Polarization independent optical isolator
Provided is a polarization independent optical isolator including: wedge-shaped birefringent crystal plates each made of a LiNbO 3 single crystal; a Faraday rotator 3 made of a magnetic garnet single crystal; and sapphire single crystal plates 2 and 4 bonded to light transmitting surfaces of the Faraday rotator, respectively. A light transmitting surface of each of the sapphire single crystal plates is formed in such a manner as to be offset from the c-plane of the sapphire single crystal plate. An incident angle θa of imaginary light 300 on each of the sapphire single crystal plates, and an offset angles θoff of the light transmitting surface from the c-plane of each sapphire single crystal plates are set within predetermined ranges, the imaginary light 300 being represented by a bisector of an angle formed by optical axes of the ordinary ray and the extraordinary ray.
1. A polarization independent optical isolator comprising:
a pair of wedge-shaped birefringent crystal plates placed on an optical path;
a Faraday rotator which is placed, on the optical path, between the wedge-shaped birefringent crystal plates and which is made of a magnetic garnet single crystal;
collimator lenses which are placed, on the optical path, at positions outside the respective wedge-shaped birefringent crystal plates in relation to the Faraday rotator taken as a center; and
sapphire single crystal plates bonded to light transmitting surfaces of the Faraday rotator, respectively, wherein
the pair of wedge-shaped birefringent crystal plates are each made of a LiNbO 3 single crystal,
a light transmitting surface of each of the sapphire single crystal plates is formed in such a manner as to be parallel to a non-inclined light transmitting surface of a corresponding adjacent one of the wedge-shaped birefringent crystal plates, and to be offset from a c-plane of the sapphire single crystal plate, and
the polarization independent optical isolator is set to satisfy the following conditions:
an incident angle θa of imaginary light on each of the sapphire single crystal plate is 19.19 to 24.16 degrees, the imaginary light being represented by a bisector of an angle formed by optical axes of an ordinary ray and an,extraordinary ray separated by each of the wedge-shaped birefringent crystal plates;
an offset angle θ off of the light transmitting surface from the c-plane of each sapphire single crystal plate is 10.40 to 13.80 degrees; and
3 mm ≧f≧57.5/θa (mm), where f represents a focal length of each of the collimator lenses.
2. The polarization independent optical isolator according to claim 1 , wherein
optical fibers each having a cladding diameter of 125 μm are placed, on the optical path, at positions outside the respective collimator lenses in relation to the Faraday rotator taken as a center.
3. The polarization independent optical isolator according to claim 2 , which has a peak isolation characteristic of 40 dB or more.
4. The polarization independent optical isolator according to claim 3 , which is applied to an optical isolator for a fiber laser.
5. The polarization independent optical isolator according to claim 2 , which is applied to an optical isolator for a fiber laser.
6. The polarization independent optical isolator according to claim 1 , which has a peak isolation characteristic of 40 dB or more.
7. The polarization independent optical isolator according to claim 6 , which is applied to an optical isolator for a fiber laser.
8. The polarization independent optical isolator according to claim 1 , which is applied to an optical isolator for a fiber laser.