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Photonic crystal

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A photonic crystal is an optical nanostructure characterized by a periodic change in its refractive index. The refractive index is a measure of how much light slows down when traveling through a material. By arranging materials in repeating patterns, these crystals can control how light waves move through them. This process is similar to how the atomic lattice of a semiconductor affects the movement of electrons.

Teinopalpus imperialis verso
Teinopalpus imperialis verso

In nature, these structures create colors through structural coloration, such as the iridescent shimmer seen in opal gemstones.

Opal Armband 800pix
Opal Armband 800pix

Because they can manipulate light, they are essential to the field of photonics, which is the study of light and optical engineering.

The mechanism of a photonic crystal relies on regularly repeating regions of high and low refractive index. When light waves encounter these repeating boundaries, they may propagate through the structure or be blocked entirely. The specific wavelengths that are allowed to pass through are called modes, and the ranges of these wavelengths are called bands. Conversely, the ranges of wavelengths that cannot pass through are known as photonic band gaps. This phenomenon occurs due to destructive interference. This happens when multiple reflections of light at the interfaces between layers cancel each other out.

To open a complete photonic band gap, scientists can increase the refractive index contrast or make the Brillouin zone more similar to a sphere.

Photonic crystals are categorized by their dimensions: one, two, or three dimensions. One-dimensional crystals are often created by depositing thin film layers on top of each other. These are used to create dielectric mirrors, which produce ultra-high reflectivity at specific wavelengths. Two-dimensional crystals can be fabricated using photolithography or by drilling holes into a substrate.

PMMA03
PMMA03

A common example of a two-dimensional structure is the photonic-crystal fiber, which contains air holes to guide light. These fibers are used extensively in fiber-optic communication.

Photonic-crystal-fiber-from-NRL
Photonic-crystal-fiber-from-NRL

Three-dimensional crystals are the most complex to produce. They can be made through direct laser writing, stacking 2-D layers, or by using self-assembly, where spheres settle into a pattern within a matrix.

The history of this field began with early experiments in the late 19th century. In 1887, the English physicist Lord Rayleigh experimented with periodic multi-layer dielectric stacks. He demonstrated that these stacks could create a one-dimensional photonic band-gap, also known as a stop-band. In 1973, Melvin M. Weiner described these systems as "discrete phase-ordered media" in a patent. However, the modern term "photonic crystal" did not emerge until 1987. This was following two milestone papers by Eli Yablonovitch and Sajeev John. Yablonovitch aimed to control the spontaneous emission of materials, while John focused on using crystals to localize and control light.

Significant milestones followed the 1987 research surge. In 1991, Yablonovitch demonstrated the first three-dimensional photonic band-gap using the microwave regime. He achieved this by drilling an array of holes in a transparent material to create an inverse diamond structure called Yablonovite. In 1996, Thomas Krauss demonstrated a two-dimensional photonic crystal at optical wavelengths. This was a major step because it allowed researchers to use methods from the semiconductor industry. In 1998, Philip Russell developed photonic-crystal fibers, which offer enhanced properties over standard optical fibers. These developments moved the field from theoretical physics into practical, measurable technology.

The scale of these structures is incredibly small. For a photonic crystal to exhibit interference effects, the repeating pattern must be around or larger than half the wavelength of the light. Visible light has wavelengths between approximately 400 nanometers for violet and 700 nanometers for red. Because the wavelength changes depending on the material, these repeating regions must be fabricated at the nanoscale. This precision is why many early studies were conducted in the microwave regime. At microwave frequencies, the structures can be built at a much more accessible centimeter scale due to scale invariance.

Looking forward, the applications for these crystals are vast. Three-dimensional photonic crystals may one day be used to develop optical computers. They also hold the potential to create more efficient photovoltaic cells for solar energy. Researchers are currently investigating photonic crystal slabs, which are two-dimensional structures etched into semiconductor slabs. These slabs use total internal reflection to confine light. Scientists hope to use these in integrated computer chips to improve how information is processed. By mastering the control of light at the smallest scales, photonics promises to transform modern computing and communication systems.

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🖼️ Images & Media (7)
File:Opal Armband 800pix.jpg
Opal Armband 800pix.jpg
File:Teinopalpus imperialis verso.JPG
Teinopalpus imperialis verso.JPG
Photonic Band Gap vs Wavelength.webm
File:Photonic-crystal-fiber-from-NRL.jpg
Photonic-crystal-fiber-from-NRL.jpg
PMMA03.tif
Scattering-Forces-within-a-Left-Handed-Pho...
File:Photonic Crystal 1D DBR aircore epsr12point25 DbyA0point8.png
Photonic Crystal 1D DBR aircore...
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