US4222668A
Expired / Lapsed
US
⏱️ 0.0 years remaining
Ferrimagnetic Faraday elements for ring lasers
Assignee: Boeing North American Inc
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Filing: 1978-02-23
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Granted: 1980-09-16
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Expires: 1998-02-23
Abstract
Abstract A ring laser having a Faraday cell for biasing the mode locking region beyond the range of rotation rates of interest. The Faraday element included in the cell is a composite comprising a monocrystalline thin film of a ferrimagnetic material epitaxially deposited on a non-magnetic single crystal substrate. An antireflection coating on the composite reduces reflections. Reflections are further reduced by the selection of thickness and index of refraction for the layers of the composite. Selected substituents are used in garnet layers to achieve desired magnetic properties, desired indices of refraction, and desired matching of the lattice parameter from layer to layer to minimize internal stresses. Where a composite is provided with a reflection coating on one side thereof, it is adapted to serve as an optical cavity forming corner reflector.
Inventors
- 👤 Rodney D. Henry
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-24 05:38
CPC Classifications
G; G02; G02F; G02F1/00; G02F1/01; G02F1/09; G01; G01C; G01C19/00; G01C19/58; G01C19/64; G01C19/66; G01C19/68
Claims Analysis
Total Claims: 22
Claim 1
Independent Claim
242 words
A ring laser comprising: an optical cavity formed as a closed path describing a ring; light amplifier means disposed in said optical cavity for producing at least two linearly polarized light beams counter-propagating around said ring; Faraday cell means for producing a relatively large frequency difference between said at least two light beams at relatively small rotation rates of said ring; said Faraday cell comprising: first and second quarter-wave plate means for changing the polarization of said at least two light beams from linear polarization to circular polarization where said at least two light beams are incident upon said Faraday cell and for changing the polarization of said at least two light beams from circular polarization to linear polarization where said at least two light beams exit from said Faraday cell; and thin film Faraday element means of ferrimagnetic material interposed between said first and second quarter-wave plate means for interacting with said at least two light beams wherein said ferrimagnetic material exhibits circular magnetic birefringence and thereby induces non-reciprocal phase shift in said at least two light beams; wherein said thin film Faraday element means comprises: a single crystal substrate of a non-magnetic material; and a thin monocrystalline film of said ferrimagnetic material epitaxially deposited on said substrate, wherein the optical thickness of said thin film of said ferrimagnetic material is any odd multiple of one-half of a wavelength of the light of said light beams propagating in said ferrimagnetic material.
Claim 2
Dependent Claim
242 words
A ring laser comprising: an optical cavity formed as a closed path describing a ring; light amplifier means disposed in said optical cavity for producing at least two linearly polarized light beams counter-propagating around said ring; Faraday cell means for producing a relatively large frequency difference between said at least two light beams at relatively small rotation rates of said ring; said Faraday cell comprising: first and second quarter-wave plate means for changing the polarization of said at least two light beams from linear polarization to circular polarization where said at least two light beams are incident upon said Faraday cell and for changing the polarization of said at least two light beams from circular polarization to linear polarization where said at least two light beams exit from said Faraday cell; and thin film Faraday element means of ferrimagnetic material interposed between said first and second quarter-wave plate means for interacting with said at least two light beams wherein said ferrimagnetic material exhibits circular magnetic birefringence and thereby induces non-reciprocal phase shift in said at least two light beams; wherein said thin film Faraday element means comprises: a single crystal substrate of a non-magnetic material; and a thin monocrystalline film of said ferrimagnetic material epitaxially deposited on said substrate, wherein the optical thickness of said thin film of said ferrimagnetic material is any odd multiple of one-half of a wavelength of the light of said light beams propagating in said ferrimagnetic material.
Claim 3
Dependent Claim
52 words
A ring laser as recited in claim 1 wherein said non-reciprocal phase shift induced in a clockwise propagating one of said at least two light beams is equal in magnitude and opposite in sign to said non-reciprocal phase shift induced in a counterclockwise propagating one of said at least two light beams.
Claim 4
Dependent Claim
22 words
A ring laser as recited in claim 2 wherein said ferrimagnetic material of said thin film Faraday element is a ferrimagnetic garnet.
Claim 5
Dependent Claim
22 words
A ring laser is recited in claim 3 wherein said ferrimagnetic garnet is a thin film of monocrystalline ferrimagnetic yttrium iron garnet.
Claim 6
Dependent Claim
40 words
A ring laser as recited in claim 4 wherein said ferrimagnetic yttrium iron garnet has a selected quantity of gallium substituted for iron therein to give said garnet a selected index of refraction and a selected relatively low saturation magnetization.
Claim 7
Dependent Claim
43 words
A ring laser as recited in claim 5 wherein said ferrimagnetic yttrium iron garnet has a selected quantity of an element selected from the group consisting of gadolinium, lanthanum, and bismuth substituted for yttrium therein to give said garnet a selected lattice parameter.
Claim 8
Dependent Claim
18 words
A ring laser as recited in claim 6 wherein said single crystal substrate is of a non-magnetic garnet.
Claim 9
Dependent Claim
30 words
A ring laser as recited in claim 7 wherein said lattice parameter selected for said ferrimagnetic yttrium iron garnet is selected to match the lattice parameter of said non-magnetic garnet.
Claim 10
Dependent Claim
16 words
A ring laser as recited in claim 8 wherein said non-magnetic garnet is gadolinium gallium garnet.
Claim 11
Dependent Claim
58 words
A ring laser as recited in claim 1 wherein said thin film Faraday element means is disposed in said optical cavity interposed between adjacent optical cavity forming corner reflectors of said cavity wherein each of said at least two light beams is transmitted through said thin film once for each passage of said light beams around said ring.
Claim 12
Dependent Claim
84 words
A ring laser as recited in claim 1 wherein said thin film Faraday element means comprises a cavity forming reflector disposed at a corner of said ring to receive light transmitted through said thin film of ferrimagnetic material and to reflect said light back through said thin film of ferrimagnetic material wherein each of said at least two light beams is transmitted through and reflected back through said thin film of ferrimagnetic material once for each passage of said light beams around said ring.
Claim 13
Dependent Claim
88 words
A ring laser as recited in claim 6 wherein said thin film Faraday element means comprises: said single crystal substrate of a non-magnetic garnet, a first thin film of monocrystalline paramagnetic yttrium iron garnet epitaxially deposited on a first surface of said substrate; said thin film of monocrystalline ferrimagnetic yttrium iron garnet epitaxially deposited on said first thin film of monocrystalline paramagnetic yttrium iron garnet; and a second thin film of monocrystalline paramagnetic yttrium iron garnet epitaxially deposited on said thin film of monocrystalline ferrimagnetic yttrium iron garnet.
Claim 14
Dependent Claim
44 words
A ring laser as recited in claim 12 wherein said first and second thin films of monocrystalline paramagnetic yttrium iron garnet each have a selected quantity of gallium substituted for iron therein to give said garnet a selected index of refraction and paramagnetic properites.
Claim 15
Dependent Claim
57 words
A ring laser as recited in claim 13 wherein said first thin film of monocrystalline paramagnetic yttrium iron garnet has a selected quantity of an element selected from the group consisting of gadolinium, lanthanum, and bismuth substituted for yttrium therein to give said garnet a lattice parameter matched to the lattice parameter of said non-magnetic garnet substrate.
Claim 16
Dependent Claim
16 words
A ring laser as recited in claim 14 wherein said non-magnetic garnet is gadolinium gallium garnet.
Claim 17
Dependent Claim
37 words
A ring laser as recited in claim 15 wherein said lattice parameter selected for said ferrimagnetic yttrium iron garnet is selected to match the lattice parameter of said first thin film of monocrystalline paramagnetic yttrium iron garnet.
Claim 18
Dependent Claim
62 words
A ring laser as recited in claim 16 wherein said second thin film of monocrystalline paramagnetic yttrium iron garnet has a selected quantity of an element selected from the group consisting of gadolinium, lanthanum, and bismuth substituted for yttrium therein to give said garnet a lattice parameter matched to the lattice parameter of said thin film of monocrystalline ferrimagnetic yttrium iron garnet.
Claim 19
Dependent Claim
54 words
A ring laser as recited in claim 17 wherein said first and second thin films of monocrystalline paramagnetic yttrium iron garnet each have an optical thickness substantially equal to an odd multiple of one-quarter of a wavelength of the light of said light beams propagating in said thin film of paramagnetic yttrium iron garnet.
Claim 20
Dependent Claim
60 words
A ring laser as recited in claim 2, wherein said Faraday element means further comprises an antireflection coating formed on each outer surface of said Faraday element means at which light enters said Faraday element, and wherein the optical thickness of said antireflection coating is any odd multiple of one-quarter of a wavelength of the light of said light beams.
Claim 21
Dependent Claim
16 words
A ring laser as recited in claim 9, wherein said antireflection coating is of magnesium fluoride.
Claim 22
Dependent Claim
16 words
A ring laser as recited in claim 18, wherein said antireflection coating is of magnesium fluoride.
References Cited (Backward Citations)
US3927946A
Cited
US3890047A
Cited
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1983-09-16 | 1984-03-17 | 1984-09-16 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1987-09-16 | 1988-03-17 | 1988-09-16 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1991-09-16 | 1992-03-17 | 1992-09-16 | $7700.00 | Window Closed / Lapsed |