Crystal body, optical device having the same, and method of manufacturing crystal body

Patent metadata

Field	Value
Publication number	US-9910299-B2
Application number	US-201414780588-A
Country	US
Kind code	B2
Filing date	Oct 23, 2014
Priority date	Oct 23, 2013
Publication date	Mar 6, 2018
Grant date	Mar 6, 2018

Abstract

The present invention is a crystal body configured with a crystal and having a pair of light passing surfaces which face each other and pass light and at least one side surface which connects the pair of the light passing surfaces. In the crystal body according to the present invention, a ratio B/A of a dislocation density A (number/cm 2 ) in the light passing surfaces and a dislocation density B (number/cm 2 ) in the side surface satisfies the following general formula.

1≦( B/A )≦3600  (1)

First claim

The invention claimed is:

1. A crystal body configured with a crystal and having a pair of light passing surfaces which face each other and pass light and at least one side surface which connects the pair of the light passing surfaces,
wherein the crystal is a single crystal,
wherein the single crystal is a terbium scandium aluminum garnet-type single crystal, a terbium scandium lutetium aluminum garnet-type single crystal, a terbium gallium garnet-type single crystal, or a terbium aluminum garnet-type single crystal, and
wherein a ratio B/A of a dislocation density A (number/cm 2 ) in the light passing surfaces and a dislocation density B (number/cm 2 ) in the side surface satisfies the following general formula:
1≦( B/A )≦3600  (1).

2. The crystal body according to claim 1 , wherein the ratio (B/A) is in a range of 1 to 1000.

3. The crystal body according to claim 2 , wherein the ratio (B/A) is 1.

4. An optical device comprising the crystal body according to claim 1 .

5. The optical device according to claim 4 , further comprising:
a polarizer arranged to face the one light passing surface of the pair of the light passing surfaces of the crystal body;
an analyzer arranged to face the other light passing surface of the pair of the light passing surfaces of the crystal body; and
a magnetic field applying unit applying a magnetic field to the crystal body.

6. A method of manufacturing a crystal body configured with a crystal and having a pair of light passing surfaces which face each other and pass light and at least one side surface which connects the pair of the light passing surfaces, the method comprising:
a preparation process of preparing a workpiece material which is configured with the crystal and is used for obtaining the crystal body; and
a cutting process of obtaining the crystal body by cutting the workpiece material,
wherein, in the cutting process, the crystal body is formed by removing a surface layer portion including a cut face newly appearing by the cutting of the workpiece material,
wherein the crystal is a single crystal,
wherein the single crystal is a terbium scandium aluminum garnet-type single crystal, a terbium scandium lutetium aluminum garnet-type single crystal, a terbium gallium garnet-type single crystal, or a terbium aluminum garnet-type single crystal, and
wherein, in the cutting process, the surface layer portion includes dislocations, and the surface layer portion is removed so that a ratio B/A of a dislocation density A (number/cm 2 ) in the light passing surfaces and a dislocation density B (number/cm 2 ) in the side surface satisfies the following general formula:
1≦( B/A )≦3600  (1).

7. The method of manufacturing a crystal body according to claim 6 , wherein the dislocations included in the surface layer portion are dislocations caused from the cutting of the workpiece material or the grinding on the cut face.

8. The method of manufacturing a crystal body according to claim 6 , wherein the ratio (B/A) is in a range of 1 to 1000.

9. The method of manufacturing a crystal body according to claim 8 , wherein the ratio (B/A) is 1.

10. The method of manufacturing a crystal body according to claim 6 , wherein, in the cutting process, the surface layer portion is removed by polishing.

Assignees

• Fujikura Ltd

Inventors

• Kizaki Takeshi

Classifications

• C30B29/28 Primary

  with formula A3Me5O12 wherein A is a rare earth metal and Me is Fe, Ga, Sc, Cr, Co or Al, e.g. garnets · CPC title

• G02F1/09

  based on magneto-optical elements, e.g. exhibiting Faraday effect · CPC title

• G02B27/286

  for controlling or changing the state of polarisation, e.g. transforming one polarisation state into another (G02B5/3083 takes precedence; light guide coupling means utilising polarising elements G02B6/34) · CPC title

• G02F1/0136

  for the control of polarisation, e.g. state of polarisation [SOP] control, polarisation scrambling, TE-TM mode conversion or separation (G02F1/0353 takes precedence) · CPC title

• G02F1/0036 Primary

  Magneto-optical materials · CPC title