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US5073809A
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Electro-optic modulation method and device using the low-energy oblique transition of a highly coupled super-grid
Assignee: Centre National de la Recherche Scientifique
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Filing: 1990-12-03
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Granted: 1991-12-17
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Expires: 2010-12-03
Abstract
Abstract An Electro-Optic modulation method and device using a low-energy oblique transition of a tightly coupled super-grid. According to the present invention, a luminous beam is injected into a tightly coupled super-grid and an electric field (E) is applied to the super-grid whose amplitude is made to gradually vary so as to cause the intensity of the beam to vary. This beam is injected parallel to the plane of the films of the super-grid which guides the injected beam. The electric field is weak and applied along the growth direction of the super-grid, which provokes the appearance of a low energy oblique transition (TB) in a domain of wavelengths where the super-grid is transparent in the absence of any electric field. The super-grid is one whereby the wavelength of the luminous beam is contained in this domain. Such a device may find application in optical telecommunications systems.
Inventors
- 👤 Erwan Bigan
- 👤 Michel Allovon
- 👤 Paul Voisin
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-11-08 03:51
CPC Classifications
G; G02; G02F; G02F1/00; G02F1/01; G02F1/015; G02F1/017; G02F1/01708; B; B82; B82Y; B82Y20/00; G02F1/0155; G02F1/0157
Claims Analysis
Total Claims: 16
Claim 1
Independent Claim
161 words
A method for modulating the intensity of a luminous beam, comprising the steps of: injecting a luminous beam into an electro-absorbent semiconductive element, wherein the electro-absorbent element includes a tightly coupled super-grid formed of films stacked along a direction constituting a growth direction of the super-grid, wherein the luminous beam is injected into the super-grid parallel to a plane of the films of this super-grid wherein this super-grid is provided to guide the injected luminous beam; and applying to this semiconductive element an electric field whose amplitude is made to gradually vary so as to vary the intensity of the luminous beam, wherein the electric field is weak and applied along the growth direction of the super-grid, thereby provoking the appearance of a low-energy oblique transition in a domain of wavelengths where the super-grid is transparent in the absence of any electric field, and wherein the super-grid is such that a wavelength of the luminous beam is contained in this domain.
Claim 2
Independent Claim
161 words
A method for modulating the intensity of a luminous beam, comprising the steps of: injecting a luminous beam into an electro-absorbent semiconductive element, wherein the electro-absorbent element includes a tightly coupled super-grid formed of films stacked along a direction constituting a growth direction of the super-grid, wherein the luminous beam is injected into the super-grid parallel to a plane of the films of this super-grid wherein this super-grid is provided to guide the injected luminous beam; and applying to this semiconductive element an electric field whose amplitude is made to gradually vary so as to vary the intensity of the luminous beam, wherein the electric field is weak and applied along the growth direction of the super-grid, thereby provoking the appearance of a low-energy oblique transition in a domain of wavelengths where the super-grid is transparent in the absence of any electric field, and wherein the super-grid is such that a wavelength of the luminous beam is contained in this domain.
Claim 3
Dependent Claim
36 words
A method according to claim 1, wherein a thickness of the super-grid is about 0.5 micrometers and wherein the electric field is obtained for a control voltage of about 1 V for controlling the semiconductive element;
Claim 4
Dependent Claim
45 words
A method according to claim 1, wherein the super-grid is included in a core of a luminous wave guide, this wave guide comprising two films between which the core is located and whose respective optical indices are smaller than the optical index of the super-grid.
Claim 5
Dependent Claim
43 words
A method according to claim 3, wherein the wave guide is a PIN type diode which is polarized, and whose intrinsic region I contains the super-grid and whose regions P and N have optical indices smaller than an optical index of the super-grid.
Claim 6
Dependent Claim
32 words
A method according to claim 1, wherein the wavelength of the luminous beam is about 1.5 micrometers and wherein the super-grid is comprised by a stacking of alternate GaInAs and AlInAs films.
Claim 7
Dependent Claim
32 words
A method according to claim 1, wherein the wavelength of the luminous beam is about 1.5 micrometers and wherein the super-grid is comprised by a stacking of alternate GaInAs and InP films.
Claim 8
Dependent Claim
32 words
A method according to claim 1, wherein the wavelength of the luminous beam is about 0.8 micrometers and wherein the super-grid is comprised by a stacking of alternate GaAs and GaAlAs films.
Claim 9
Independent Claim
178 words
A device for modulating the intensity of a luminous beam, comprising: an electro-absorbent semiconductive element to receive the luminous beam, wherein the electro-absorbent element includes a tightly coupled super-grid formed of films stacked along a direction which constitutes a growth direction of the super-grid, wherein the super-grid is provided to guide the luminous beam when the luminous beam is injected into the super-grid parallel to a plane of the films of the super-grid; and control means for applying to this semiconductive element an electric voltage and to gradually vary the amplitude of the voltage so as to vary the intensity of the luminous beam, wherein the control means are provided to apply an electric voltage which generates in the super-grid a weak electric field which is parallel to the growth direction of the super-grid, thereby provoking the appearance of a low-energy oblique transition in a domain of wavelengths where the super-grid is transparent in the absence of any electric field, and wherein the super-grid is such that a wavelength of the luminous beam is contained in this domain.
Claim 10
Independent Claim
178 words
A device for modulating the intensity of a luminous beam, comprising: an electro-absorbent semiconductive element to receive the luminous beam, wherein the electro-absorbent element includes a tightly coupled super-grid formed of films stacked along a direction which constitutes a growth direction of the super-grid, wherein the super-grid is provided to guide the luminous beam when the luminous beam is injected into the super-grid parallel to a plane of the films of the super-grid; and control means for applying to this semiconductive element an electric voltage and to gradually vary the amplitude of the voltage so as to vary the intensity of the luminous beam, wherein the control means are provided to apply an electric voltage which generates in the super-grid a weak electric field which is parallel to the growth direction of the super-grid, thereby provoking the appearance of a low-energy oblique transition in a domain of wavelengths where the super-grid is transparent in the absence of any electric field, and wherein the super-grid is such that a wavelength of the luminous beam is contained in this domain.
Claim 11
Dependent Claim
36 words
A method according to claim 8, wherein a thickness of the super-grid is about 0.5 micrometers and wherein the electric field is obtained for a control voltage of about 1 V for controlling the semiconductive element.
Claim 12
Dependent Claim
45 words
A method according to claim 8, wherein the supergrid is included in a core of a luminous wave guide, this wave guide comprising two films between which the core is located and whose respective optical indices are smaller than the optical index of the super-grid.
Claim 13
Dependent Claim
43 words
A method according to claim 10, wherein the wave guide is a PIN type diode which is polarized and whose intrinsic region I contains the super-grid and whose regions P and N have optical indices smaller than an optical index of the super-grid.
Claim 14
Dependent Claim
32 words
A method according to claim 8, wherein the wavelength of the luminous beam is about 1.5 micrometers and wherein the super-grid is comprised by a stacking cf alternate GaInAs and AlInAs films.
Claim 15
Dependent Claim
32 words
A method according to claim 8, wherein the wavelength of the luminous beam is about 1.5 micrometers and wherein the super-grid is comprised by a stacking of alternate GaInAs and InP films.
Claim 16
Dependent Claim
32 words
A method according to claim 8, wherein the wavelength of the luminous beam is about 0.8 micrometers and wherein the super-grid is comprised by a stacking of alternate GaAs and GaAlAs films.
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