An optical isolator is a device that is designed in such a way that it
allows the optical signal to travel in the forward direction along with blocking
reflections that would travel in the backward direction. In many applications
in optical systems, optical isolators are critically important. For example, to
external optical feedback, a single-frequency semiconductor laser is very
susceptive. To cause a significant increase in laser phase noise, intensity
noise, and wavelength instability even a very low level of optical reflection
from an external optical circuit, on the order of − 50 dB, is sufficient. Thus,
at the output of each laser diode, an optical isolator is needed in
applications needing low optical noise and optical frequency that is stable
single.
In sophisticated lightwave
systems, an optical isolator is used where one cannot allow light reflection
that might perturb the laser oscillator. However, to maintain system
performance one can introduce an optical isolator, but at times cost prevents
this.
On a Faraday rotator sandwiched
between two polarizers, a traditional optical isolator is based. In this
particular configuration, the optical signal that comes from the left side then
passes through the first polarizer whose optical switch is in the vertical direction, which matches the polarization
orientation of the input optical signal. Then, in a clockwise direction, the
polarization of the optical signal is rotated by a Faraday rotator by 45
degrees.
Concerning the first polarizer,
the optical axis of the second polarizer is oriented 45 degrees, which then
allows the optical signal to pass through with little attenuation. The
reflected optical signal has to pass through the Faraday rotator from right to
left only when there is a reflection from the optical circuit at the right
side. As the Faraday rotator is a nonreciprocal device so in the same direction
as the input signal, the polarization state of the reflected optical signal
will rotate for an additional 45 degrees, thus becoming horizontal, which is
perpendicular to the optical amplifier
of the first polarizer. In this way, the first polarizer effectively blocks the
reflected optical signal and the unidirectional transmission of the optical isolator is assured.
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