USH1080H - Electronic light beam switch - Google Patents
Electronic light beam switch Download PDFInfo
- Publication number
- USH1080H USH1080H US07/611,556 US61155690A USH1080H US H1080 H USH1080 H US H1080H US 61155690 A US61155690 A US 61155690A US H1080 H USH1080 H US H1080H
- Authority
- US
- United States
- Prior art keywords
- fiber optic
- switch
- transparent
- electrode
- optic switch
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/29—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the position or the direction of light beams, i.e. deflection
- G02F1/31—Digital deflection, i.e. optical switching
- G02F1/313—Digital deflection, i.e. optical switching in an optical waveguide structure
- G02F1/3131—Digital deflection, i.e. optical switching in an optical waveguide structure in optical fibres
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/07—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on electro-optical liquids exhibiting Kerr effect
- G02F1/073—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on electro-optical liquids exhibiting Kerr effect specially adapted for gating or modulating in optical waveguides
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/29—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the position or the direction of light beams, i.e. deflection
- G02F1/31—Digital deflection, i.e. optical switching
- G02F1/313—Digital deflection, i.e. optical switching in an optical waveguide structure
- G02F1/3137—Digital deflection, i.e. optical switching in an optical waveguide structure with intersecting or branching waveguides, e.g. X-switches and Y-junctions
Definitions
- the present invention relates generally to the technology of fiber optic light switches, particularly to switches that utilize an electric current in conjunction with crystal systems, and more particularly to fiber optic switches utilizing Kerr cells.
- Kerr effect when an electric field is applied to liquids with anisotropic molecules, an optical birefringence is induced. This effect is referred to as the Kerr effect and is generally defined as a quadratic function of the applied electric field. Thus, when an electric field is applied to a Kerr cell constructed on this principle it changes from opaque to transparent.
- the present invention utilizes the Kerr effect in anisotropic materials with pairs of polarizers to switch light paths from one fiber optic bundle to another by applying an electrical field to the anisotropic material.
- the present invention comprises a fiber optic cable that is divided into several fiber optic bundles. At each fiber optic bundle a switch device is inserted along the bundle.
- the switch device comprises a pair of transparent polarizers with the same index of refraction. These polarizers, in turn, sandwich a pair of transparent electrodes. The space between the transparent electrodes is filled with an anisotropic material.
- the electrodes of the switch device are electrically connected to a power source and an electrical switch.
- the polarizers may be paired in a number of different ways. Generally, one set of polarizers is positioned such that the pair of polarizers are aligned with each other and the other set such that its pair are crossed.
- the anisotropic material passes the light between the electrodes.
- the set of crossed polarizers does not transmit the light while the set of aligned polarizers does pass the light.
- the unit with the crossed polarizers transmits the light while the unit with the aligned polarizers does not.
- the anisotropic material passes the light with or without the presence of the electric field.
- This invention may be inserted into any optical transmission line.
- FIG. 1 is a schematic illustration of the present invention.
- FIG. 1 is a schematic illustration of the present invention.
- the major components of the present invention are a fiber optic cable 10 that is divided into several fiber optic bundles 110; polarizer units 15 and 16 with polarizers 120 of the same index of refraction which are attached to a polished end of each fiber optic bundle 110; transparent electrodes 130 which are sandwiched between the polarizers; anisotropic material 140, such as nitrobenzene, which fills the space between the pairs of transparent electrodes 130; a power source 150 which is electrically connected to the transparent electrodes; and an electric switch 160 that completes the circuit between the power source 150 and transparent electrodes 130 when the electric switch 160 is activated.
- anisotropic material 140 such as nitrobenzene
- the polarizer units 15 and 16 have polarizers 120 that are either aligned such that they cross each other or they complement each other. With the electric field switched on, the polarizer unit 16 with crossed polarizations (as shown by arrows 135) is transparent and the polarizer unit 15 with aligned polarizations (as shown by arrows 135) is opaque. When the electric field is off, the polarizer unit 16 with crossed polarizations becomes opaque and the polarizer unit 15 with aligned polarizations becomes transparent. Therefore, when the electrical switch is activated the aligned polarizer unit is opaque and the crossed polarizer unit is transparent. The converse is the case when the electric switch is not activated.
- Various modifications may be used to couple light signals from different fiber optic bundles or cables to other fiber optic lines or to add light signals through a cable from an auxiliary line.
- the properties of an anisotropic material permit light of one polarization to be switched from one filer optic bundle to another. Therefore, the cross-sections of the fiber optic bundles should equal each other through any one coupling.
- the polarizer units should also be attached only to polished ends of the fiber optic bundles.
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
The invention disclosed herein is a fiber optic switch which utilizes Kerrells to change the polarization of light passing through a pair of polarizers when an electric field is applied to the Kerr cell. The fiber optic switch is comprised of a pair of transparent polarized panels which have the same index of refraction, a pair of transparent electrodes which are electrically connected to a power source and an electric switch and which are sandwiched between the transparent polarized panels, and a layer of anisotropic material which fills the space between the electrodes.
Description
The invention described herein may be manufactured, used and licensed by or for the Government of the United States for governmental purposes without the payment to us of any royalties thereon.
The present invention relates generally to the technology of fiber optic light switches, particularly to switches that utilize an electric current in conjunction with crystal systems, and more particularly to fiber optic switches utilizing Kerr cells.
It is well known that when an electric field is applied to liquids with anisotropic molecules, an optical birefringence is induced. This effect is referred to as the Kerr effect and is generally defined as a quadratic function of the applied electric field. Thus, when an electric field is applied to a Kerr cell constructed on this principle it changes from opaque to transparent.
Heretofore liquid crystals have been incorporated in fiber optic switching devices as disclosed in U.S. Pat. No. 3,918,794 issued to A. Fenner Milton on Nov. 11, 1975. This device, however, has a relatively slow switch rate as compared to the rate of the present device which utilizes the Kerr effect as the principle used in the optic switch.
It is an objective of this invention to provide a high speed switch for fiber optic cables.
It is another objective of this invention to provide a low cost fiber optic switch that may be fabricated in volume.
It is another objective to provide a fiber optic switch with no moving or mechanical parts.
These and other objectives are accomplished by the present invention which utilizes the Kerr effect in anisotropic materials with pairs of polarizers to switch light paths from one fiber optic bundle to another by applying an electrical field to the anisotropic material. The present invention comprises a fiber optic cable that is divided into several fiber optic bundles. At each fiber optic bundle a switch device is inserted along the bundle. The switch device comprises a pair of transparent polarizers with the same index of refraction. These polarizers, in turn, sandwich a pair of transparent electrodes. The space between the transparent electrodes is filled with an anisotropic material. The electrodes of the switch device are electrically connected to a power source and an electrical switch. Depending on the desired effect, the polarizers may be paired in a number of different ways. Generally, one set of polarizers is positioned such that the pair of polarizers are aligned with each other and the other set such that its pair are crossed.
In the absence of an electrical field between the electrodes, the anisotropic material passes the light between the electrodes. However, the set of crossed polarizers does not transmit the light while the set of aligned polarizers does pass the light. With the electric field between the electrodes, the unit with the crossed polarizers transmits the light while the unit with the aligned polarizers does not. The anisotropic material passes the light with or without the presence of the electric field.
This invention may be inserted into any optical transmission line.
FIG. 1 is a schematic illustration of the present invention.
FIG. 1 is a schematic illustration of the present invention. The major components of the present invention are a fiber optic cable 10 that is divided into several fiber optic bundles 110; polarizer units 15 and 16 with polarizers 120 of the same index of refraction which are attached to a polished end of each fiber optic bundle 110; transparent electrodes 130 which are sandwiched between the polarizers; anisotropic material 140, such as nitrobenzene, which fills the space between the pairs of transparent electrodes 130; a power source 150 which is electrically connected to the transparent electrodes; and an electric switch 160 that completes the circuit between the power source 150 and transparent electrodes 130 when the electric switch 160 is activated. The polarizer units 15 and 16 have polarizers 120 that are either aligned such that they cross each other or they complement each other. With the electric field switched on, the polarizer unit 16 with crossed polarizations (as shown by arrows 135) is transparent and the polarizer unit 15 with aligned polarizations (as shown by arrows 135) is opaque. When the electric field is off, the polarizer unit 16 with crossed polarizations becomes opaque and the polarizer unit 15 with aligned polarizations becomes transparent. Therefore, when the electrical switch is activated the aligned polarizer unit is opaque and the crossed polarizer unit is transparent. The converse is the case when the electric switch is not activated.
Various modifications may be used to couple light signals from different fiber optic bundles or cables to other fiber optic lines or to add light signals through a cable from an auxiliary line. The properties of an anisotropic material permit light of one polarization to be switched from one filer optic bundle to another. Therefore, the cross-sections of the fiber optic bundles should equal each other through any one coupling. The polarizer units should also be attached only to polished ends of the fiber optic bundles.
The exact dimensions and configurations of the fiber optic switch are all considered to be within the knowledge of persons conversant with this art. It is therefore considered that the foregoing disclosure relates to a general illustration of the invention and should not be construed in any limiting sense, it being the intent to define the invention by the appended claims.
Claims (5)
1. A fiber optic switch useful for switching a portion of a fiber optic signal transmitted through a multi-fiber optic cable to at least one other fiber optic cable, the fiber optic switch comprising:
a first transparent polarized panel;
a fiber optic cable wherein an end of the fiber optic cable is attached to said first transparent polarized panel;
a first electrode connected to said first transparent polarized panel;
a power source electrically connected to said first electrode;
a second electrode positioned adjacent to said first electrode;
an electric switch electrically connected to said second electrode;
a second transparent polarized panel connected to the opposite end of said fiber optic cable and connected to said second electrode, said second transparent polarized panel having an index of refraction equal to that of said first transparent polarized panel;
an anisotropic material disposed between said first and second electrodes.
2. The fiber optic switch of claim 1 wherein said fiber optic switch is connected to a plurality of fiber optic cables.
3. The fiber optic switch of claim 1 wherein said anisotropic material consists of nitrobenzene.
4. The fiber optic switch of claim 1 wherein said fiber optic switch is hermetically sealed.
5. The fiber optic switch of claim 1 wherein said fiber optic switch is attached to polished and fused ends of said fiber optic bundle.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US07/611,556 USH1080H (en) | 1990-11-13 | 1990-11-13 | Electronic light beam switch |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US07/611,556 USH1080H (en) | 1990-11-13 | 1990-11-13 | Electronic light beam switch |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| USH1080H true USH1080H (en) | 1992-07-07 |
Family
ID=24449499
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US07/611,556 Abandoned USH1080H (en) | 1990-11-13 | 1990-11-13 | Electronic light beam switch |
Country Status (1)
| Country | Link |
|---|---|
| US (1) | USH1080H (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20110169937A1 (en) * | 2010-01-12 | 2011-07-14 | Mclaughlin John | Mode of action screening method |
-
1990
- 1990-11-13 US US07/611,556 patent/USH1080H/en not_active Abandoned
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20110169937A1 (en) * | 2010-01-12 | 2011-07-14 | Mclaughlin John | Mode of action screening method |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| STCF | Information on status: patent grant |
Free format text: PATENTED CASE |