发明授权
US5982806A Laser beam converter for converting a laser beam with a single
high-order transverse mode into a laser beam with a desired intensity
distribution and laser resonator for producing a laser beam with a
single high-order transverse mode
失效
用于将具有单个高阶横模的激光束转换为具有期望强度分布的激光束的激光束转换器和用于产生具有单个高阶横向模式的激光束的激光谐振器
- 专利标题: Laser beam converter for converting a laser beam with a single high-order transverse mode into a laser beam with a desired intensity distribution and laser resonator for producing a laser beam with a single high-order transverse mode
- 专利标题(中): 用于将具有单个高阶横模的激光束转换为具有期望强度分布的激光束的激光束转换器和用于产生具有单个高阶横向模式的激光束的激光谐振器
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申请号: US854096申请日: 1997-05-09
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公开(公告)号: US5982806A公开(公告)日: 1999-11-09
- 发明人: Satoshi Yamaguchi , Katsuhiro Minamida
- 申请人: Satoshi Yamaguchi , Katsuhiro Minamida
- 申请人地址: JPX Tokyo
- 专利权人: Nippon Steel Corporation
- 当前专利权人: Nippon Steel Corporation
- 当前专利权人地址: JPX Tokyo
- 优先权: JPX8-140746 19960510; JPX8-140747 19960510
- 主分类号: H01S3/00
- IPC分类号: H01S3/00 ; H01S3/10
摘要:
In order to obtain a high-power laser beam with a high beam quality with use of a small-sized and low-cost apparatus, there has been disclosed a laser resonator which is constructed so as to produce a single high-order transverse mode laser beam, and a technique for converting the laser beam with a single high-order transverse mode into a laser beam with a high beam quality. The laser resonator is provided with a regulating plate of a high-order transverse mode which is constructed so as to produce a laser beam in a single high-order transverse mode. A phase adjusting plate inverts a phase for each region of the laser beam divided depending upon a lateral mode thereof to match the phase for each region of the laser beam, and subsequently, a traveling direction of the laser beam is changed for each position thereof by means of the first binary optics element, and further, the laser beam is converted into a parallel beam by means of the second binary optical element. The first binary optics element changes the traveling direction of the ray of the laser beam for each region thereof so that the laser beam has a desired intensity distribution on the second binary optics element.
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