Optical fibers and cables are used to transmit optical energy and information over short or long distances. Over the past few decades, the combination of optical fibers with semiconductor laser diodes and optical receivers has rapidly advanced optical fiber communication systems.

An optical fiber is a dielectric waveguide with a circular cross-section, consisting of a core surrounded by a concentric cladding with slightly lower refractive index (approximately 1%). Optical fibers are typically made of silica doped with materials like GeO₂, which alters the refractive index of the silica. Optical fiber cables, on the other hand, encapsulate optical fibers within protective layers, making them easier to handle, reducing crosstalk between adjacent fibers, and preventing damage caused by rough surfaces. In addition to the advantages of optical transmission, confining light to the small core of the fiber has also spurred the development of fiber lasers and photonic crystal fibers.

Fundamental Knowledge of Optical Fibers

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Total Internal Reflection (TIR) and Numerical Aperture (NA)

As shown in Figure 1, light propagating from a medium with a higher refractive index (n₁) to a lower one (n₂) follows Snell’s law. When the angle of incidence exceeds the critical angle (θc), total internal reflection (TIR) occurs, confining light within the core. The critical angle can be calculated as:
𝜃𝑐=arcsin⁡(𝑛2𝑛1)

The Numerical Aperture (NA) of a fiber is defined as the sine of the maximum acceptance angle (α) that allows light to be guided by the core. NA reflects the light-gathering ability of the fiber and the ease of coupling light into it. The geometrical structure and material composition of a fiber determine the discrete electromagnetic modes or “fiber modes” that can propagate within it. Modes are categorized into:

  1. Radiation modes: Energy quickly dissipates from the core.
  2. Guided modes: Confined to the core, enabling energy transmission.

Single-mode propagation, often preferred for its Gaussian spatial distribution and minimal distortion, is possible when the core diameter is sufficiently small. The normalized frequency parameter (V-number) of a fiber indicates the number of modes that can propagate at a given wavelength.

Attenuation and Dispersion

Loss Mechanisms

As light propagates through the fiber, power diminishes exponentially due to attenuation, caused by:

  1. Absorption Loss: Predominantly due to impurities like hydroxyl ions (OH⁻).
  2. Scattering Loss: Results from microscopic irregularities in fiber structure.

Advances in fiber purity have reduced attenuation losses to as low as 0.1 dB/km.

Dispersion

Dispersion, which broadens light pulses over time, limits the data transmission rate and distance. Types of dispersion include:

  1. Intra-modal dispersion:
    • Chromatic dispersion: Caused by wavelength-dependent refractive index variations.
    • Polarization mode dispersion (PMD): Arises from birefringence effects.
  2. Inter-modal dispersion: Relevant to multi-mode fibers, caused by different propagation speeds of distinct modes.

basic physical knowledge about optical fiber 2

Dispersion compromises pulse clarity, as illustrated in Figure 2, where overlapping pulses obscure transmitted information.

Polarization and Special Fibers

Single-mode fibers support two orthogonal polarization modes. Random birefringence induced by external stresses disturbs polarization states. Special fibers, such as polarization-maintaining fibers (PMFs), introduce consistent birefringence along their length to maintain polarization. This is achieved by engineering fiber geometry and stress-inducing materials.basic physical knowledge about optical fiber 3

Polarization control in fibers operates similarly to free-space optical elements like wave plates. Figure 3 demonstrates stress-induced birefringence in fibers used to create wave plates or polarization devices like fiber squeezers. By applying pressure, linear birefringence is introduced, enabling precise control of light polarization.

Conclusion

Optical fibers, with their unique ability to guide light through precise internal reflection, are indispensable for modern communication and laser systems. Their design and physical properties continue to evolve, enabling advanced applications in telecommunications, laser technology, and beyond.