multimode beams (original) (raw)

Author: the photonics expert (RP)

Definition: light beams in free space or in transparent media which involve multiple (often many) modes, frequently with highly random characteristics

Categories: article belongs to category general optics general optics, article belongs to category physical foundations physical foundations

Related: light beamslaser beamsdiffraction-limited beamscoherenceGaussian beamsmultimode fibers

Opposite terms: diffraction-limited beams, single-mode beams

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DOI: 10.61835/8ud Cite the article: BibTex BibLaTex plain textHTML Link to this page! LinkedIn

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Contents

What are Multimode Beams?

Monochromatic Multimode Beams

Polychromatic Multimode Beams

Evolution of Free-space Intensity Profiles

Limitations of Multimode Beams

Beam Quality

Smooth Intensity Profiles

Amplification and Transmission Through Optical Components

Frequently Asked Questions

Summary: This article explains the concept of multimode beams, which consist of multiple spatial modes. It details the differences between monochromatic beams, which exhibit granular speckle patterns due to interference, and polychromatic beams, which often have smoother intensity profiles.

The text also covers the evolution of beam profiles during propagation and discusses key limitations of multimode beams, such as their poor beam quality (high [[_M_^2 factor]]) and incompatibility with single-mode optical components like [[single-mode fibers]].

What are Multimode Beams?

Multimode beams are light beams in free space or in transparent optical materials which involve multiple spatial modes. The conceptually simplest situations are encountered in cases involving waveguide structures such as optical fibers, where there is a well-defined set of waveguide modes, and the total optical power is spread over some (often large) number of such modes. In the case of free-space light beams, one may choose a set of free-space propagation modes, e.g. TEM modes for a given beam radius of the fundamental Gaussian mode, but that choice is arbitrary. The number of involved modes is then dependent on that choice.

Frequently, multimode beams have highly random characteristics because a large number of modes is involved, where the distribution of powers and the optical phases of the particular modes are not known in detail, but are only statistically described.

In principle, a laser beam with a single spatial mode but multiple frequency components may also be called multimode, but what is usually meant is a beam involving multiple spatial modes.

Monochromatic Multimode Beams

The simplest cases are (quasi-)monochromatic multimode beams, i.e., those involving only a single optical frequency. Such a beam may arise, for example, by launching light from a single-frequency laser into a multimode fiber, where the input beam profile is not matched to one particular fiber mode. By using an optical diffuser, or alternatively by strong bending of a section of fiber, one may obtain a broader distribution of optical power over the fiber modes.

As an example, Figure 1 shows a simulated intensity profile of multimode radiation in a fiber, which is largely restricted to the area of the fiber core.

multimode profile

Figure 1: Intensity profile of monochromatic multimode radiation in a multimode fiber with a core diameter of 50 μm. (For details of its computation, see an article on generating multimode beam profiles.) After only a few micrometers of propagation, the details of the pattern are substantially modified.

It is characteristic for monochromatic multimode beams that the intensity profile exhibits a granular pattern as seen in Figure 1. That arises from the interference of the many mode fields, most of which exhibit oscillating amplitude patterns. The more higher-order modes are involved, which exhibit a stronger beam divergence, the finer are the granular structures.

The details of the intensity profile (e.g. the positions of intensity maxima) change during propagation along the fiber (often already within a couple of micrometers) as the relative optical phases of the modes change due to their different propagation constants.

Similar results would be obtained when a multimode free-space beam is generated, e.g. by sending a single-frequency laser beam first through an optical diffuser and then through an aperture which limits the beam divergence. Again, one would obtain a granular intensity pattern which changes during propagation.

For numerical simulations of monochromatic multimode beam propagation, one generally uses some kind of beam propagation method.

Polychromatic Multimode Beams

Substantial new aspects come into play when considering polychromatic multimode beams. Generally, the different frequency components of such a beam will exhibit different amplitude and intensity patterns — often with similar granular structures, but with the maxima and minima occurring at different locations. As a result, the total intensity profile is often quite smooth.

Important details can substantially depend on how such a beam is generated. Some examples:

Numerical simulations of the propagation of polychromatic multimode beams may again be based on numerical beam propagation. Here, a representative set of frequency components is selected, a monochromatic propagation is performed for each one, and the results are combined (e.g. by adding up the intensity profiles). Alternative numerical methods such as ray tracing are based on a statistical distribution of the light field, involving a limited set of parameters. Such methods can be computationally much more efficient, particularly in cases where a large number of frequency components and/or long propagation distances are involved.

Evolution of Free-space Intensity Profiles

In contrast to Gaussian beams, for example, which maintain their Gaussian shape during propagation (with changes only of the beam radius), the shape of the transverse intensity profile for multimode beam will generally change during propagation. For example, the beam profile of a diode bar at a short distance after an applied fast axis collimator has an approximately supergaussian intensity profile in the “long” direction. After longer propagation distance, however, the profile will be closer to Gaussian, reflecting the angular intensity distribution. The supergaussian profile may be obtained again when focusing the beam with a lens — but only around the beam focus.

Limitations of Multimode Beams

Beam Quality

Multimode beams generally have a relatively poor beam quality (far from diffraction-limited), i.e., a low spatial coherence — particularly when a large number of modes is involved. Typically, the beam quality is quantified with the beam parameter product or the _M_2 factor. It can be measured with certain beam profilers.

Smooth Intensity Profiles

As explained above, a multimode beam can have a smooth intensity profile only if it is polychromatic. Therefore, single-mode beams are required when monochromatic radiation with a smooth intensity profile is required. For example, Gaussian beams are then often used.

Amplification and Transmission Through Optical Components

Multimode beams cannot be transmitted through single-mode fibers. Most fiber amplifiers can amplify only single-mode or few-mode light. One can also make fiber amplifiers for highly multimode radiation by using a large multimode fiber core, but that leads to substantially reduced gain efficiency and mode-dependent gain.

For efficiently launching a multimode beam into a multimode fiber, the beam profile at the input facet of the fiber needs to be limited to the fiber core, and at the same time the beam divergence must not exceed the limit set by the numerical aperture of the fiber.

Even various bulk-optical devices are more or less limited to working with single-mode beams only. For example, and acousto-optic modulator may in principle work with multimode beams, but it may require substantial beam focusing while at the same time the beam divergence needs to be limited; optimal performance may thus be obtained only with single-mode beams.

Frequently Asked Questions

What is a multimode beam?

A multimode beam is a light beam which involves multiple spatial modes. This means the total optical power is distributed over several distinct beam shapes, which is common in waveguides like multimode optical fibers.

Why do monochromatic multimode beams have a granular or speckled appearance?

The granular intensity pattern of a monochromatic multimode beam arises from the interference of its many spatial mode fields. The pattern's structure becomes finer as more higher-order modes with stronger beam divergence are involved.

Why are the intensity profiles of polychromatic multimode beams often smooth?

Polychromatic multimode beams often have a smooth intensity profile because the granular patterns from different frequency components average out. In contrast, monochromatic beams usually show a strong speckle pattern.

What is the beam quality of a multimode beam?

Can a multimode beam be transmitted through a single-mode fiber?

No, multimode beams cannot be transmitted through single-mode fibers. Additionally, most fiber amplifiers are designed to work only with single-mode or few-mode light.

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