Creating Coherent Light from UV LEDs and Pinhole Aperture

Click For Summary
SUMMARY

The discussion centers on the feasibility of generating temporally and spatially coherent light using a UV LED and a pinhole aperture. It is established that while a pinhole aperture can facilitate diffraction, creating coherence from a narrow bandwidth light source like a UV LED is possible but limited in efficiency. The concept of spatial coherence is further clarified through the Rayleigh Distance formula, which defines the boundary between Far and Near Radiation Zones, emphasizing the importance of distance and wavelength in achieving coherence.

PREREQUISITES
  • Understanding of light diffraction and wave behavior
  • Familiarity with the concept of spatial and temporal coherence
  • Knowledge of UV LED characteristics and applications
  • Basic grasp of the Rayleigh Distance and its significance in optics
NEXT STEPS
  • Research the principles of light diffraction and its applications in optics
  • Explore the characteristics of UV LEDs and their coherence properties
  • Study the Rayleigh Distance and its implications for spatial coherence
  • Investigate methods to enhance the efficiency of coherence generation using pinhole apertures
USEFUL FOR

Optics researchers, physicists, and engineers interested in light coherence, as well as students studying wave phenomena and optical systems.

dlbi
Messages
5
Reaction score
0
I've read that using a pinhole aperture and a wavelength filter can turn a "white" incoherent light source like a light bulb into a temporally and spatially coherent light source (albeit at low efficiency).

Can a temporally and spatially coherent light source be made with a monoenergetic (or actually narrow bandwidth) light source like a UV LED and a pinhole aperture alone?

Thanks!
 
Science news on Phys.org
dlbi said:
I've read that using a pinhole aperture and a wavelength filter can turn a "white" incoherent light source like a light bulb into a temporally and spatially coherent light source (albeit at low efficiency).

Can a temporally and spatially coherent light source be made with a monoenergetic (or actually narrow bandwidth) light source like a UV LED and a pinhole aperture alone?
The reason why this occurs is due to diffraction of light since light is wave. Waves will curve around solids as they move, so you are able to create something like a light bulb. The strength of the diffraction which occurs is completely up to the wavelength of the light.

Light has a relatively small wavelength to other waves. Sound has quite large wavelengths which means it diffracts around basically everything (doorways, objects, etc.). Since light has a smaller wavelength, the diffraction isn't as much as a sound wave, so you need tiny pinholes to create any kind of light bulb effect.

But to answer your question regarding narrow bandwidth light (UV led), you could create a diffraction. You could create a diffraction with any electromagnetic wave, and anything which acts like a wave to be precise. The only thing changing is the effect of the diffraction.
 
dlbi said:
I've read that using a pinhole aperture and a wavelength filter can turn a "white" incoherent light source like a light bulb into a temporally and spatially coherent light source (albeit at low efficiency).

Can a temporally and spatially coherent light source be made with a monoenergetic (or actually narrow bandwidth) light source like a UV LED and a pinhole aperture alone?

Thanks!
When I was at school it was before the invention of the laser, so we used a Sodium flame and a slit to obtain coherent light for Young's Slits.
I think that spatial coherence will be obtained if a source is very distant, because we then have a plane wave having a uniform phase across our area of interest. It also seems that if we are in the Far Zone of a source we will have spatial coherence, because the boundary of the Far and Near Radiation Zones is where all the rays from the source are approximately in phase. This boundary occurs approximately at the Rayleigh Distance, defined as R = D^2/(2 x lambda), where D is the largest dimension across the source. To take a typical case, for orange light with a 1mm pin hole, R = (10^-3)^2 / (2 x 0.6 x 10^-6) = 83 cm.
 

Similar threads

  • · Replies 14 ·
Replies
14
Views
3K
  • · Replies 24 ·
Replies
24
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 68 ·
3
Replies
68
Views
14K
  • · Replies 10 ·
Replies
10
Views
5K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 16 ·
Replies
16
Views
10K
  • · Replies 3 ·
Replies
3
Views
9K
  • · Replies 1 ·
Replies
1
Views
2K