GB1309378A - Multi-frequency laser interferometers - Google Patents

Multi-frequency laser interferometers

Info

Publication number
GB1309378A
GB1309378A GB2797071A GB2797071A GB1309378A GB 1309378 A GB1309378 A GB 1309378A GB 2797071 A GB2797071 A GB 2797071A GB 2797071 A GB2797071 A GB 2797071A GB 1309378 A GB1309378 A GB 1309378A
Authority
GB
United Kingdom
Prior art keywords
beams
light
prism
laser
prisms
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
Application number
GB2797071A
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Norges Teknisk Naturvitenskapelige Forskningsrad
Original Assignee
Norges Teknisk Naturvitenskapelige Forskningsrad
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Norges Teknisk Naturvitenskapelige Forskningsrad filed Critical Norges Teknisk Naturvitenskapelige Forskningsrad
Publication of GB1309378A publication Critical patent/GB1309378A/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/08Construction or shape of optical resonators or components thereof
    • H01S3/081Construction or shape of optical resonators or components thereof comprising three or more reflectors
    • H01S3/083Ring lasers
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B9/00Measuring instruments characterised by the use of optical techniques
    • G01B9/02Interferometers
    • G01B9/02001Interferometers characterised by controlling or generating intrinsic radiation properties
    • G01B9/02007Two or more frequencies or sources used for interferometric measurement
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B2290/00Aspects of interferometers not specifically covered by any group under G01B9/02
    • G01B2290/45Multiple detectors for detecting interferometer signals

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • General Physics & Mathematics (AREA)
  • Instruments For Measurement Of Length By Optical Means (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Optical Transform (AREA)

Abstract

1309378 Interferometers NORGES TEKNISK-NATURVITENSKAPELIGE FORSKNINGSRAD 15 June 1971 [16 June 1970] 27970/71 Heading G2J [Also in Division G4] In an interferometer using as the light source a multi-frequency laser, to ensure that the contrast of at least one interference pattern is good, the sub-beams in one of the branches of the interferometer are made to travel over different length paths, since if the laser has a resonator of length L all frequencies except those for which half the wavelength is a fraction of the resonator length L are suppressed and consequently if light beams of adjacent frequencies are in phase after travelling a particular distance they are out of phase after travelling a further distance L. In one embodiment, Fig. 5 (not shown) a movable prism (P51) and a fixed prism (P52) each receiving one of the sub-beams from the laser via a mirror (S51) split the sub-beams into two light beams one of the light beams associated with the fixed prism additionally being transmitted to and reflected from a further mirror (S'51) so that it travels an additional distance L. After recombination the light is transmitted to two separate detectors (D51, D52 and D53, D54), good contrast always being obtained at one set. In the embodiment of Fig. 6 the light from the laser is split into two parallel light beams by mirrors S62 and S62', the beams then being directed towards semi-reflecting plane mirror S61. The resulting two reflected beams are transmitted to two fixed prisms P62, P62', at different distances from mirror S61. The transmitted beams are fed to movable prism P61 After reflection the recombined light beams are received by detector sets D61, D62, D63, D64. The two parallel light beams may alternately be derived using two pentagon prisms (S72, S'72) Fig.7a (not shown) or a plane parallel transparent plate (S72) Fig.7b (not shown) with a mirror on part of the side nearest the laser and a semi-reflecting mirror on part of the side furthest from the laser. In another embodiment, Fig. 8 (not shown) light emitted from both ends of the laser is divided by mirrors (S'83, S83 and S'82, S82) into two pairs of parallel beams which are transmitted to fixed pentagon prisms (P'82, P82) and a movable prism (P81) the reflected beams after recombination at the lowest (S81, S'81) being received by detectors (D81, D82, D83, D84). In another embodiment two parallel light beams (I, II) Fig.10c (not shown) with a suitable phase difference are derived by means of two mirrors (S'102, S102) and fed via a first prism (103) having a semi-reflecting coating (S101) on the hypotenuse to movable prism (P101) and fixed prism (P102) cemented to the first prism (103). The reflected light is detected by two sets of detectors. In another embodiment, Fig.11 (not shown) light beams (I, II) from the laser are transmitted to fixed prisms (P111, P112) having semireflecting coating on two of their sides so that the light beams are fed via movable mirrors (S111, S112, S113) back via the other prism (P112, P111) to four detectors. Further prisms (P113-P116) act as complementary prisms. This apparatus is suitable for measuring displacement in a drafting machine. In the embodiment of Fig.12a a fixed mirror arrangement S125-S128 receiving light beams I, II from a laser and co-operating with a beam splitter 120 results in light beams IT, IR, IIT, and IIR being fed by a second mirror assembly S121-S124 to a movable assembly 121 comprising two triangular prisms with a semi-reflecting common base surface, the resulting light being sensed by four detectors. The beam splitter P120 comprising two triangular prisms one half of the common base surface being semi-reflecting and one half being completely reflecting, Fig.12b (not shown). Additional prisms (P121, P122) provide for the return of light reflected from the semi-reflecting section of the base surface. In another embodiment, Fig.13a (not shown) the light from a polarizing laser is split by plane parallel plates (F132, F133) into phase displaced beams (IR, IT, IIR, IIT) which are reflected by a movable prism (P132) and a fixed prism (P131) onto a plate (F131) where the beams are recombined and detected by four detectors. A pair of detectors may be selected by either (1) comparing the contrasts in the two sets of interference patterns (2) switching from one detector set to another each time a predetermined number of patterns have been counted or (3) operating a switch each time the movable member moves past sensing elements at fixed positions.
GB2797071A 1970-06-16 1971-06-15 Multi-frequency laser interferometers Expired GB1309378A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
NO2327/70A NO125554B (en) 1970-06-16 1970-06-16

Publications (1)

Publication Number Publication Date
GB1309378A true GB1309378A (en) 1973-03-07

Family

ID=19878772

Family Applications (1)

Application Number Title Priority Date Filing Date
GB2797071A Expired GB1309378A (en) 1970-06-16 1971-06-15 Multi-frequency laser interferometers

Country Status (4)

Country Link
DE (1) DE2129899A1 (en)
GB (1) GB1309378A (en)
NO (1) NO125554B (en)
SE (1) SE379244B (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4702603A (en) * 1985-07-23 1987-10-27 Cmx Systems, Inc. Optical phase decoder for interferometers
DE102005038362A1 (en) * 2005-08-11 2007-02-15 Prüftechnik Dieter Busch AG Beam splitter for optical measuring systems for determining parameters on machine tools
CN108089217A (en) * 2017-11-15 2018-05-29 中国工程物理研究院激光聚变研究中心 X-ray detector based on Michelson's interferometer

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4702603A (en) * 1985-07-23 1987-10-27 Cmx Systems, Inc. Optical phase decoder for interferometers
DE102005038362A1 (en) * 2005-08-11 2007-02-15 Prüftechnik Dieter Busch AG Beam splitter for optical measuring systems for determining parameters on machine tools
US7714994B2 (en) 2005-08-11 2010-05-11 Prueftechnik Dieter Busch Ag Beam splitter for optical measurement systems for determining the characteristics of machine tools
CN108089217A (en) * 2017-11-15 2018-05-29 中国工程物理研究院激光聚变研究中心 X-ray detector based on Michelson's interferometer

Also Published As

Publication number Publication date
DE2129899A1 (en) 1971-12-23
SE379244B (en) 1975-09-29
NO125554B (en) 1972-09-25

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Legal Events

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