| CPC G02F 1/093 (2013.01) [H01F 7/02 (2013.01); H01F 7/0205 (2013.01); H01F 7/021 (2013.01)] | 4 Claims |
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1. A magneto-optic device comprising:
a Faraday rotator which includes a magnetic circuit including first to third magnets each provided with a through hole allowing light to pass through and a Faraday element disposed in the through hole in the magnetic circuit and made of a paramagnetic material capable of transmitting light;
a first optical component disposed at one end of the Faraday rotator in a direction of an optical axis; and
a second optical component disposed at the other end of the Faraday rotator in the direction of the optical axis,
light through the through hole in the magnetic circuit passing through the first optical component and the second optical component,
wherein the magnetic circuit is composed of the first to third magnets arranged coaxially in this order in a front-to-rear direction,
wherein when a direction of light passing through the through hole in the magnetic circuit is defined as the direction of the optical axis,
one of the first and third magnets is magnetized in a direction perpendicular to the direction of the optical axis to have a north pole located toward the through hole,
the other of the first and third magnets is magnetized in a direction perpendicular to the direction of the optical axis to have a south pole located toward the through hole,
the second magnet is magnetized in a direction parallel to the direction of the optical axis to have a north pole located toward the one of the first and third magnets having the north pole located toward the through hole,
wherein a distance from a center of the Faraday element to the first optical component along the direction of the optical axis is different from a distance from the center of the Faraday element to the second optical component along the direction of the optical axis, and
wherein the second optical component is disposed toward the third magnet in the direction of the optical axis, and a ratio L4/(L1+L2+L3) is in a range of not less than 0.2 and less than 0.5 where (L1+L2+L3) represents a sum of respective lengths of the first magnet, the second magnet, and the third magnet along the direction of the optical axis and L4 represents the distance from the center of the Faraday element to the second optical component along the direction of the optical axis.
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