Patent US4826295A successfully refreshed from Google Patents.
US4826295A
Expired / Lapsed
US
⏱️ 0.0 years remaining
Controlled Optical signal absorber apparatus and method using quantum well layer structure
Assignee: British Telecommunications PLC
•
Filing: 1984-11-21
•
Granted: 1989-05-02
•
Expires: 2004-11-21
Abstract
Abstract An optical device having controllable absorption for an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 ev comprises (i) a semiconductor structure including one or more quantum well layers and (ii) means adapted for applying to the quantum well layers(s) an electric field such that the component of the field normal to the layer(s) may be controlled so as to determine the absorption edge of the quantum well layer(s) to be on either side of the optical signal wavelength. The device may be used as an optical modulator or switch and in optical demultiplexing.
Inventors
- 👤 Michael G. Burt
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-29 09:52
CPC Classifications
B; B82; B82Y; B82Y20/00; G; G02; G02F; G02F1/00; G02F1/01; G02F1/015; G02F1/017
Claims Analysis
Total Claims: 29
Claim 1
Independent Claim
111 words
An optical device having controllable absorption for an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 eV, which comprises: (i) a semiconductor structure including at least one quantum well layer; (ii) means for applying to the quantum well layer an electric field having a component of the field normal to the layer which may be controlled so as to determine the absorption edge of the quantum well layer to be on either side of the optical signal wavelength; and optical signal input and output ports arranged to cause the propagation of the optical signal through the quantum well layer in a direction parallel to said layer.
Claim 2
Dependent Claim
111 words
An optical device having controllable absorption for an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 eV, which comprises: (i) a semiconductor structure including at least one quantum well layer; (ii) means for applying to the quantum well layer an electric field having a component of the field normal to the layer which may be controlled so as to determine the absorption edge of the quantum well layer to be on either side of the optical signal wavelength; and optical signal input and output ports arranged to cause the propagation of the optical signal through the quantum well layer in a direction parallel to said layer.
Claim 3
Dependent Claim
26 words
An optical device accroding to claim 1, wherein the said component of the elctric field is controllable over a range of at least 10 3 volt/cm.
Claim 4
Dependent Claim
25 words
An optical device according to claim 2, wherein the said component of the electric field is controllable over range of at least 10 4 volt/cm.
Claim 5
Dependent Claim
27 words
An optical device according to any one of claims 1 to 3 having additionally means for sweeping out carriers generated by absorption in the quantum well layers.
Claim 6
Dependent Claim
22 words
An optical device according to any one of claims 1 to 3, wherein the said photon energy does not exceed 1.0 ev.
Claim 7
Dependent Claim
50 words
A combined optical source and modulator comprising (a) a source adapted to produce light having a source wavelength corresponding to a photon energy not exceeding 1.2 eV and (b) a device according to claim 1 having variable absorption for the source wavelength, the source and the device being optically coupled.
Claim 8
Dependent Claim
23 words
A combined optical source and modulator according to claim 6, wherein the source wavelength corresponds to a photon energy not exceeding 1.0 eV.
Claim 9
Dependent Claim
17 words
A combined optical source and modulator according to claim 6, wherein the source is a semiconductor laser.
Claim 10
Dependent Claim
23 words
A combined optical source and modulator according to claim 6 wherein the source is a semiconductor source and is integrated with the device.
Claim 11
Dependent Claim
24 words
An optical demultiplexer comprising two or more devices each according to claim 1 with optical connection between the quantum well layer of sequential devices.
Claim 12
Dependent Claim
8 words
An integrated optical demultiplexer according to claim 10.
Claim 13
Independent Claim
81 words
A method of modulating or switching an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 eV which comprises: introducing the optical signal into at least one semiconductor quantum well layer so as to propagate in the plane of said layer and modulating a component of an eIectric field disposed normal to the quantum well layer so as to move the absorption edge of the quantum well layer between positions to either side of the signal wavelength.
Claim 14
Independent Claim
81 words
A method of modulating or switching an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 eV which comprises: introducing the optical signal into at least one semiconductor quantum well layer so as to propagate in the plane of said layer and modulating a component of an eIectric field disposed normal to the quantum well layer so as to move the absorption edge of the quantum well layer between positions to either side of the signal wavelength.
Claim 15
Dependent Claim
25 words
A method according to claim 12, wherein the said component of the electric field is varied over a range of at least 10 3 volt/cm.
Claim 16
Dependent Claim
25 words
A method according to claim 13, wherein the said component of the electric field is varied over a range of at least 10 4 volt/cm.
Claim 17
Independent Claim
21 words
A method according to any one of claims 12 to 14 wherein the said photon energy does not exceed 1.0 eV.
Claim 18
Independent Claim
142 words
A method of time demultiplexing an optical signal corresponding to a photon energy not exceeding 1.2eV which comprises applying respectively different time-varying electric fields to successive multiple quantum well layer devices, each having semiconductor quantum well layer with a low conductance-valence energy band gap located between interleaved layers having a substantially higher conductance-valence energy band gap encompassing and bracketing said low energy band gap so as to provide quantum well confinement of both electrons and holes in each quantum well layer, said devices being optically coupled for passage of an optical signal propagating within said multiple quantum well layers and parallel to the plane of said quantum well layers while said electric field are oriented perpendicular to said quantum well layers so as to move the absorption edge of the quantum well layers between positions to either side fo the signal wavelength.
Claim 19
Independent Claim
142 words
A method of time demultiplexing an optical signal corresponding to a photon energy not exceeding 1.2eV which comprises applying respectively different time-varying electric fields to successive multiple quantum well layer devices, each having semiconductor quantum well layer with a low conductance-valence energy band gap located between interleaved layers having a substantially higher conductance-valence energy band gap encompassing and bracketing said low energy band gap so as to provide quantum well confinement of both electrons and holes in each quantum well layer, said devices being optically coupled for passage of an optical signal propagating within said multiple quantum well layers and parallel to the plane of said quantum well layers while said electric field are oriented perpendicular to said quantum well layers so as to move the absorption edge of the quantum well layers between positions to either side fo the signal wavelength.
Claim 20
Independent Claim
116 words
A method of frequency demultiplexing an optical signal corresponding to photon energy not exceeding 1.2eV which comprises applying respectively different but constant electric fields to the multiple quantum well layers of successive quantum well layer devices, each having semiconductor quantum well layers with a low conductance-valence energy band gap located between interleaved layers having a substantially higher conductance-valance energy band gap encompassing and bracketing said low energy band gap so as to provide quantum well confinement of both electrons and holes in each quantum well layer, said devices being optically coupled for passage of an optical signal propagating within said multiple quantum well layers while said electric fields are oriented perpendicular to said quantum well layers.
Claim 21
Independent Claim
116 words
A method of frequency demultiplexing an optical signal corresponding to photon energy not exceeding 1.2eV which comprises applying respectively different but constant electric fields to the multiple quantum well layers of successive quantum well layer devices, each having semiconductor quantum well layers with a low conductance-valence energy band gap located between interleaved layers having a substantially higher conductance-valance energy band gap encompassing and bracketing said low energy band gap so as to provide quantum well confinement of both electrons and holes in each quantum well layer, said devices being optically coupled for passage of an optical signal propagating within said multiple quantum well layers while said electric fields are oriented perpendicular to said quantum well layers.
Claim 22
Dependent Claim
159 words
An optical device having controllable absorption for an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 eV and not based upon use of the Stark effect on excitons, which device comprises: (i) a semiconductor structure including multiple quantum well layers; (ii) means for applying to the quantum well layers an electric field having a component of the field normal to the layers which may be controlled so as to determine the absorption edge of the quantum well layers to be on either side of the optical signal wavelength for optical signals propagating through the quantum well layers in a direction parallel to said layers, said optical signal having an electric vector disposed parallel to said layers; and (iii) optical signal input and output ports arranged to cause the propagation of the optical signal, having an electric vector disposed parallel to the layers, through the quantum well layers in a direction parallel to said layers.
Claim 23
Dependent Claim
159 words
An optical device having controllable absorption for an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 eV and not based upon use of the Stark effect on excitons, which device comprises: (i) a semiconductor structure including multiple quantum well layers; (ii) means for applying to the quantum well layers an electric field having a component of the field normal to the layers which may be controlled so as to determine the absorption edge of the quantum well layers to be on either side of the optical signal wavelength for optical signals propagating through the quantum well layers in a direction parallel to said layers, said optical signal having an electric vector disposed parallel to said layers; and (iii) optical signal input and output ports arranged to cause the propagation of the optical signal, having an electric vector disposed parallel to the layers, through the quantum well layers in a direction parallel to said layers.
Claim 24
Independent Claim
112 words
A method of modulating or switching an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 eV without substantially using the Stark effect on excitons, which method comprises the step of: introducing an optical signal into multiple semiconductor quantum well layers so as to propagate in the plane of said layer and modulating a component of an electric field disposed normal to the quantum well layers so as to move the absorption edge of the quantum well layers between positions to either side of the signal wavelength for optical signals propagating through the quantum well layers, said optical signal having an electric vector disposed parallel to said layers.
Claim 25
Independent Claim
112 words
A method of modulating or switching an optical signal having a wavelength corresponding to a photon energy not exceeding 1.2 eV without substantially using the Stark effect on excitons, which method comprises the step of: introducing an optical signal into multiple semiconductor quantum well layers so as to propagate in the plane of said layer and modulating a component of an electric field disposed normal to the quantum well layers so as to move the absorption edge of the quantum well layers between positions to either side of the signal wavelength for optical signals propagating through the quantum well layers, said optical signal having an electric vector disposed parallel to said layers.
Claim 26
Independent Claim
187 words
A method of time demultiplexing an optical signal corresponding to a photon energy not exceeding 1.2eV by propagating within multiple quantum well layers along an x-axis parallel to said layers, an optical signal having an electric vector oriented along a y-axis perpendicular to said x-axis but yet parallel to said layers, and applying respectively different time-varying electric fields to successive quantum well layer devices, each having semiconductor quantum well layers with a low conductance-valence energy band gap located between interleaved layers having a substantially higher conductance-valence energy band gap encompassing and bracketing said low energy band gap so as to provide quantum well confinement of both electrons and holes in each quantum well layer, said devices being optically coupled for passage of an optical signal propagating within said multiple quantum well layers and parallel to the plane of said quantum well layers while said electric fields are oriented along a z-axis perpendicular to said quantum well layers and perpendicular to both said x and y axes so as to move the absorption edge of the quantum well layers between positions to either side of the signal wavelength.
Claim 27
Independent Claim
187 words
A method of time demultiplexing an optical signal corresponding to a photon energy not exceeding 1.2eV by propagating within multiple quantum well layers along an x-axis parallel to said layers, an optical signal having an electric vector oriented along a y-axis perpendicular to said x-axis but yet parallel to said layers, and applying respectively different time-varying electric fields to successive quantum well layer devices, each having semiconductor quantum well layers with a low conductance-valence energy band gap located between interleaved layers having a substantially higher conductance-valence energy band gap encompassing and bracketing said low energy band gap so as to provide quantum well confinement of both electrons and holes in each quantum well layer, said devices being optically coupled for passage of an optical signal propagating within said multiple quantum well layers and parallel to the plane of said quantum well layers while said electric fields are oriented along a z-axis perpendicular to said quantum well layers and perpendicular to both said x and y axes so as to move the absorption edge of the quantum well layers between positions to either side of the signal wavelength.
Claim 28
Independent Claim
159 words
A method of frequency demultiplexing an optical signal corresponding to a photon energy not exceeding 1.2eV by propagating within multiple quantum well layer along an x-axis parallel to said layers, an optical signal having an electric vector oriented along a y-axis perpendicular to said x-axis but yet parallel to said layers, and applying respectively different but constant electric fields to the quantum well layers of successive quantum well layer devices, each having semiconductor quantum well layers with a low conductance-valaence energy band gap located between interleaved layers having a substantially higher conductance-valence energy band gap encompassing and bracketing said low energy band gap so as to provide quantum well confinement of both electrons and holes in each quantum well layer, said devices being optically coupled for passage of an optical signal in the plane of said quantum well layers while said electric fields are oriented perpendicular to said quantum well layers and perpendicular to both x and y axis.
Claim 29
Independent Claim
159 words
A method of frequency demultiplexing an optical signal corresponding to a photon energy not exceeding 1.2eV by propagating within multiple quantum well layer along an x-axis parallel to said layers, an optical signal having an electric vector oriented along a y-axis perpendicular to said x-axis but yet parallel to said layers, and applying respectively different but constant electric fields to the quantum well layers of successive quantum well layer devices, each having semiconductor quantum well layers with a low conductance-valaence energy band gap located between interleaved layers having a substantially higher conductance-valence energy band gap encompassing and bracketing said low energy band gap so as to provide quantum well confinement of both electrons and holes in each quantum well layer, said devices being optically coupled for passage of an optical signal in the plane of said quantum well layers while said electric fields are oriented perpendicular to said quantum well layers and perpendicular to both x and y axis.
References Cited (Backward Citations)
GB1102749A
Cited
GB1331228A
Cited
US3748597A
Cited
US3863070A
Cited
US4208667A
Cited
US4525687A
Cited
US4507776A
Cited
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1992-05-01 | 1992-10-31 | 1993-05-02 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1996-05-01 | 1996-10-31 | 1997-05-02 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 2000-05-01 | 2000-10-31 | 2001-05-02 | $7700.00 | Window Closed / Lapsed |