发明授权
US5677783A Method of making a deformable grating apparatus for modulating a light
beam and including means for obviating stiction between grating
elements and underlying substrate
失效
制造用于调制光束的可变形光栅装置的方法,并且包括用于消除光栅元件和下面的衬底之间的静电的装置
- 专利标题: Method of making a deformable grating apparatus for modulating a light beam and including means for obviating stiction between grating elements and underlying substrate
- 专利标题(中): 制造用于调制光束的可变形光栅装置的方法,并且包括用于消除光栅元件和下面的衬底之间的静电的装置
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申请号: US404139申请日: 1995-03-13
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公开(公告)号: US5677783A公开(公告)日: 1997-10-14
- 发明人: David M. Bloom , Francisco S. A. Sandejas , Olav Solgaard , Raj B. Apte
- 申请人: David M. Bloom , Francisco S. A. Sandejas , Olav Solgaard , Raj B. Apte
- 申请人地址: CA Stanford
- 专利权人: The Board of Trustees of the Leland Stanford, Junior University
- 当前专利权人: The Board of Trustees of the Leland Stanford, Junior University
- 当前专利权人地址: CA Stanford
- 主分类号: B81B3/00
- IPC分类号: B81B3/00 ; G02B5/18 ; G02B26/08
摘要:
A modulator for modulating incident rays of light, the modulator comprising a plurality of equally spaced apart beam elements, each of which includes a light reflective planar surface. The elements are arranged parallel to each other with their light reflective surfaces parallel to each other. The modulator includes means for supporting the beam elements in relation to one another and means for moving the beam elements relative to one another so that the beams move between a first configuration wherein the modulator acts to reflect the incident rays of light as a plane mirror, and a second configuration wherein the modulator diffracts the incident rays of light as they are reflected therefrom. In operation, the light reflective surfaces of the beam elements remain parallel to each other in both the first and the second configurations and the perpendicular spacing between the reflective surfaces of adjacent beam elements is equal to m/4 times the wavelength of the incident rays of light, wherein m=an even whole number or zero when the beam elements are in the first configuration and m=an odd number when the beam elements are in the second configuration.
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