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Passive Fiber Optics

This is part 1 of a tutorial on passive fiber optics from Dr. Paschotta. The tutorial has the following parts:

1:  Guiding light in a glass fiber
2:  Fiber modes
3:  Single-mode fibers
4:  Multimode fibers
5:  Fiber ends
6:  Fiber joints
7:  Propagation losses
8:  Fiber couplers and splitters
9:  Polarization issues
10:  Chromatic dispersion of fibers
11:  Nonlinearities of fibers
12:  Ultrashort pulses and signals in fibers
13:  Accessories and tools

Part 1: Guiding Light in a Glass Fiber

The basic function of any optical fiber is to guide light, i.e., to act as a dielectric waveguide: light injected into one end should stay guided in the fiber. In other words, it must be prevented from getting lost e.g. by reaching the outer surface and escaping there. We explain this here for glass fibers, but the operation principle of plastic optical fibers is the same.

In principle, the simplest solution for guiding light would be a homogeneous glass rod. (If it is thin enough, it can also be bent to some degree.) The outer surface can reflect light via total internal reflection. Due to the large refractive index contrast, this works for a considerable range of input beam angles, and in principle there don't need to be any power losses.

homogeneous glass fiber with total internal reflection
Figure 1: Total internal reflection can be used to guide light in a homogeneous fiber. Note that only partial reflection occurs at the end faces, where the angle of incidence is smaller.

However, this simple solution has some crucial disadvantages:

  • Due to the high index contrast, even tiny scratches of the glass on the outer surface could lead to substantial optical losses by scattering. Therefore, the outer surface would have to be made with high optical quality and well protected against damage and dirt. This problem can be mitigated only to some extent with some suitable buffer coating around the fiber; such coatings, not being highly homogeneous, can hardly provide very low optical losses.
  • Even if the fiber were pretty thin (e.g., with a diameter of 0.1 mm), it would support a huge number of modes (see part 2), which is bad e.g. when preserving a high beam quality is important.

One can, however, modify the idea of a very clean coating: use another glass region, having a slightly smaller refractive index than the core glass, as a cladding:

glass fiber with a cladding
Figure 2: A multimode glass fiber with a cladding, made of glass with a slightly lower refractive index.

Total internal reflection can occur at the glass/glass interface, but the incidence angles need to be larger.

That gives us several advantages:

  • Glass can be much more clean and homogeneous than a plastic buffer coating. That already reduces the losses.
  • Due to the reduced index contrast at the reflection points, small irregularities of the interface do not cause as serious optical losses as for a glass/air interface. Irregularities at the outer interface do not matter anymore, as the light cannot “see” them.
  • The guiding region – called the fiber core – can now be made much smaller than the total fiber, if this is wanted. One can adapt the core size e.g. to the size of some small light emitter.
  • With a combination of small core size and weak index contrast one can even obtain single-mode guidance (see below).

Note, however, that smaller index contrasts imply a smaller acceptance angle: total internal reflection can only occur if the incidence angle is above the critical angle. The maximum angle of incidence at the input face of the fiber is then determined by the numerical aperture (NA):

$${\rm{NA}} = n\;\sin {\theta _{{\rm{max}}}}$$

The NA is the sine of the maximum angle of incidence at the input face. In the equation, <$n_0$> is the refractive index of the medium around the fiber, which is close to 1 in the case of air.

Considering the Wave Nature of Light

The preceding considerations were based on a simple geometrical ray picture. Particularly in the domain of small cores and weak index contrasts, that simple picture does no more represent an accurate model for light propagation, as it ignores the wave nature of light. So let us now consider the wave nature.

First, we imagine at a Gaussian beam in a homogeneous medium (e.g., some glass). Even if such a beam has flat wavefronts initially, within one Rayleigh length it will start diverging significantly:

Gaussian beam
Figure 3: A Gaussian beam with 1.5 μm vacuum wavelength in a homogeneous glass. It initially propagates in a nearly parallel fashion, but eventually diverges.

The divergence is intimately related to a curvature of the wavefronts. Apparently, the wavefronts on the beam axis progress faster in <$z$> direction than those at higher or lower positions. That observation can trigger an idea: couldn't we work against that bending of wavefronts by somewhat slowing down the light near the beam axis? That could be done by using an inhomogeneous structure, with a somewhat increased refractive index in the central region. Indeed, this works quite well if we simply increase the core index by 0.014 within a radius of 3 μm:

Gaussian beam
Figure 4: A Gaussian beam injected into a step-index fiber structure.

The two horizontal gray lines indicate the position of the core/cladding interface. The beam propagation has been simulated with the RP Fiber Power software.

The numerical aperture is then 0.3. Nearly all light of the injected Gaussian beam is guided. An even lower index contrast would be sufficient for that purpose if we make the initial beam radius and the core region larger.

Note that the guiding of light works even if the fiber is not perfectly straight, but somewhat bent. If the bending is not too strong, bend losses (i.e., power losses induced by bending) are negligibly small.

Go to Part 2: Fiber Modes or back to the start page.


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