Optical Bit Error Rate

Chapter 2.6 - Matter

2.6   MATTER

The study of matter is extremely complex and almost impossible to be covered in a
section of a book. Matter may be in one of several phases; gaseous, plasma (or completely
ionized), liquid, and solid. For example, oxygen is typically a gas, but it is
also liquid at low temperatures. Water (H2O) is typically liquid, but at low temperatures
it is solid and at high temperatures it is a gas. Moreover, each element and
each compound exhibits different behavior and properties when in one of these
phases. Some matter allows most optical energy (most photons) to propagate
through it and it is called optically transparent (for example, glass or water). In Table 2.2


contrast, some dense matter absorbs (or scatters) light within the first few atomic
layers and it is called nonoptically transparent or opaque (for example, a sheet of
metal).

Some matter passes a portion of optical energy through it and absorbs part of it
(typically ~50%) and is called semitransparent (for example, most transparent matter,
semitransparent mirrors). Such matter attenuates the optical power of light and
may be used in optical devices known as optical attenuators.

Some matter allows selected frequencies to pass through and thus it is optically
transparent
to them; it absorbs all others. For example, red, green, yellow, or blue
glass each allow a selected range of frequencies to be propagated through it; the
Sun’s ionized surface or hot sulfur vapors absorb specific frequencies. Such matter
is called an optical filter.

Some matter permits rays with a certain polarization to propagate through it and
absorbs or reflects the others (for example, polarizing sunglasses). Such matter is
called a polarizing filter.

Some matter emits photons when in an intense electric field and some matter
emits photons of specific wavelengths when it is illuminated with light of shorter
wavelength (for example, most minerals under UV light; fluorescent substances, erbium,
etc.).

Some matter is homogeneously optically transparent; that is, it has the same
chemical, mechanical, electrical, magnetic, or crystallographic properties throughout
its volume and in all directions.

Some matter is heterogeneously optically transparent; that is, it does not have the
same chemical, mechanical, electrical, magnetic, or crystallographic properties
throughout its volume.

Some matter is isotropically optically transparent; that is, it has the same index
of refraction, polarization state, and propagation constant in every direction
throughout the material.

Some matter is anisotropically optically transparent; that is, it does not have the
same index of refraction, polarization state, and propagation constant in every direction
throughout the material. Anisotropy is explained as follows: the electrons of
certain crystals, such as calcite (CaCO3), move with different amounts of freedom
in selective directions in the crystal, and the dielectric constant as well as the refractive
index of the crystal is different in these selective directions. As a result, as photons
enter the crystal, their electromagnetic fields interact differently in one direction
than in another, and this affects their propagation pattern in the crystal.


2.6.1   Attributes of Matter


The attributes of matter and their significance of interest to optical communications
DWDM may be summarized as follows:

Refractive index (n)Is a function of molecular structure of matter
 
Is a function of optical frequency {n(ω)}
 Is a function of optical intensity
 Determines optical propagation properties of each λ
 May not be distributed equally in all directions
 Is affected by external temperature, pressure, and fields
  
Reflectivity (R)Is a function of geometry, λ, and n
 Material surface reflects optical power
 Changes polarization of incident optical wave
 Changes phase of incident optical wave
  
Transparency (T)Depends on matter consistency
  
ScatteringDue to molecular matrix disorders
  
Absorption (A)Due to the presence of ions in the molecular matrix and atomic
 excitation; ions act like dipoles, which exhibit eigenfrequencies and antenna characteristics (receiver/ transmitter)
  
Polarization (P)Due to X–Y uneven electromagnetic fields (light–matter interaction)
  
Birefringence (B)Due to nonuniform distribution of n in all directions
  
Phase shift (ΔΦ)Due to wave propagation property of light through matter

 

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