# US 5,706,086 A · System for measuring surface aberrations of concave cylindrical surfaces

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- Number: US 5,706,086 A
- Document ID: US5706086A
- Status: Granted
- Kind: A
- Application number: 08/608,103
- Filed: 1996-02-28
- Granted: 1998-01-06
- Earliest claimed: 1996-02-28
- Assignees: Hughes Aircraft Company
- Inventors: L. David LaFleur
- Web page: https://patentgrep.com/patent/US5706086A

## CPC

- G01M 11/0271: {by using interferometric methods}
- G01B 11/255: for measuring radius of curvature {(measuring diameter G01B11/08)}
- G01M 11/005: {Testing of reflective surfaces, e.g. mirrors}
- G01M: TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01B: MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS

## Abstract

An improved system (30) for measuring surface aberrations of concave cylindrical surfaces. In the illustrative embodiment, the invention includes a transmission flat (20), an interferometer (32), and a surface to be measured (28). The transmission flat (20) is a transparent disc that is placed between the interferometer (32) and the surface (28) to be measured. An electromagnetic wave (33,34,36,37) is generated by the interferometer (32), and is directed through the transmission flat (20). The wave (41) bounces off the surface (28) to be measured and is retro-reflected off a first surface (26) of the transmission flat. The electromagnetic wave (42) returns to the opposite side of the surface (28) under test. The wave (43) then bounces off the surface (28) under test and passes through the transmission flat (20). The wave (43) interferes with light (39) that is reflected from a reference surface (26) of transmission flat (20) on a first bounce. Information contained in the interference pattern is used by the interferometer (32) to construct an image representative of the surface (28) to be measured. In a specific embodiment, a non-transparent strip of material (22) is disposed across the center of the transmission flat (20). The strip (22) prevents skewed light reflected off the measured surface from entering the interferometer (32) on the first bounce from the surface (28) under test, and blurring the image of the surface (28). In the illustrative embodiment, the transmission flat (20) has a reference surface (26) that reflects a portion of the electromagnetic wave (38,39) back toward the interferometer (32). The reflected wave (38,39) provides a reference for interferometer (32) calculations.

## Claims

### Claim 1

A system for measuring surface aberrations comprising:
first means for generating a first wave of electromagnetic energy;
second means for extracting, from said first wave, second wave and third waves of electromagnetic energy, said second wave being a reference wave;
third means disposed on said second means for selectively blocking electromagnetic energy in said third wave;
fourth means for combining said reference wave and said selectively blocked third wave to provide an interference pattern; and
interferometer means for analyzing said interference pattern to identify aberrations in said surface.

### Claim 2 (depends on 1)

The invention of claim 1 wherein said first wave of electromagnetic energy is a collimated electromagnetic wavefront.

### Claim 3 (depends on 2)

The invention of claim 2 wherein said first wave of electromagnetic energy is generated by an interferometer.

### Claim 4 (depends on 2)

The invention of claim 2 wherein said first means includes an interferometer for generating said first wave.

### Claim 5 (depends on 1)

The invention of claim 1 wherein said second means includes a transmission flat having a first and second surface.

### Claim 6 (depends on 5)

The invention of claim 5 wherein said transmission flat is a transparent glass disc.

### Claim 7 (depends on 5)

The invention of claim 5 wherein said third means is disposed on said second surface of said transmission flat.

### Claim 8 (depends on 7)

The invention of claim 7 wherein second means includes said first surface of said strip with a surface to air interface for providing said second wave for interferometer calculations.

### Claim 9 (depends on 7)

The invention of claim 7 wherein said third means is a strip of non-transparent material for selectively blocking electromagnetic energy in said third wave that is not perpendicular to the transmission flat.

### Claim 10 (depends on 9)

The invention of claim 9 wherein said third means includes a surface facing said surface to be measured and having a refractive index equal to the refractive index of said transmission flat.

### Claim 11 (depends on 1)

The invention of claim 1 wherein said fourth means is an interferometer.

### Claim 12 (depends on 1)

The invention of claim 1 wherein said fourth means is a transmission flat.

### Claim 13 (depends on 1)

The invention of claim 1 wherein said interferometer means is an interferometer.

### Claim 14

An improved system for measuring surface aberrations of a surface comprising:
a transparent disc shaped transmission flat including a first surface to air interface for generating a reference wave for interferometer calculations;
an interferometer placed to one side of the transmission flat for directing a collimated electromagnetic wave beam through the transmission flat and reflecting a first portion of the beam off a surface to be measured and retro-reflecting a second portion of said beam off a reference surface of said transmission flat so that said first portion and said second portion of said beam interfere, creating an interference pattern representative of the surface to be measured; and
a strip of non-transparent material deposited across the center of said transmission flat for blocking a second portion of said electromagnetic wave beam from entering said interferometer and subsequently distorting said interference pattern.

### Claim 15

A technique for measuring the surface aberrations of cylindrical surfaces comprising the steps of:
painting a strip of opaque material across the center of a transmission flat;
directing a collimated electromagnetic wave beam through said transmission flat;
generating an interference pattern by reflecting a first portion of said wave beam off a surface to be measured and retro-reflecting a second portion of said wave beam off a reference surface of said transmission flat so that said first portion and said second portion of said wave interfere creating said interference pattern; and
constructing an image representative of said surface to be measured from said interference pattern using an interferometer.
