How do you increase the diameter of a laser beam?

How do you increase the diameter of a laser beam?

Beam expanders are optical systems for increasing or decreasing the diameter of a laser beam. A beam expander can enlarge an input beam by the factor M, but it can also reduce it by the factor 1/M with a reversed optical beam path. Usually beam expanders are used to increase the diameter of laser beams.

Does a laser beam expand with distance?

All laser beams diverge. Only an infinitely wide beam (a plane wave) does not spread out, and therefore has parallel waves. Divergence is observed by shining a laser light on a wall and then seeing the spot grow bigger as you move away from the wall.

How do you reduce the size of a beam?

The only way to make the spot size smaller is to use a lens of shorter focal length or expand the beam. If this is not possible because of a limitation in the geometry of the optical system, then this spot size is the smallest that could be achieved.

What is the beam of a laser?

Lasers produce a narrow beam of light in which all of the light waves have very similar wavelengths. The laser’s light waves travel together with their peaks all lined up, or in phase. This is why laser beams are very narrow, very bright, and can be focused into a very tiny spot.

How far can a laser beam go?

Around 100 meters away from a red laser pointer, its beam is about 100 times wider and looks as bright as a 100-watt light bulb from 3 feet away. Viewed from an airplane 40,000 feet in the air — assuming there’s no clouds or smog — the pointer would be as bright as a quarter moon.

Can laser reach moon?

The typical red laser pointer is about 5 milliwatts, and a good one has a tight enough beam to actually hit the Moon—though it’d be spread out over a large fraction of the surface when it got there. The atmosphere would distort the beam a bit, and absorb some of it, but most of the light would make it.

How do you focus a laser beam?

basically, the focusing of a laser beam is achieved by using a single- or multi-lens laser optic, that is mainly characterized by its focal length and the diameter of the free aperture. Figure 1 shows the transformation of a laser beam through an ideal optical lens with a focal length f.

What is the purpose of laser beam?

laser, a device that stimulates atoms or molecules to emit light at particular wavelengths and amplifies that light, typically producing a very narrow beam of radiation. The emission generally covers an extremely limited range of visible, infrared, or ultraviolet wavelengths.

What are laser beams used for?

Lasers are used in optical disc drives, laser printers, barcode scanners, DNA sequencing instruments, fiber-optic, semiconducting chip manufacturing (photolithography), and free-space optical communication, laser surgery and skin treatments, cutting and welding materials, military and law enforcement devices for …

How does a Keplerian laser beam expander work?

In the design of a laser beam expander, the objective and image lenses are reversed. In a Keplerian beam expander the input beam is focussed to a point between the two lenses. This creates a spot of concentrated energy within the beam expander which heats the air within the system and deflects light from it’s optical path.

How does a laser beam expander affect diffraction?

In regards to diffraction, the shorter the focal length, the smaller the spot size. More importantly, the larger the input beam diameter the smaller the spot size. By expanding the beam within the system, the input diameter is increased by a factor of MP, reducing the divergence by a factor of MP.

How is the beam divergence of a beam expander expressed?

This can be done using the formula: Beam divergence is expressed as a full angle in terms of θ I and not θ I /2 . Because a beam expander will increase the beam diameter and decrease the beam divergence by it’s magnifying power, we can combine these equations to give us:

Where are the object rays located in a laser beam expander?

Contemporary laser beam expander designs are afocal systems that developed from well-established optical telescope fundamentals. In such systems, the object rays, located at infinity, enter parallel to the optical axis of the internal optics and exit parallel to them as well.

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