Faraday rotator
A Faraday rotator excellent in productivity and also hardly causing an isolation function of an optical isolator to deteriorate even when the Faraday rotator is used in a high-power laser with a wavelength of 1.1 μm or less and an output of 1 W or more. The Faraday rotator comprises a non-magnetic garnet substrate; bismuth-substituted rare-earth iron garnet films grown respectively on both surfaces of the non-magnetic garnet substrate by a liquid phase epitaxial method; and sapphire crystal substrates bonded respectively to outer surfaces of the bismuth-substituted rare-earth iron garnet films, and configured to dissipate heat. The bismuth-substituted rare-earth iron garnet films has an absorption coefficient of 9 cm −1 or less for light at a wavelength of 1.06 μm, and that the bismuth-substituted rare-earth iron garnet films grown on the respective surfaces of the non-magnetic garnet substrate differ from each other in film thickness by 10 μm or less.
1. A Faraday rotator constituting a part of an optical isolator, the optical isolator comprising a light incident side and a light emission side, the Faraday rotator comprising:
a non-magnetic garnet substrate;
bismuth-substituted rare-earth iron garnet films grown respectively on both surfaces of the non-magnetic garnet substrate by a liquid phase epitaxial method; and
sapphire crystal substrates bonded respectively to outer surfaces of the bismuth-substituted rare-earth iron garnet films, and configured to dissipate heat, the Faraday rotator characterized in that
the bismuth-substituted rare-earth iron garnet films have an absorption coefficient of 9 cm −1 or less for light at a wavelength of 1.06 μm,
the bismuth-substituted rare-earth iron garnet films grown on the respective surfaces of the non-magnetic garnet substrate differ from each other, wherein a difference in film thickness is 10 μm or less, and
the bismuth-substituted rare-earth iron garnet film having the smaller film thickness is disposed at a light incident side of the optical isolator.
2. The Faraday rotator according to claim 1 , characterized in that the bismuth-substituted rare-earth iron garnet films grown on the respective surfaces of the non-magnetic garnet substrate differ from each other, wherein a difference in film thickness is 4 μm or less.
3. The Faraday rotator according to claim 1 , characterized in that a Faraday rotation angle is 45°±2° for the wavelength of light used.
4. The Faraday rotator according to claim 2 , characterized in that a Faraday rotation angle is 45°±2° for the wavelength of light used.