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US3319515A Expired / Lapsed US ⏱️ 0.0 years remaining

Interferometric optical phase discrimination apparatus

Assignee: EIDP Inc
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Filing: 1963-08-27
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Granted: 1967-05-16
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Expires: 1983-08-27
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Abstract

Abstract 1,024,598. Selective signalling. E. I. DU PONT DE NEMOURS & CO. Aug. 27, 1964 [Aug. 27, 1963], No. 35235/64. Heading G4H. [Also in Divisions G1 and G2] To determine the thickness of a travelling film 10<SP>1</SP> two beams of light reflected from the top and bottom faces of the film are made to constructively interfere by shortening the optical path of one beam by means of a reciprocating mirror 30<SP>1</SP>, the position of the mirror, and hence the instant in its cycle, at which interference takes place indicates the film thickness. The two beams are split by a 45-degree half-silvered mirror 32<SP>1</SP> on to the fixed mirror 311 and moving mirror 30<SP>1</SP>. At the position of the mirror 30<SP>1</SP> which compensates for the additional optical path in the film, light of one beam from the fixed mirror and light of the other beam from the moving mirror constructively interfere and initiate a pulse in the detecting circuit. The instant at which this occurs gives a measure of the thickness of the film. The timing of this interference is based upon a fixed reference pulse created during each cycle of the mirror when light from each beam individually constructively interferes. In the arrangement shown the moving mirror is offset so that the reference interference is not produced. The single pulse per cycle is superimposed upon an oscillator 70 input to a bistable multivibrator 79 and is centred upon it for the nominal thickness of the film, any time deviation by the pulse from the oscillator input indicates a change from the nominal thickness. In another arrangement (Fig. 6A, not shown) the reference pulse and the varying pulse are used to start and stop a clock-driven counter to give a measure of the thickness of the film. Instead of using a clock the counter pulses may be provided by using a source of monochromatic light to give a large number of constructive interferences per cycle of the mirror. In an alternative inferometer (Fig. 5, not shown) the additional optical path is changed by angularly moving the mirror. The main source of light delivers infra-red radiation for a lead sulphide photoresistor. (Refractive index and bi-refringence.may also be measured.)

Inventors

  • 👤 Philip A Flournoy

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-10-23 17:41
CPC Classifications
G; G01; G01B; G01B11/00; G01B11/02; G01B11/06; G01B11/0691; G01B9/00; G01B9/02; G01B9/02015; G01B9/02017; G01B9/02021; G01B9/02055; G01B9/02062; G01B9/02064; G01B9/02065; G01B9/0209; G01J; G01J3/00; G01J3/28; G01J3/45; G01J3/453; G01N; G01N21/00; G01N21/17; G01N21/41; G01N21/45; G02; G02F; G02F2/00; G02F2/002

Claims Analysis

Total Claims: 2
Claim 1
Independent Claim 128 words
A METHOD FOR DETERMINING A PHYSICAL PROPERTY OF A SPECIMEN ON THE BASIS OF INTERFEROMETRIC OPTICAL PHASE DISCRIMINATION COMPRISING, IN SEQUENCE, DIRECTING ANALYTICAL RADIATION UPON SAID SPECIMEN ALONG A COURSE SUCH THAT THERE IS DEVELOPED AN OPTICAL PHASE DIFFERENCE BETWEEN RADIATION EMANATING FROM A FIRST RADIATION-REFLECTIVE SURFACE OF SAID SPECIMEN AND FROM A SECOND RADIATIONREFLECTIVE SURFACE OF SAID SPECIMEN, CYCLICALLY VARYING AT A PREDETERMINED TIME RATE THE LENGTH OF THE PATH OF TRAVEL OF SAID RADIATION EMANATING FROM A GIVEN ONE OF THE PAIR CONSISTING OF SAID FIRST RADIATION-REFLECTIVE SURFACE OF SAID SPECIMEN AND SAID SECOND RADIATION-REFLECTIVE SURFACE OF SAID SPECIMEN, WITH RESPECT TO THE LENGTH OF THE PATH OF TRAVEL OF THE RADIATION EMANATING FROM THE OTHER OF SAID PAIR OVER A SPAN INCLUSIVE OF A ZERO-ORDER
Claim 2
Independent Claim 128 words
A METHOD FOR DETERMINING A PHYSICAL PROPERTY OF A SPECIMEN ON THE BASIS OF INTERFEROMETRIC OPTICAL PHASE DISCRIMINATION COMPRISING, IN SEQUENCE, DIRECTING ANALYTICAL RADIATION UPON SAID SPECIMEN ALONG A COURSE SUCH THAT THERE IS DEVELOPED AN OPTICAL PHASE DIFFERENCE BETWEEN RADIATION EMANATING FROM A FIRST RADIATION-REFLECTIVE SURFACE OF SAID SPECIMEN AND FROM A SECOND RADIATIONREFLECTIVE SURFACE OF SAID SPECIMEN, CYCLICALLY VARYING AT A PREDETERMINED TIME RATE THE LENGTH OF THE PATH OF TRAVEL OF SAID RADIATION EMANATING FROM A GIVEN ONE OF THE PAIR CONSISTING OF SAID FIRST RADIATION-REFLECTIVE SURFACE OF SAID SPECIMEN AND SAID SECOND RADIATION-REFLECTIVE SURFACE OF SAID SPECIMEN, WITH RESPECT TO THE LENGTH OF THE PATH OF TRAVEL OF THE RADIATION EMANATING FROM THE OTHER OF SAID PAIR OVER A SPAN INCLUSIVE OF A ZERO-ORDER

References Cited (Backward Citations)

US2518647A Cited
US3202052A Cited
US3238839A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1970-05-15 1970-11-14 1971-05-16 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1974-05-15 1974-11-14 1975-05-16 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 1978-05-15 1978-11-14 1979-05-16 $7700.00 Window Closed / Lapsed

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