Control of thickness of Fabry-Perot etalon - uses detection of peak light transmission of etalon when source coincides with Newton ring
The Fabry-Perot standard thickness control system forms a quasi point image at infinity from a light source. This image describes a geometric figure whose form is such that it cuts the localised Newtons ring system at infinity associated with the standard. The zone of the standard whose thickness is...
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Format | Patent |
Language | English French |
Published |
24.02.1978
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Subjects | |
Online Access | Get full text |
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Abstract | The Fabry-Perot standard thickness control system forms a quasi point image at infinity from a light source. This image describes a geometric figure whose form is such that it cuts the localised Newtons ring system at infinity associated with the standard. The zone of the standard whose thickness is to be controlled is illuminated by the light source at infinity. The light transmitted by the standard is detected. A peak intensity is detected when the source coincides with a Newton ring. From a knowledge of the instants of peak appearance one can calculate the fractional excess of the standard in the zone. This fractional excess is compared with a reference. An error signal is produced which is proportional to any difference. This error signal is applied to a control system which controls the thickness of the standard in the zone.
L'invention concerne l'asservissement de l'épaisseur d'un étalon Fabry-Pérot. Selon l'invention, on éclaire un étalon Fabry-Pérot par une source qui décrit une figure géométrique, notamment bicyclique, qui coupe les anneaux de Newton associés à l'étalon et on détecte l'intensité lumineuse transmise par l'étalon. On en déduit l'excédent fractionnaire de l'étalon, ce qui permet d'asservir l'épaisseur. Application en optique à la réalisation d'étalons à épaisseur contrôlée. |
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AbstractList | The Fabry-Perot standard thickness control system forms a quasi point image at infinity from a light source. This image describes a geometric figure whose form is such that it cuts the localised Newtons ring system at infinity associated with the standard. The zone of the standard whose thickness is to be controlled is illuminated by the light source at infinity. The light transmitted by the standard is detected. A peak intensity is detected when the source coincides with a Newton ring. From a knowledge of the instants of peak appearance one can calculate the fractional excess of the standard in the zone. This fractional excess is compared with a reference. An error signal is produced which is proportional to any difference. This error signal is applied to a control system which controls the thickness of the standard in the zone.
L'invention concerne l'asservissement de l'épaisseur d'un étalon Fabry-Pérot. Selon l'invention, on éclaire un étalon Fabry-Pérot par une source qui décrit une figure géométrique, notamment bicyclique, qui coupe les anneaux de Newton associés à l'étalon et on détecte l'intensité lumineuse transmise par l'étalon. On en déduit l'excédent fractionnaire de l'étalon, ce qui permet d'asservir l'épaisseur. Application en optique à la réalisation d'étalons à épaisseur contrôlée. |
Author | JACQUES MORET-BAILLY |
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Discipline | Medicine Chemistry Sciences Physics |
DocumentTitleAlternate | PROCEDE ET SYSTEME D'ASSERVISSEMENT DE L'EPAISSEUR D'UN ETALON DE FABRY-PEROT |
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Notes | Application Number: FR19760022742 |
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PublicationDate | 19780224 |
PublicationDateYYYYMMDD | 1978-02-24 |
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Snippet | The Fabry-Perot standard thickness control system forms a quasi point image at infinity from a light source. This image describes a geometric figure whose form... |
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SubjectTerms | COLORIMETRY CONTROLLING MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT,POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRA-RED,VISIBLE OR ULTRA-VIOLET LIGHT MEASURING PHYSICS RADIATION PYROMETRY REGULATING SYSTEMS FOR CONTROLLING OR REGULATING NON-ELECTRIC VARIABLES TESTING |
Title | Control of thickness of Fabry-Perot etalon - uses detection of peak light transmission of etalon when source coincides with Newton ring |
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