# US 4,398,806 A · Broadband variable optical attenuator

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- Number: US 4,398,806 A
- Document ID: US4398806A
- Status: Granted
- Kind: A
- Application number: 06/199,845
- Filed: 1980-10-23
- Granted: 1983-08-16
- Earliest claimed: 1980-10-23
- Assignees: The Board of Trustees of the Leland University
- Inventors: Keith E. Bennett; Robert L. Byer
- Web page: https://patentgrep.com/patent/US4398806A

## CPC

- G02B 6/266: {the optical element being an attenuator}
- G02B 26/02: for controlling the intensity of light {(G02B26/004 takes precedence)}
- G02B 27/281: {used for attenuating light intensity, e.g. comprising rotatable polarising elements}
- G02B: OPTICAL ELEMENTS, SYSTEMS OR APPARATUS

## Abstract

An optical variable attenuator includes first, second, third and fourth wedge shaped plates, each of said plates having two surfaces defined by an angle of convergence, the first and second plates being supported with two of said surfaces of said first and second plates being in spaced parallel alignment and with the angle of convergence of the two plates being in opposite directions, and the third and fourth plates being supported with two of said surfaces of said third and fourth plates being in spaced parallel alignment and with the angle of convergence of the third and fourth plates.

## Claims

### Claim 1

An optical variable attenuator comprising first and second wedge shaped plates, each of said plates having two surfaces defined by an angle of convergence, means for rotatably supporting said two plates with two of said surfaces of said plates being in spaced parallel alignment and with the angle of convergence of said two plates being in opposite directions, and means for rotatably positioning said two plates in an optical path with the axis of rotation of said two plates being perpendicular to the axis of said optical path.

### Claim 2 (depends on 1)

An optical variable attenuator as defined by claim 1 wherein said angles of convergence are equal.

### Claim 3 (depends on 2)

An optical variable attenuator as defined by claim 2 and further including third and fourth wedge shaped plates, each of said third and fourth plates having two surfaces defined by an angle of convergence, means for rotatably supporting said third and fourth plates with two of said surfaces of said third and fourth plates being in spaced parallel alignment and with the angle of convergence of said third and fourth plates being in opposite directions, and means for rotatably positioning said third and fourth plates in said optical path with the axis of rotation of said third and fourth plates being perpendicular to the axis of said optical path.

### Claim 4 (depends on 3)

An optical variable attenuator as defined by claim 3 wherein said angles of convergence of said third and fourth plates are equal to the angles of convergence of said first and second plates.

### Claim 5

An optical variable attenuator comprising a first set of first, second, third and fourth wedge shaped plates, each of said plates having two surfaces defined by an angle of convergence, means for rotatably supporting said first and second plates with two of said surfaces of said first and second plates being in spaced parallel alignment and with the angle of convergence of said two plates being in opposite directions, means for rotatably supporting said third and fourth plates with two of said surfaces of said third and fourth plates being in spaced parallel alignment and with the angle of convergence of said third and fourth plates being in opposite directions, and means for cooperatively rotating said first and second plates and said third and fourth plates in an optical path whereby a light beam passes through said attenuator with the incidence path in alignment with the exit path, the axis of rotation being perpendicular said light beam.

### Claim 6 (depends on 5)

An optical variable attenuator as defined by claim 5 and further including a second set of four wedged plates with axis of rotation rotated 90.degree. to the axis of the first set of four wedged plates such that the attenuation is independent of incident polarization, said second set being serially positioned with said first set.