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US5216680A
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US
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Optical guided-mode resonance filter
Assignee: The University of Texas System
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Filing: 1991-07-11
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Granted: 1993-06-01
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Expires: 2011-07-11
Abstract
Abstract A guided-mode resonance filer is provided which can be used as an optical filter with very narrow line width and as an efficient optical switch. Diffraction efficiencies and passband frequencies are calculated based on guided-mode resonance properties of periodic dielectric structures in a waveguide geometry. The guided-mode resonance filter preferably includes means for changing various parameters within the grating so as to change passband frequencies in response thereto. Also, the present invention envisions a narrowband tuneable laser having a diffraction grating of the present invention placed within a laser cavity to provide narrowband optical wave output from the narrowband tuneable laser In another preferred embodiment, the present diffraction grating can be supported by a semiconductor substrate, preferably adjacent to a semiconductor laser for fine-tuning the output of the semiconductor laser. In still another preferred embodiment, the present diffraction grating can be placed between thin-film layers to enhance thin-film performance characteristics.
Inventors
- 👤 Robert Magnusson
- 👤 Shu-Shaw Wang
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-25 22:25
CPC Classifications
H; H01; H01S; H01S3/00; H01S3/10; H01S3/106; G; G02; G02B; G02B5/00; G02B5/18; G02B5/1828; G02B5/20; G02B5/203; H01S5/00; H01S5/10; H01S5/14; H01S5/141; G02F; G02F1/00; G02F1/01; G02F1/03; G02F1/0338; G02F2201/00; G02F2201/30; G02F2201/302; G02F2203/00; G02F2203/05; G02F2203/055; H01S3/105; H01S3/1055; H01S3/107; H01S5/02; H01S5/028; H01S5/12; H01S5/125
Claims Analysis
Total Claims: 26
Claim 1
Independent Claim
57 words
A guided-mode resonance filter, comprising: a grating having a plurality of variable parameters including thickness, periodic structure and permittivity of dielectric materials within said grating; an input wave directed at an angle of incidence upon said grating; and means for changing at least one said variable parameter to produce a tuned output wave from said input wave.
Claim 2
Dependent Claim
57 words
A guided-mode resonance filter, comprising: a grating having a plurality of variable parameters including thickness, periodic structure and permittivity of dielectric materials within said grating; an input wave directed at an angle of incidence upon said grating; and means for changing at least one said variable parameter to produce a tuned output wave from said input wave.
Claim 3
Dependent Claim
34 words
The filter as recited in claim 1, wherein said tuned output wave comprises said input wave diffracted from said grating, whereby said tuned output wave having a substantially high diffraction efficiency at select wavelengths.
Claim 4
Dependent Claim
25 words
The filter as recited in claim 1, wherein the permittivity within said grating is higher than the permittivity average value of regions surrounding said grating.
Claim 5
Dependent Claim
21 words
The filter as recited in claim 1, further comprising a support structure and a thermoelectric cooling means coupled to said grating.
Claim 6
Dependent Claim
42 words
The filter as recited in claim 4, wherein said support structure comprises a semiconductor of larger surface dimension than said grating, said semiconductor including a semiconductor laser means configured adjacent to said grating for providing said input wave incident upon said grating.
Claim 7
Dependent Claim
20 words
The filter as recited in claim 1, further comprising means for rotating said grating, whereby said angle of incidence changes.
Claim 8
Dependent Claim
36 words
The filter as recited in claim 1, further comprising a voltage supply connected across said grating to change said permittivity and selectively induce variations in said output wave depending upon a state of said voltage supply.
Claim 9
Dependent Claim
18 words
The filter as recited in claim 1, wherein said grating is placed between a pair of thin-film layers
Claim 10
Dependent Claim
20 words
The filter as recited in claim 8, wherein said thin-film layers are made of single or multiple homogenous dielectric materials.
Claim 11
Independent Claim
113 words
A method of producing a tuneable output wave, comprising the steps of: providing a planar, rotatable diffraction grating having a plurality of variable parameters including: thickness, a plurality of equi-distant periodic structures placed within said grating, and permittivity typical of dielectric materials in the visible and infrared spectral regions; directing an input wave possessing a characteristic wavelength spectrum upon a surface of said grating at an angle of incidence which varies depending upon a position of said rotatable diffraction grating; changing at least one said parameter for producing a tuneable output wave and redirecting said input wave incident upon said grating to produce said tuneable output wave in accordance with said changing step.
Claim 12
Independent Claim
113 words
A method of producing a tuneable output wave, comprising the steps of: providing a planar, rotatable diffraction grating having a plurality of variable parameters including: thickness, a plurality of equi-distant periodic structures placed within said grating, and permittivity typical of dielectric materials in the visible and infrared spectral regions; directing an input wave possessing a characteristic wavelength spectrum upon a surface of said grating at an angle of incidence which varies depending upon a position of said rotatable diffraction grating; changing at least one said parameter for producing a tuneable output wave and redirecting said input wave incident upon said grating to produce said tuneable output wave in accordance with said changing step.
Claim 13
Dependent Claim
21 words
The method as recited in claim 10, wherein said changing step comprises changing said thickness to produce said tuneable output wave.
Claim 14
Dependent Claim
25 words
The method as recited in claim 10, wherein said changing step comprises changing the spacing between said equi-distant structures to produce said tuneable output wave.
Claim 15
Dependent Claim
21 words
The method as recited in claim 10, wherein said changing step comprises changing said permittivity to produce said tuneable output wave.
Claim 16
Dependent Claim
23 words
The method as recited in claim 10, wherein said changing step comprises changing said angle of incidence to produce said tuneable output wave.
Claim 17
Dependent Claim
15 words
The method as recited in claim 10, wherein said diffraction grating comprises a photorefractive crystal.
Claim 18
Independent Claim
44 words
The method as recited in claim further comprising directing at least two laser beams incident upon a photofractive crystal to produce a grating of a changed spacing between the equidistant structures depending upon changing an angle of incidence of at least one laser beam.
Claim 19
Dependent Claim
35 words
The method as recited in claim 10, wherein said tuneable output wave includes at least one substantially narrow window of passband frequencies corresponding to wavelengths of said input waves having a substantially high diffraction efficiency.
Claim 20
Dependent Claim
34 words
The method as recited in claim 10, further comprising: applying voltage across said grating; and changing a digital magnitude output signal of said output wave in accordance with changing said voltage across said grating.
Claim 21
Independent Claim
171 words
A method of producing a narrowband tuneable laser, comprising the steps of: providing at least one partially transmissive concave mirror; providing a planar diffraction grating spaced apart from and facing the concave portion of said mirror, said grating having a plurality of variable parameters including thickness, spacing between a plurality of equi-distant structures within said grating, and a permittivity typical of dielectric materials in the visible and infrared spectral regions; providing an optical laser medium between said concave mirror and said grating; directing an input broadband optical wave from said laser medium upon said grating surface; backward diffracting said input broadband optical wave from said grating as an output narrowband optical wave in accordance with changing at least one said variable parameter; repeating said steps of directing and backward diffracting to continuously produce a tuned said output narrowband optical backward diffracted wave between said grating and said mirror; and transmitting a portion of said output narrowband optical wave through said partially transmissive concave mirror as output from said narrowband tuneable laser.
Claim 22
Independent Claim
171 words
A method of producing a narrowband tuneable laser, comprising the steps of: providing at least one partially transmissive concave mirror; providing a planar diffraction grating spaced apart from and facing the concave portion of said mirror, said grating having a plurality of variable parameters including thickness, spacing between a plurality of equi-distant structures within said grating, and a permittivity typical of dielectric materials in the visible and infrared spectral regions; providing an optical laser medium between said concave mirror and said grating; directing an input broadband optical wave from said laser medium upon said grating surface; backward diffracting said input broadband optical wave from said grating as an output narrowband optical wave in accordance with changing at least one said variable parameter; repeating said steps of directing and backward diffracting to continuously produce a tuned said output narrowband optical backward diffracted wave between said grating and said mirror; and transmitting a portion of said output narrowband optical wave through said partially transmissive concave mirror as output from said narrowband tuneable laser.
Claim 23
Dependent Claim
34 words
The method as recited in claim 19, wherein said backward diffracting step comprises selecting a specific grating thickness, permittivity and spacing between the equi-distant structures to produce a targeted narrowband set of output wavelengths.
Claim 24
Dependent Claim
26 words
The method as recited in claim 19, wherein said output wavelengths correspond to a set of wavelengths whose backward diffracted wave diffraction efficiency is substantially high.
Claim 25
Dependent Claim
15 words
The method as recited in claim 21, wherein said diffraction efficiency is greater than 0.8.
Claim 26
Dependent Claim
16 words
The method as recited in claim 19, wherein said optical laser medium includes a semiconductor laser.
References Cited (Backward Citations)
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