GB796661A - Optical arrangement for comparing the transmission ratio of a sample with a standard - Google Patents
Optical arrangement for comparing the transmission ratio of a sample with a standardInfo
- Publication number
- GB796661A GB796661A GB17004/56A GB1700456A GB796661A GB 796661 A GB796661 A GB 796661A GB 17004/56 A GB17004/56 A GB 17004/56A GB 1700456 A GB1700456 A GB 1700456A GB 796661 A GB796661 A GB 796661A
- Authority
- GB
- United Kingdom
- Prior art keywords
- comparison
- polarizer
- polarization
- interference
- transmission ratio
- 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
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/21—Polarisation-affecting properties
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
796,661. Optical apparatus. ZEISSSTIFTUNG. C.. [trading as JENAER GLASWERK SCHOTT & GEN.]. June 1, 1956 [June 2, 1955], No. 17004/56. Class 97(1) [Also in Group XL(b)] In apparatus for determining the light transmission ratio of a sample with respect to a standard, a beam of light is split into a measuring beam and a comparison beam and the beams recombined after passing through the sample and standard respectively by one or more interference polarizers. An optical device is used to determine the degree of polarization of the recombined beam, preferably by a null method. In a simple embodiment light from a source 10 passes through a condenser 11 and interchangeable filter 12 to an interference polarizer 13 provided with a deflecting prism. The resulting twin beams of polarized light are passed through the specimen 14 and standard 15 respectively and are then recombined by interference polarizer and prism 16. The photocell 18 associated with a suitable indicator views the final beam through analyzer 17. Comparison of the indications of photo-cell current when the analyzer is parallel and at right angles to the incidence plane of the polarizers may be used to determine the transmission ratio. Alternatively the analyzer may be rotated and the A.C. output of the cell measured. To convert this. embodiment to a null method a polarizer is placed in front of interference polarizer 13 and the angle through which it must be rotated to once again give zero output polarization on insertion of the specimen measured to give the transmission ratio. It is also possible to compensate the light beam energizing from the system to achieve zero polarization or to attenuate the comparison beam in a measurable manner for the same purpose. The system of Fig. 1 may be re-arranged so that the measuring and comparison beams are each transmitted at one interference polarizer and reflected at the other to give a symmetrical path arrangement. In this arrangement it is necessary to insert an optical element rotating the plane of polarization in each beam (Fig. 2, not shown). If a #/2 plate is used in the comparison beam for this it may be rotated to attenuate the beam to achieve zero output polarization as referred to above. The angle of rotation will be a function of the transmission ratio. In a further embodiment the paths followed by the measuring and comparison beams are again made symmetrical and the prisms associated with the interference polarizers so arranged that the measuring beam travels parallel to and to one side of a continuation of the axis of the initial light beam whilst the comparison beam travels parallel to and below it (Fig. 3A and B, not shown). As described a rotatable polarizer in the path of the comparison beam is used for obtaining an output of zero polarization. Fig. 4 shows an embodiment in which only one interference polarizer 40 is used and the beams pass through the specimen 41 and comparison member 42 twice because of the use of totally reflecting prisms 43 and 44. Elements 45 and 46 rotate the plane of polarization of the returning beams so that they pass out of the polarizer 40 towards the photo-cell. For the determination of the transmission ratio a rotatable analyzer 47 or any of the means previously described may be used. If modifications are made to the apparatus of Fig. 4 it can be arranged for measuring the reflection coefficient, the proportion of light reflected and transmitted, or the dispersion losses, in a specimen. As described with reference to Fig. 5 (not shown) this may be done by replacing the prisms 43 and 44 by a mirror and placing the specimen under test in the path of the measuring beam. The interference polarizers used, if they have a layer of uniform thickness, only operate within a limited frequency band and it may be necessary to combine a plurality of optical devices having different layer thicknesses in one polarizer if it is necessary to work with a wide frequency band. Specification 768,727 is referred to.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE796661X | 1955-06-02 |
Publications (1)
Publication Number | Publication Date |
---|---|
GB796661A true GB796661A (en) | 1958-06-18 |
Family
ID=6710997
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB17004/56A Expired GB796661A (en) | 1955-06-02 | 1956-06-01 | Optical arrangement for comparing the transmission ratio of a sample with a standard |
Country Status (1)
Country | Link |
---|---|
GB (1) | GB796661A (en) |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3146294A (en) * | 1959-02-13 | 1964-08-25 | American Optical Corp | Interference microscope optical systems |
US4120592A (en) * | 1976-03-24 | 1978-10-17 | E. I. Du Pont De Nemours And Company | Multiplex optical analyzer apparatus |
WO1984000213A1 (en) * | 1982-06-29 | 1984-01-19 | Labsystems Oy | Method for the measurement of the difference in the optical properties of two samples |
US4469443A (en) * | 1982-06-01 | 1984-09-04 | The United States Of America As Represented By The Secretary Of The Navy | Atmospheric transmissometer |
CN106483071A (en) * | 2016-12-30 | 2017-03-08 | 郑州光力科技股份有限公司 | A kind of gas detector and its absorption cell |
-
1956
- 1956-06-01 GB GB17004/56A patent/GB796661A/en not_active Expired
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3146294A (en) * | 1959-02-13 | 1964-08-25 | American Optical Corp | Interference microscope optical systems |
US4120592A (en) * | 1976-03-24 | 1978-10-17 | E. I. Du Pont De Nemours And Company | Multiplex optical analyzer apparatus |
US4469443A (en) * | 1982-06-01 | 1984-09-04 | The United States Of America As Represented By The Secretary Of The Navy | Atmospheric transmissometer |
WO1984000213A1 (en) * | 1982-06-29 | 1984-01-19 | Labsystems Oy | Method for the measurement of the difference in the optical properties of two samples |
CN106483071A (en) * | 2016-12-30 | 2017-03-08 | 郑州光力科技股份有限公司 | A kind of gas detector and its absorption cell |
CN106483071B (en) * | 2016-12-30 | 2023-08-22 | 光力科技股份有限公司 | Gas detector and absorption tank thereof |
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