

Encyclopedia of Laser Physics and Technology

Fresnel Number

previous  |  next  |  feedback

Definition: a parameter determining the regime of diffraction effects

Originally, the Fresnel number was introduced in the context of diffraction theory for beam propagation. If a light wave first passes through an aperture of size (e.g. radius) a and then propagates over a distance L to a screen, the situation is characterized with the Fresnel number

Fresnel number

where λ is the wavelength.

For values of the Fresnel number well below 1, Fraunhofer diffraction occurs where the screen essentially shows the far-field diffraction pattern of the aperture, which is closely related to the spatial Fourier transform of the complex amplitude distribution of the light field after the aperture.

Fresnel numbers around 1 or larger characterize the situation of Fresnel diffraction (or near-field diffraction), where the mathematical description is more complicated. For not too large Fresnel numbers and diffraction angles, the Fresnel approximation can be used.

Fresnel Number of a Resonator

The concept of the Fresnel number has also been applied to optical resonators (cavities), in particular to laser resonators [1]. One again uses the equation

Fresnel number

where a is now the radius of the end mirrors, and L is the resonator length.

A large Fresnel number (well above 1) of a resonator (cavity) means that diffraction losses at the end mirrors are small for typical mode sizes (i.e. not near a stability limit of the resonator, where mode sizes can diverge). This is the usual situation in a stable laser resonator. Conversely, a small Fresnel number means that diffraction losses can be significant – particularly for higher-order modes, so that diffraction-limited operation may be favored.

Most stable laser resonators have a fairly large Fresnel number, whereas small Fresnel numbers occur in unstable resonators, which are sometimes applied in high-power lasers.

The Fresnel number is also important for the analysis of the modes of (plane) Fabry–Pérot interferometers, which extend to the edges of the mirrors.

Bibliography

[1]A. E. Siegman, Lasers, University Science Books, Mill Valley, CA (1986)

See also: optical resonators, laser resonators, Fabry–Pérot interferometers

Categories: general optics, resonators

arrow
Home New articles Spotlight Feedback Advertising
Categories Search Quiz Links Page hits
F

This encyclopedia is provided by
RP Photonics Consulting GmbH.

Utilize the expertise of the author, Dr. Rüdiger Paschotta, also in the form of technical consulting services!

A.L.S. logo

A.L.S. GmbH

Picosecond laser diodes
<30 ps, 375 – 1600 nm, >1 Wp, single shot – 120 MHz

RP Q-switch

A powerful software tool for designing
Q-switched lasers. See the details.

RP Fiber Power

This software helps to design and analyze fiber amplifiers and lasers.

TRUMPF logo

TRUMPF-Laser

a leading supplier of industrial diode pumped solid state lasers,
CO2 lasers, and laser systems for material processing.

Onefive logo

Onefive

Low-noise
femtosecond,
picosecond,
and tunable single-frequency lasers for OEM and R&D applications.

Field Guide to Lasers

This new book by Dr. Paschotta explains principles and types of lasers.

Your Advertisement at This Place

will be seen by many thousands of visitors per month. These banners receive far over 100'000 page hits per month. Check the details.