1. Field of the Invention
The present application relates to a novel manufacture method for a blazed concave grating, which can be widely applied to the fields such as optical spectrum instruments, and analysis and measurement, and belongs to the technical field of grating manufacture.
2. Related Arts
A holographic concave grating, which integrates dispersion, focusing and a flat field (where an important characteristic of the concave grating is imaging, and it is capable of imaging in a plane, and therefore, a CCD can be used as a receiving device), is a key element in a portable grating optical spectrum instrument and directly decides the final quality of the optical spectrum instrument. Due to the restriction of a geometric shape of a concave substrate, it is difficult, even impossible in many cases, to directly etch a concave grating by using ion beams. Consequently, a groove profile of the concave grating cannot be precisely controlled, and it has been difficult to improve the diffraction efficiency, leading to an application bottleneck of the concave grating.
For this problem, a common method at present is to directly manufacture a convex master grating by means of exposure and then obtain a concave grating by means of replication. Because flat-field concave gratings have uniform groove profiles, after being replicated by using the convex master grating, a flat-field concave grating only needs to be pulled along the vertical direction, to obtain a required concave gating. However, due to a blazed angle, if a blazed concave grating is also pulled along the vertical direction, the diffraction efficiency of the grating is greatly affected, and the application of the grating is limited.
In order to overcome the deficiency of an existing replication method, the present application provides a manufacture method for a blazed concave grating, which solves the problem of a big error in the existing replication method for a blazed concave grating.
Therefore, an original whole replication grating blank is divided into two blocks that are completely identical in size and shape, and after replication, the two blocks are separately pulled. Finally, the two blocks are spliced to obtain a required concave grating.
Preferably, the present application also has the following features:
In step A, a convex blazed master grating is formed by conducting sensitization, developing and ion beam etching on a convex blazed master grating substrate, where a working surface of the convex blazed master grating substrate is an optical surface and has been polished; in a preparation process, a working surface of the convex blazed master grating substrate is coated with a photosensitive material, namely, photoresist, in a rotating manner; the convex blazed master grating substrate is first subjected to holographic exposure, to obtain a convex photoresist mask grating, then developing is conducted on the convex photoresist mask grating to obtain a photoresist master grating, and finally ion beam etching is conducted on the developed photoresist master grating to obtain the convex blazed master grating.
A functional surface of the convex blazed master grating substrate is a plane, a spherical surface or an aspheric surface.
In step B, a surface type of the concave grating substrate is consistent with that of the working surface of the convex blazed master grating substrate, and the concave grating substrate can be divided into two blocks having an identical size and shape; a material of a segmentation sheet is a hard high-temperature steaming PE sealing film, of which a main component is polyethylene.
The segmentation sheet cannot be bonded to a silicone oil coating separation layer, a reflection coating, or an epoxy resin glue.
In step C, first, the segmentation sheet is vertically placed in the middle of the convex blazed master grating, the prepared convex blazed master grating is first plated with a layer of a thin and uniform silicone oil coating that serves as a separation layer, and then plated with a reflection coating; then, the convex blazed master grating after evaporation is placed on a platform in a drying oven, epoxy resin is poured onto the convex blazed master grating, and the concave grating substrate is pressed thereon; after leveling and bubble removal, the drying oven is heated to a suitable curing temperature, and after the epoxy resin is cured, the master grating is taken out from the drying oven.
In step E, two gratings have a spacing of B=0 in the vertical direction, and the two gratings have a spacing of S=Nd in the horizontal direction, that is, S is an integer multiple of a grating constant, where N is a positive integer, and d is a grating constant of a grating to be spliced.
The manufacture method for a blazed concave grating of the present application may avoid impact on the diffraction efficiency of a grating caused by pulling, thereby solving the problem of a big error in the existing replication method for a blazed concave grating.
In the figures:
The present application is further described below with reference to the accompanying drawings and embodiments, so that the technological concept to be protected by the present application can be more clearly understood.
A manufacture method for a blazed concave grating is described in this embodiment, which is specifically as follows:
1. First, a convex blazed master grating 1 is prepared. The prepared convex blazed master grating 1 is as shown in
2. A concave grating substrate 2 is prepared, as shown in
3. A segmentation sheet 4 is prepared. The segmentation sheet 4 can be used for segmentation. The segmentation sheet 4 cannot be bonded to a silicone oil coating separation layer, a reflection coating, or an epoxy resin glue. A material of the segmentation sheet is a hard high-temperature steaming PE sealing film, of which a main component is polyethylene. Segmentation is a main function of the segmentation sheet, and therefore, the segmentation sheet is very thin.
4. A concave grating is replicated, as shown in
5. The blazed concave gratings are separated, as shown in
6. The concave gratings are spliced, where a principle is as shown in
In order to ensure the overall diffraction efficiency of the gratings, high phase precision is required for the concave gratings. In order to ensure the consistency of phases between diffraction wave surfaces of the gratings to be spliced in the spliced grating, not only are all gratings to be spliced required to be coplanar (that is, B is equal to 0), but also a value of the following formula is required to be an integer multiple of 2π:
That is to say, not only B=0, but also S=Nd, that is, the spacing S is an integer multiple of a grating constant, where N is a positive integer, and d is a grating constant of the gratings to be spliced.
Therefore, the splicing and replication of the blazed concave gratings are completed.
For a person skilled in the art, various corresponding alterations and transformations can be made according to the technical solution and concept described above, and all such alterations and transformations shall fall within the protection scope of the claims of the present application.
Number | Date | Country | Kind |
---|---|---|---|
2013 1 0462037 | Sep 2013 | CN | national |
Number | Name | Date | Kind |
---|---|---|---|
20120156967 | Sukegawa et al. | Jun 2012 | A1 |
Number | Date | Country |
---|---|---|
101126825 | Feb 2008 | CN |
101246229 | Aug 2008 | CN |
103105638 | May 2013 | CN |
H0882551 | Mar 1996 | JP |
2012141647 | Jul 2012 | JP |
Entry |
---|
International Search Report of PCT/CN2013/087439 and its English translation, dated Jul. 3, 2014 (4 pages). |
Number | Date | Country | |
---|---|---|---|
20160131807 A1 | May 2016 | US |
Number | Date | Country | |
---|---|---|---|
Parent | PCT/CN2013/087439 | Nov 2013 | US |
Child | 14983334 | US |