IP Library › Granted Patent US 12,405,168
Granted Patent B2
US 12,405,168 · App. 17/915,009 · Granted Sep 2, 2025

Phase difference measuring device, beam output apparatus and phase difference measuring method

Inventors: Koichi Hamamoto (Tokyo, JP); Tomoya Morioka (Tokyo, JP); Shingo Nishikata (Tokyo, JP); Hiroyuki Daigo (Tokyo, JP); Noriaki Miyanaga (Osaka, JP)
Assignees: MITSUBISHI HEAVY INDUSTRIES, LTD.; INSTITUTE FOR LASER TECHNOLOGY
G01J9/02G02B5/3083G02B5/32G01J2009/0261
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Quick Facts
Patent No.
US 12,405,168
App. No.
17/915,009
Granted
Sep 2, 2025
Kind
B2
Abstract

A phase difference measuring device is provided with a phase conversion device and a detection device. The phase conversion device converts a first laser beam that passes therethrough so that the first laser beam includes a phase distribution of one cycle in an azimuth direction in a cross section of the first laser beam included in an arbitrary virtual plane perpendicular to an optical axis of the first laser beam. The detection device detects an azimuth angle of an intensity centroid of an interference pattern generated by at least a part of a first laser beam that has passed through the phase conversion device, and a part of a second laser beam that derives from a laser beam as seed light from which the first laser beam derives, of which an optical intensity is same as the at least a part of the first laser beam, and detects an inter-beam phase difference of the second laser beam.

Claims (76)

1. Phase difference measuring device comprising:

a phase conversion device configured to convert a first laser beam that passes therethrough, so that the first laser beam includes a phase distribution of one cycle in an azimuth direction in a cross section of the first laser beam that has passed therethrough included in an arbitrary virtual plane perpendicular to an optical axis of the first laser beam; and

a detection device configured to detect an azimuth angle of an intensity centroid of an interference pattern and detect an inter-beam phase difference of a second laser beam with respect to the first laser beam based on the azimuth angle for a measurement of the inter-beam phase difference,

wherein the interference pattern is generated by a shaped detection beam in a cross section of a detection beam,

wherein the cross section of the shaped detection beam is a circle having a predetermined radius and having a center at a point, where the cross section of the detection beam and an extension line extended along an optical axis from an optical axis of the phase conversion device intersect,

wherein the cross section is perpendicular to an optical axis of the detection beam,

wherein a part outside the circle is masked,

wherein the detection beam is obtained by combining a first partial intensity laser beam and a second partial intensity laser beam on a same optical path,

wherein the first partial intensity laser beam has at least a part of an intensity component of the first laser beam that has passed through the phase conversion device, and

wherein the second partial intensity laser beam has at least a part of an intensity component of a second laser beam derived from a laser beam as seed light from which the first laser beam derives.

2. The phase difference measuring device according to claim 1 ,

wherein the detection device comprises:

a sensor device that has a plurality of sensors configured to detect optical intensity in each of a plurality of regions included in the interference pattern; and

a processor configured to calculate the azimuth angle of the optical intensity centroid of the interference pattern based on the optical intensity, and calculate the inter-beam phase difference based on the azimuth angle.

3. The phase difference measuring device according to claim 2 ,

wherein the sensor device comprises:

a four-quadrant detector that has four sensors configured to detect four optical intensities, respectively,

wherein the four optical intensities respectively correspond to four regions included in the interference pattern,

wherein the four regions are four quadrants defined by a cartesian coordinate system provided on a virtual plane perpendicular to the optical axis of the first laser beam.

4. The phase difference measuring device according to claim 1 , wherein the phase conversion device comprises a spiral phase plate configured to convert a wavefront of the first laser beam, that passes therethrough, into a spiral.

5. The phase difference measuring device according to claim 1 ,

wherein the phase conversion device comprises a hologram of a spiral phase plate configured to convert a wavefront of the first laser beam, that passes therethrough, into a spiral.

6. The phase difference measuring device according to claim 1 , wherein the phase conversion device comprises a multilevel spiral phase plate configured to convert a wavefront of the first laser beam, that passes therethrough, from a state with spatially-uniform-phase into a multilevel spiral state.

7. A beam output apparatus comprising:

a first beam splitter configured to split a laser beam configured to be seed light into a first laser beam and another laser beam from which a second laser beam derives;

a phase conversion device configured to convert the first laser beam that passes therethrough, so that the first laser beam that has passed therethrough includes a phase distribution of one cycle in an azimuth direction in a cross section of the first laser beam included in an arbitrary virtual plane perpendicular to an optical axis of the first laser beam that has passed therethrough;

a detection device configured to detect an azimuth angle of an intensity centroid of an interference pattern and detect an inter-beam phase difference of the second laser beam with respect to the first laser beam based on the azimuth angle; and

a phase controller configured to control a phase of the second laser beam based on the inter-beam phase difference,

wherein the interference pattern is generated by a shaped detection beam in a cross section of a detection beam,

wherein the cross section of the shaped detection beam is a circle having a predetermined radius and having a center at a point, where the cross section of the detection beam and an extension line extended along an optical axis from an optical axis of the phase conversion device intersect,

wherein the cross section is perpendicular to an optical axis of the detection beam,

wherein a part outside the circle is masked,

wherein the detection beam is obtained by combining a first partial intensity laser beam and a second partial intensity laser beam on a same optical path,

wherein the first partial intensity laser beam has at least a part of an intensity component of the first laser beam that has passed through the phase conversion device, and

wherein the second partial intensity laser beam has at least a part of an intensity component of a second laser beam.

8. The beam output apparatus according to claim 7 ,

wherein the detection device comprises:

a sensor device that has a plurality of sensors configured to detect optical intensity in each of a plurality of regions included in the interference pattern; and

a processor configured to calculate an azimuth angle of an optical intensity centroid of the interference pattern based on the optical intensity, and calculate an inter-beam phase difference based on the azimuth angle.

9. The beam output apparatus according to claim 8 ,

wherein the sensor device comprises:

a four-quadrant detector that has four sensors configured to respectively detect four optical intensities that respectively correspond to four regions included in the interference pattern,

wherein the four regions are four quadrants defined by a cartesian coordinate system provided on an arbitrary virtual plane perpendicular to the optical axis of the first laser beam.

10. The beam output apparatus according to claim 7 , wherein the phase conversion device comprises a spiral phase plate configured to convert a wavefront of the first laser beam, that passes therethrough, into a spiral.

11. The beam output apparatus according to claim 7 , wherein the phase conversion device comprises a hologram of a spiral phase plate configured to convert a wavefront of the first laser beam, that passes therethrough, into a spiral.

12. The beam output apparatus according to claim 7 , wherein the phase conversion device comprises a multilevel spiral phase plate configured to convert a wavefront of the first laser beam, that passes therethrough, into a spiral.

13. The beam output apparatus according to claim 7 , further comprising an amplifier configured to amplify the second laser beam.

14. The beam output apparatus according to claim 7 , further comprising:

a splitting device configured to split the second laser beam into a plurality of second split intensity laser beams, each of which has a part of intensity component of the second laser beam; and

a plurality of amplifiers configured to respectively amplify the plurality of second split intensity laser beams,

wherein the phase conversion device includes a plurality of phase conversion devices arranged so that a plurality of first partial cross section laser beams including parts of beam cross sections of the first laser beam, respectively pass therethrough,

wherein each of the plurality of phase conversion devices is configured to convert each of the plurality of first partial cross section laser beams that passes therethrough, so that each of the plurality of first partial cross section laser beams includes a phase distribution of one cycle in an azimuth direction in a cross section of each of the plurality of first partial cross section laser beams that has passed therethrough included in an arbitrary virtual plane perpendicular to an optical axis of each of the plurality of first partial cross section laser beams,

wherein the detection device is further configured to detect an azimuth angle of an intensity centroid of each of a plurality of interference patterns in a plurality of shaped detection beams and detect an inter-beam phase difference of each of a plurality of second partial intensity laser beams with respect to the plurality of first partial cross section laser beams based on the azimuth angle,

wherein the plurality of second partial intensity laser beams derive from the plurality of second split intensity laser beams, respectively,

wherein the plurality of shaped detection beams are each a circle having a predetermined radius and having a center at a point, where the cross section of the each detection beam and an extension line extended along an optical axis from an optical axis of the each phase conversion device intersect,

wherein the cross section is perpendicular to an optical axis of each of the plurality of detection beams,

wherein a part outside the circle is masked,

wherein the plurality of detection beams is obtained by combining the plurality of first partial cross section laser beams and the plurality of second partial intensity laser beams, respectively on same optical paths, and

wherein the phase controller is further configured to control a phase of each of the plurality of second partial intensity laser beams based on the each inter-beam phase difference.

15. The beam output apparatus according to claim 7 , further comprising:

a half-wave plate configured to convert a linear polarization direction of at least one of the first laser beam and the second laser beam;

another amplifier configured to amplify the first laser beam;

a polarizing beam splitter configured to combine the first laser beam and the second laser beam, each of which the linear polarization direction is different from each other, to generate a third laser beam;

a second beam splitter configured to split the third laser beam into a combined laser beam and a detection laser beam; and

a third beam splitter configured to split the detection laser beam into a first detection laser beam and a second detection laser beam,

wherein the detection device is further configured to detect an azimuth angle of an intensity centroid of an interference pattern generated by the first detection laser beam and the second detection laser beam.

16. A phase difference measuring method including:

converting a first laser beam that has passed through a phase conversion device, so that the first laser beam includes a phase distribution of one cycle in an azimuth direction in a cross section of the first laser beam included in an arbitrary virtual plane perpendicular to an optical axis of the first laser beam;

detecting an azimuth angle of an intensity centroid of an interference pattern; and

detecting an inter-beam phase difference of a second laser beam with respect to the first laser beam based on the azimuth angle, wherein the interference pattern is generated by a shaped detection beam in a cross section of a detection beam,

wherein the cross section of the shaped detection beam is a circle having a predetermined radius and having a center at a point, where the cross section of the detection beam and an extension line extended along an optical axis from an optical axis of the phase conversion device intersect,

wherein the cross section is perpendicular to an optical axis of the detection beam,

wherein a part outside the circle is masked,

wherein the detection beam is obtained by combining a first partial intensity laser beam and a second partial intensity laser beam on a same optical path,

wherein the first partial intensity laser beam has at least a part of an intensity component of the first laser beam that is converted, and

wherein the second partial intensity laser beam has at least a part of an intensity component of a second laser beam derived from a laser beam as seed light from which the first laser beam derives.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 27, 2022
From: HAMAMOTO, KOICHI; MORIOKA, TOMOYA; NISHIKATA, SHINGO; DAIGO, HIROYUKI; MIYANAGA, NORIAKI
To: MITSUBISHI HEAVY INDUSTRIES, LTD.; INSTITUTE FOR LASER TECHNOLOGY
Reel/Frame 061229/0743 →
Priority Claims (1)
JP 2020-061991 · Mar 31, 2020 · national
Continuity (1)
Related Publication 20230152163A1 · May 18, 2023
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