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Fiber Optic Communication System

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The optical circulator has similar function and design as the optical isolator. An optical circulator is an nonreciprocal passive device that directs light sequentially from port 1 to port 2, from port 2 to port 3, and so on in only one direction. The operation of a circulator is similar to that of an isolator except its constructions is more complex. Like the isolator, its uses polarization to do its job.



The typical construction of an circulator consists of a number of walk-off polarizers, half-wave plates and Faraday rotators. Typically an optical ciruclator has three or four ports.

A variety of circulators are available commercially. They have low insertion loss, high isolation over a wide wavelength range, minimal polarization dependent loss, and low polarization mode dispersion.

The typical insertion loss of an isolator is about 0.6dB, channel isolation is over 40dB, optical return loss is over 50dB and polarization dependent loss is lower than 0.1dB.

The applications of optical ciruclators

In advanced optical communication systems, circulators are used for bi-directional transmissions, WDM networks, fiber amplifier systems, and for optical time domain reflectometer (OTDR) measurements.

Optical circulators are essential compoents of optical communication systems. They enable the routing of light from one optical fiber or waveguide to another based upon the direction of light propagation.

More information

Optical ciruculators extend the basic idea behind an optical isolator and add more functionality to the device. A circulator does not disgard the backward propagating light, as an isolator does, but directs it to another port, thus resulting in a three-port device in the simplest configuration. More ports can be added if one wants to redirect light coming from the third port to a fourth port. Even six ports circulators exist which direct light to different ports in a circular fashion depending on which port light enters.

You may guess that with the increasing of ports, the design becomes increasingly complex. You are absolutely correct on that guess. A second layer of complexity is added for polarization-independent circulators because they must split the incoming light from any port into its orthogonally polarized components and process each component separately.

In general, a circulator requires a large number of parts. The most important component in a polarization independent circulator is the beam displacer. Beam displacer is made from a strongly birefringent medium such that it displaces the orthogonally polarized components spatially by different amounts.

In spite of their complexity, optical circulators are available commercially in a relatively compact size with fiber pigtails on each end. Insertion losses are also very acceptable for such complex devices.

Optical circulators have found many applications in designing lightwave systems. A example could be a three-port circulator used with a fiber grating to realize a narrowband bandpass filter working in transmission. The circulator coverts the device into a transmission filter for all practical purposes.

Without a circulator, many applications have to be replaced by a 3dB fiber coupler which will introduce 3dB losses. The use of circulator allows to realize the same goal with less than -1dB insertion losses.
Fiber Optic Communication System
A fiber optic attenuator, also called an optical attenuator, simulates the loss the would be caused by a long length of fiber. Typically, this device performs receiver testing. While an optical attenuator can simulate the optical loss of a long length of fiber, it cannot accurately simulate the dispersion that would be caused by a long length of fiber.

Put it simply, for a fiber optic receiver, too much light can overload it and degrade the bit error ratio. In order to achieve the best bit error ratio (BER), the light power must be reduced. Fiber optic attenuators fit the requirement perfectly. This can happen when the transmitter delivers too much power such as when the transmitter is too close to the receiver.

What Is a Fiber Attenuator and How Does It Work?

Attenuators are like your sunglasses, which absorbs the extra light energy and protect your eyes from being dazzled. Attenuators typically have a working wavelength range in which they absorb the light energy equally.

An important characteristic of a good fiber attenuator is that they should not reflect the light, instead, they should absorb the extra light without being damaged. Since the light power used in fiber optic communications are fairly low, they usually can be absorbed without noticeable damage to the attenuator itself.

Types of Attenuators

Two types of fiber optic attenuators exist: fixed value attenuators and variable attenuators.

Fixed Value Attenuators

Fixed value attenuators have fixed values that are specified in decibels. Their applications include telecommunication networks, optical fiber test facility, Local Area Network(LAN) and CATV systems.

For example, a -3dB attenuator should reduce intensity of the output by 3 dB(50%).

Fixed value attenuator's attenuation value cannot be varied. The attenuation is expressed in dB. The operating wavelength for optical attenuators should be specified for the rated attenuation, because optical attenuation of a material varies with wavelength.

Fixed value attenuators are composed of two big groups: In-line type and connector type. In-line type looks like a plain fiber patch cable; it has a fiber cable terminated with two connectors which you can specify types.

Connector type attenuator looks like a bulk head fiber connector, it has a male end and a female end. It mates to regular connectors of the same type such as FC, ST, SC and LC.

Variable Attenuators

Variable attenuators come with many different designs. They are general used for testing and measurement, but they also have a wide usage in EDFAs for equalizing the light power among different channels.

One type of variable attenuator is built on a D-shaped fiber as a type of evanescent field device. If a bulk external material, whose refractive index is greater than the mode effective index, replaces a part of the evanescent field reachable cladding, the mode can become leaky and some of the optical power can be radiated. If the index of the external material can be changed with a controllable mean, through the effects such as thermo-optic, electro-optic, or acoustic-optic, a device with controllable attenuation is achievable.

Other types of variable attenuators include air gap, clip-on, 3-step and more.
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