EP0167601A1 - Interferometrischer spektrometer mit diodennetz - Google Patents
Interferometrischer spektrometer mit diodennetzInfo
- Publication number
- EP0167601A1 EP0167601A1 EP85900572A EP85900572A EP0167601A1 EP 0167601 A1 EP0167601 A1 EP 0167601A1 EP 85900572 A EP85900572 A EP 85900572A EP 85900572 A EP85900572 A EP 85900572A EP 0167601 A1 EP0167601 A1 EP 0167601A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- radiation
- interference pattern
- mirror
- spectrometer
- forming
- 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.)
- Withdrawn
Links
- 230000005855 radiation Effects 0.000 claims description 29
- 238000001429 visible spectrum Methods 0.000 claims description 4
- 230000003068 static effect Effects 0.000 claims description 3
- 230000005670 electromagnetic radiation Effects 0.000 claims 3
- 238000002329 infrared spectrum Methods 0.000 claims 1
- 238000002211 ultraviolet spectrum Methods 0.000 claims 1
- 230000003287 optical effect Effects 0.000 abstract 1
- 238000001228 spectrum Methods 0.000 description 3
- 238000003491 array Methods 0.000 description 2
- 238000010276 construction Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000009977 dual effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000001914 filtration Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000000411 transmission spectrum Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/28—Investigating the spectrum
- G01J3/45—Interferometric spectrometry
- G01J3/453—Interferometric spectrometry by correlation of the amplitudes
- G01J3/4531—Devices without moving parts
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/28—Investigating the spectrum
- G01J3/2803—Investigating the spectrum using photoelectric array detector
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J9/00—Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength
- G01J9/02—Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength by interferometric methods
Definitions
- Interferometers take a variety of forms. They all depend upon the production of an interference pattern which is detected by a single element detector. In the case of a Michaelson interferometer, which can be used to measure visible spectra, ultra-violet, and infrared, the interference pattern is produced by varying the dis ⁇ tance that a portion of a split beam of light travels. In this type of interferometer, two plane mirrors are set perpendicular to each other with a beamsplitter positioned at 45 degrees between them. The beamsplitter is fabricated so that one-half of the light striking it is transmitted and one-half is reflected.
- Light to be analyzed enters the interferometer perpendicular to one of the mirrors.
- the beamsplitter transmits 50 percent of this light to one mirror and reflects 50 percent to the other mirror.
- the two light beams are reflected back to the beamsplitter by the mirrors, where the beams are recombined, and then exit perpendicular to their axis of entrance.
- Interference is produced by modifying the path lengths travelled by one of the two beams by moving one of the mirrors toward or away from the beamsplitter.
- the detector monitors the exiting radiation from such an interference pattern and the signal is recorded as a function of distance travelled by the moving mirror.
- the moving mirror must be kept exactly perpendicular to the fixed mirror throughout the scan. Usually special air bearings are required to accomplish this,
- Applicant's invention combines any one of a variety of means of creating a static interference pattern 15 with an array detector which can instantaneously measure an interference pattern over an area of two dimensions.
- Another object of this invention is to provide such an interferometer which may be used with a variety of devices to create an interference pattern.
- a source of radiation 10 is provided. Obviously, the radiation emanating from this source must be a type which is reflectable by mirrors so it would include the visible spectra, ultraviolet, and infrared. For purposes of illustration, three different rays of radiation from this source labeled 11, 12 and 13 are shown.
- Tilted mirror 17 is shown tilted but perpendicular to the same plane of the drawing as is the fixed mirror 16. It must be recognized that tilted mirror 17 may also be additionally tilted so that it is not perpendicular to the plane of the drawing and thus will produce a two-dimensional inter ⁇ ference pattern which may be read on a two-dimensional photodiode array detector.
- the photodiode array detector shown in this drawing is essentially in the single dimension of the plane of the drawing.
- ray 18 will have travelled a shorter distance than the other half of its ray 11 and when recombined rays 11 and 18 will create a signal of some intermediate intensity since these two rays will be out of phase.
- the thus recombined rays are transmitted through a focuss- ing lens 21 and displayed on the photodiode array detector
- photodiode array detectors having as many as 4,000 or more different detectors are used so that a great amount of different information can be obtained rapidly and much more inexpensively than would be obtained if the normal mirror of a Mi ⁇ haelson inferometer were moved backwards and forwards. If tilted mirror 17 is not positioned at right angles to the plane of the drawing and a two-dimensional photodiode array detector having a large area is employed, even more information may be obtained. Two-dimensional detectors are currently commercially available having 256 2 elements.
- the interference pattern generator described above may be replaced by a Young's double slit apparatus, a Lloyd's mirror, a Fresnel's biprism, and a Billet's split lens, all of which are described in The Theory of Light, by Thomas Preston, and published by MacMillan & Company, London, 1924, and all of which can generate interference patterns by suitable detection.
- the spectral range studied by the spectrometer can easily be altered by changing detector arrays provided a suitable interference pattern can be
- diode arrays sensitive to x-rays, are readily- available and an x-ray spectrometer of this invention would utilize Young's double slit apparatus with these x-ray detectors.
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- General Physics & Mathematics (AREA)
- Spectrometry And Color Measurement (AREA)
- Instruments For Measurement Of Length By Optical Means (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US57117584A | 1984-01-16 | 1984-01-16 | |
US571175 | 1984-01-16 |
Publications (1)
Publication Number | Publication Date |
---|---|
EP0167601A1 true EP0167601A1 (de) | 1986-01-15 |
Family
ID=24282615
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP85900572A Withdrawn EP0167601A1 (de) | 1984-01-16 | 1984-12-27 | Interferometrischer spektrometer mit diodennetz |
Country Status (3)
Country | Link |
---|---|
EP (1) | EP0167601A1 (de) |
JP (1) | JPS61500929A (de) |
WO (1) | WO1985003122A1 (de) |
Families Citing this family (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5495334A (en) * | 1990-07-26 | 1996-02-27 | Research Development Corporation Of Japan | Fourier transform spectroscope with quadrangular common path interferometer |
JP3292935B2 (ja) * | 1993-05-18 | 2002-06-17 | 富士写真フイルム株式会社 | 蛍光分光画像計測装置 |
DE4431412C1 (de) * | 1994-08-24 | 1996-03-14 | William Newton | Vorrichtung zur Durchführung spektroskopischer Messungen |
WO1997037200A1 (de) * | 1996-03-30 | 1997-10-09 | Michael Overhamm | Fourier-spektrometer |
DE19916072A1 (de) * | 1999-04-09 | 2000-10-26 | Campus Technologies Ag Zug | Vorrichtung und Verfahren zur optischen Spektroskopie |
DE10118760A1 (de) * | 2001-04-17 | 2002-10-31 | Med Laserzentrum Luebeck Gmbh | Verfahren zur Ermittlung der Laufzeitverteilung und Anordnung |
JP5317298B2 (ja) * | 2010-09-08 | 2013-10-16 | 国立大学法人 香川大学 | 分光計測装置及び分光計測方法 |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR1602535A (de) * | 1968-10-09 | 1970-12-21 | ||
US4173442A (en) * | 1977-05-27 | 1979-11-06 | The United States Of America As Represented By The Secretary Of Commerce | Apparatus and method for determination of wavelength |
-
1984
- 1984-12-27 JP JP60500455A patent/JPS61500929A/ja active Pending
- 1984-12-27 WO PCT/US1984/002134 patent/WO1985003122A1/en not_active Application Discontinuation
- 1984-12-27 EP EP85900572A patent/EP0167601A1/de not_active Withdrawn
Non-Patent Citations (1)
Title |
---|
See references of WO8503122A1 * |
Also Published As
Publication number | Publication date |
---|---|
JPS61500929A (ja) | 1986-05-08 |
WO1985003122A1 (en) | 1985-07-18 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
AK | Designated contracting states |
Designated state(s): BE CH DE FR GB LI NL SE |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
|
18D | Application deemed to be withdrawn |
Effective date: 19860321 |
|
RIN1 | Information on inventor provided before grant (corrected) |
Inventor name: WILLIAMS, RONALD, R. |