GB1333922A - Spatial filters - Google Patents
Spatial filtersInfo
- Publication number
- GB1333922A GB1333922A GB1333922DA GB1333922A GB 1333922 A GB1333922 A GB 1333922A GB 1333922D A GB1333922D A GB 1333922DA GB 1333922 A GB1333922 A GB 1333922A
- Authority
- GB
- United Kingdom
- Prior art keywords
- component
- recording
- amplitude
- plate
- produced
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/42—Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect
- G02B27/46—Systems using spatial filters
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Head (AREA)
- Diffracting Gratings Or Hologram Optical Elements (AREA)
Abstract
1333922 Spatial filters UNITED KINGDOM ATOMIC ENERGY AUTHORITY 19 April 1971 [18 March 1970] 13167/70 Heading G2J A spatial filter is produced by sequentially recording a first component and a second component on the same film or plate by two successive exposures, and developing the film or plate to give a gamma of approximately two, the first component being a diffaction pattern made from a transparency, and the second component being the interference pattern produced by combining the diffraction pattern with a further beam, the successive exposures at least approximately satisfying the relation # = E 1 /E i - E 1 /E 2 , the symbols being as defined in the Specification. The exposurerecording the second component is preferably made before the exposure recording the first component. The amplitude of the further beam is preferably large when compared with the amplitude of the diffraction pattern beam when recording the second component.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB1316770 | 1971-04-19 |
Publications (1)
Publication Number | Publication Date |
---|---|
GB1333922A true GB1333922A (en) | 1973-10-17 |
Family
ID=10018095
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB1333922D Expired GB1333922A (en) | 1971-04-19 | 1971-04-19 | Spatial filters |
Country Status (1)
Country | Link |
---|---|
GB (1) | GB1333922A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2472217A1 (en) * | 1979-12-21 | 1981-06-26 | Philips Nv | Holographic method for prodn. of inverse filter - using recording material with logarithmic characteristic and stipulated intensity ratio between reference and lens beams |
EP0114524A1 (en) * | 1982-12-27 | 1984-08-01 | The University Of Dayton | Production of high performance optical spatial filters |
-
1971
- 1971-04-19 GB GB1333922D patent/GB1333922A/en not_active Expired
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2472217A1 (en) * | 1979-12-21 | 1981-06-26 | Philips Nv | Holographic method for prodn. of inverse filter - using recording material with logarithmic characteristic and stipulated intensity ratio between reference and lens beams |
EP0114524A1 (en) * | 1982-12-27 | 1984-08-01 | The University Of Dayton | Production of high performance optical spatial filters |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PS | Patent sealed | ||
PLNP | Patent lapsed through nonpayment of renewal fees |