An optical isolator is an optical component that allows the transmission of light in only one direction. It is typically used to prevent unwanted feedback into an optical oscillator, such as a laser cavity.
The function of the optical isolator is to let the light transmitted in the forward direction pass through and isolate the light transmitted in the reverse direction, so as to prevent the reflected light from affecting the stability of the system, similar to the function of a diode in an electronic device. Optical isolators are divided into two types according to polarization dependence: polarization-dependent type and polarization-independent type. The former is also called free space type (Free Space ) because there is no optical fiber input and output at both ends; the latter is also called in-line type ( In -Line) because there are optical fiber input and output at both ends. Free-space optical isolators are generally used in semiconductor lasers, because the light emitted by semiconductor lasers has extremely high linearity, so this polarization-dependent optical isolator can be used to enjoy the advantage of low cost; in communication lines or EDFAs, in-line optical isolators are generally used, because the optical polarization characteristics on the line are very unstable, requiring devices to have small polarization-dependent losses.
The basic principle used by the optical isolator is Malus’ law of polarized light and Faraday’s magneto-optical effect. The basic structure and principle of the free-space optical isolator are shown in the figure below. It consists of a magnetic ring, a Faraday optical rotator and two polarizers. Forward incident linearly polarized light, whose polarization direction is along the transmission axis direction of polarizer 1, rotates 45° counterclockwise to the transmission axis direction of polarizer 2 when passing through the Faraday rotator, and transmits smoothly; reversely incident linearly polarized light, whose polarization direction is along the transmission axis direction of polarizer 2, still rotates 45° counterclockwise to be perpendicular to the transmission axis of polarizer 1 when passing through the Faraday rotator, and is isolated without transmission light. The free-space optical isolator is relatively simple. When assembling, the polarizer and the optical rotator are tilted at a certain angle (such as 4°) to reduce the reflected light on the surface. Pay attention to the repeatability of the test when building the test structure.
The earliest online optical isolator was made of a combination of Displacer crystal and Faraday rotator, which was replaced by Wedge optical isolator due to its large size and high cost; online optical isolator introduced PMD due to the use of birefringent crystal, so PMD compensation type Wedge isolator appeared accordingly; some applications put forward higher requirements for isolation, so dual-stage optical isolators appeared to obtain higher isolation in a wider bandwidth.
The structure and principle of inline optical isolator.
1) Displacer type optical isolator
The structure and optical path of the displacer type optical isolator are shown in the figure below. It consists of two collimators, two Displacer crystals, a half-wave plate, a Faraday optical plate and a magnetic ring (not shown in the figure). The forward light is incident on the Displacer from the collimator 1 On 1, it is divided into o-light and e-light transmission, after passing through the half-wave plate and Faraday rotation plate, it rotates 45 +45 =90 counterclockwise, the conversion of o-light and e-light occurs, and passes through the Displacer 2 synthesize a beam and couple it into collimator 2; the reverse light is incident on Displacer2 from collimator 2, and is divided into o light and e light for transmission. After passing through the Faraday rotation plate and half-wave plate, it rotates counterclockwise by 45 -45 =0, no conversion of o light and e light occurs, and passes through Dis placer 1 The latter two beams are separated by deviation from the collimator 1.
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