WO1995005617A1 - Enhancing the nonlinearity of an optical waveguide - Google Patents
Enhancing the nonlinearity of an optical waveguide Download PDFInfo
- Publication number
- WO1995005617A1 WO1995005617A1 PCT/SE1994/000745 SE9400745W WO9505617A1 WO 1995005617 A1 WO1995005617 A1 WO 1995005617A1 SE 9400745 W SE9400745 W SE 9400745W WO 9505617 A1 WO9505617 A1 WO 9505617A1
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- light
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- core
- guide
- light source
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/2804—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers
- G02B6/2821—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers using lateral coupling between contiguous fibres to split or combine optical signals
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- 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
- G02F1/35—Non-linear optics
- G02F1/365—Non-linear optics in an optical waveguide structure
Definitions
- the present invention is concerned with waveguides for optical and near optical wavelengths adopted to use nonlinear optical effects of particular kinds and of particular materials.
- Optical glass fibers are a cheap waveguide medium that can be exploited for applications in nonlinear optics.
- Fused quartz has a small nonlinear coefficient as compared with materials such as semiconductors. This has limited considerably the use of fibers in applications such as optical switching, because the optical power of the control signal has to be high in order to cause an appreciable change in the properties of the fiber, see "All-optical Waveguide Switching", G.I. Stegeman, E.M. Wright, Optical and Quantum Electronics 22 (1990), pps. 95-122.
- a non-linear optical fiber coupler having two polarization-maintaining optical fibers of elliptical cross-sections located in parallel at the opposite sides of a central structure.
- This central structure has a lens-shaped cross-section, that is formed by two oppositely placed arc sections.
- the central thickness of this middle structure is a few times larger than the diameters of the fibers and many times the diameters of the cores of the fibers.
- support structures are used for maintaining the fibers in the desired configura ions.
- the middle structure is a single crystal of an electro-optic material having a non-centro- symmetrical crystal structure.
- the materials mentioned are organic type materials being electric insulators.
- the physical effect utilized is based on the electro-optical effect, the refractive index of the material being changed by interaction with the electric field of an incoming light wave, the pump wave.
- An optical fiber has a portion of its cladding removed by polishing a slightly curved fiber along plane.
- a light-absorbing substance having non-linear light-absorbing characteristics, in particular a dye, is applied to the polished surface to make light propagating in the fiber to be absorbed in a controlled way.
- a D-fiber is used being in contact, at its flattened surface with a material which is non-centro-symmetrical in order to obtain frequency doubling.
- laser diodes are connected injecting light of the same wavelengths to the D-fiber. Light emitted by the layer is collected to find the correlation of the signals from the laser diodes.
- an optical D-fiber may be provided with a layer on the flat surface, the layer being of a material having a refractive index varying with optical intensity.
- the free surface of the layer is illuminated by coherent light beams to form a standing wave of a modulated refractive index in the layer resulting in a modulated index grating.
- This device can be used as a fiber-based nonlinear optical coupler that is controlled by a relatively weak light signal.
- the same device can be used as a laser, and in a number of other applications.
- the invention is concerned with an optical device comprising a wave-guide with a core, a layer being arranged, which has a uniform thickness and is located in parallel to and at a uniform distance from the core. The distance is such that the evanescent electromagnetic field of light propagated along the wave-guide extends into the layer.
- the material of the layer is selected to have non-linear optical properties.
- the wave-guide is preferably dimensioned for propagating light of only one wavelength, that is it is raonomode.
- the material is preferably optically homogeneous or centro- sym etric. It may have a refractive index for light of a first kind having a considered wavelength and suitable for propagation along the wave-guide, where the value of the refractive index, in particular for wavelengths close to the wavelength of the light of the first kind, is dependant, on light of a second kind which is some manner is arranged to interact with the material and has a wavelength different from that of the first light, that is the refractive index of the material for wavelengths about the wavelength of the first light varies significantly, when there is a change in the second light.
- the value of the refractive index may be dependant on the intensity of the light of the second kind.
- the material is in a preferred embodiment a semiconductor with a bandgap.
- first light may be propagated along the wave-guide and second light may be arranged to interact with the semiconductor material in the layer.
- the wavelength of the second light can in that case correspond to an energy value well exceeding the bandgap, so that photons of the second light are absorbed in the material creating an electron-hole pair.
- the wavelength of the first light then is selected to have a value corresponding to an energy value significantly below that of the bandgap, so that essentially no electron-hole pairs are created by absorption of the first light.
- the distance from the layer to the core of the wave-guide may'be smaller than the diameter of the core to fulfil the condition of the evanescent field extending into the layer.
- the thickness of the layer is generally small to allow a good adherence to the waveguide and it may in particular be a small fraction of the diameter of the core of the wave-guide, in particular in the range of 1/8 to 1/80 thereof, most preferred in the range of 1/16 to 1/80 thereof.
- the wave guide comprises a first optical D- fiber which as conventional has a curved surface corresponding to a portion of the surface of a circular cylinder, normally essentially a semi-cylindrical surface, and a flat surface.
- the flat surface should then be located in parallel with the core of the D-fiber and at a small distance from the core and the layer should the be arranged on the flat surface.
- an optical coupler may be arranged which as conventional has first and second parallel ports at a first side and first and second ports at a second side.
- the two ports at one side can be joined by a wave-guide, and a first light source provides signal light to a port at the other side.
- the layer should then be arranged at a segment of the joining wave-guide in order to control the signal light.
- a second light source may be arranged providing control light and direct it for interaction with the material of the layer.
- the second light source is in a first alternative arranged to direct the control light directly to a free surface of the layer.
- the second light source is arranged to instead provide the control light to one port at the other side of the coupler.
- a phase-delaying device is then advantageously arranged in the joining wave-guide and it delays light derived from the signal light in order to allow the control light work in an on-off fashion, controlling the signal light to either one of the ports at the other side of the coupler.
- the device constructed of a coated D-fiber can for some uses be completed by a second optical D-fiber also having an essentially semi-cylindrical surface and a flat surface, for instance of the same kind as the first one.
- the flat surface of the second D-fiber is then arranged against the free surface of the layer, that is the surface which is opposite to the first D- fiber.
- Such a double D-fiber device can be used for coupling purposes. Then there is a first light source providing signal light, where the light source is arranged to provide the signal light to a first end of the first D-fiber.
- a second light source provides control light, so that the control light is input to a first end of the second D-fiber.
- the first ends of the D-fibers are preferably defined to be those two ends which permit the signal and control light to propagate along the cores of the D- fibers in parallel to and in the same direction as each other, but it is also possible to define the first ends so that the signal and control light propagate in the opposite directions.
- the second ends of the D-fibers are naturally those which are opposite to the first ends. The second ends are then attached to signal light receiving and/or transmission means.
- the control light can be provided to the first end of the first D-fiber, that is the same end as the signal light.
- the configuration comprising two juxtaposed D-fibers can be characterized generally by the feature that the basic wave-guide, in addition to the core mentioned initially above, comprises another core extending in parallel to the first mentioned core.
- the layer should then be located at the same uniform distance of the two cores, whereby the evanescent electromagnetic fields of light propagated along the two cores extend into the layer.
- the device comprises a planar structure, where the two cores are arranged in the flat surface of a substrate. This surface is covered by a layer of having substantially the same refractive index as the substrate. The surface of this layer is in turn coated with a layer of a material having non-linear optical properties as above.
- twin-core devices can be used for coupling as the double D-fiber.
- the general device as described above may comprise a light source providing pump light.
- This source is arranged to inject the pump light to a first end of the wave ⁇ guide to make it propagate along the core into the region where the layer is positioned close to the core.
- the pump light is selected to have such a wavelength and intensity that it will cause stimulated emission of light in the material of the layer. From a second end of the wave-guide opposite to the first end thereof then the light produced by the stimulated emission can be directed to some other device.
- the layer has a width, that is a dimension in a transverse direction in relation to the longitudinal direction of the wave-guide core and in parallel with the surface of the wave-guide, which corresponds to only a few times the diameter of the core, in particular three core diameters at most, and at least one core diameter.
- the layer may be located on a flat surface of the wave-guide or it may be located in a groove in the material of the wave-guide, where the groove then extends in parallel to the wave-guide core.
- the interferometric device can also be described as comprising a coupling means having a first and a second pair of optical communication ports in which optical pulse signals received at a port of one pair are coupled substantially equally into the each port of the other pair. It further comprises an optical waveguide optically coupling together the second pair of ports.
- the optical waveguide includes a portion where light propagating in the waveguide will sense a non-linear refractive index, where this portion comprises a waveguide having a core and a piece of material, which typically is the "layer" mentioned above, being located at such a distance from the core such that the evanescent electromagnetic field of light propagated along this waveguide and its core extends into the material. This material should then exhibit non-linear optical characteristics.
- the piece of material or "layer” can then have a free surface, arranged so that a light source provides control light to the free surface for interaction with the material.
- a light source is arranged to provide control light to one port of the first pair.
- the optical device for use for coupling purposes can be generally described as comprising a wave-guide with two cores for guiding light waves along each one of the cores, where a piece of material located at such distances from the cores, that the evanescent electromagnetic field of light propagated along each wave-guide core extends into the piece of material.
- the material thereof should have non-linear optical properties.
- An optically controlled coupler system, switching or modulating system, including such a two-core device can be described as comprising generally a coupling means having a first and a second pair of optical communication ports. It further comprises a first light source providing signal light to a first one of the first pair of ports and a second light source providing control light to the first one or a second one of the first pair of ports.
- the ports of the second pair are each one as above attached to separate signal light receiving and/or transmission means.
- the coupling means comprises a wave-guide with two cores for guiding light waves along each one of the cores and a piece of material, the above "layer”, located at such distances from the cores, that the evanescent electromagnetic field of light propagated along each wave-guide core extends into the piece of material.
- the material should have non ⁇ linear optical properties.
- An optically pumped laser structure as set out above comprises then generally a wave-guide with a core. It further comprises a piece of material or layer located at such a distance from the core, that the evanescent electromagnetic field of light propagated along the wave-guide extends into the piece of material or layer. The material should then have non-linear optical properties.
- One end of the waveguide is adapted to receive pump light from a light source and the other end is adapted to issue light obtained by stimulated emission in the piece of material.
- the waveguide may have a second core, such that light waves are able to propagate along each one of the two cores.
- the piece of material is then located at such distances from the cores, that the evanescent electromagnetic field of light propagated along each one of the wave-guide cores extends into the piece of material.
- the piece of material or layer may in the laser structure have a free surface being adapted to receive pump light from a light source.
- Fig. 1 shows a partially coated D-fiber
- Fig. 2 shows the fiber of Fig. 1 as employed in an interferometric device.
- Fig. 3a shows a double D-fiber structure with a film therebetween
- Fig. 3b schematically shows the structure of Fig. 3a as employed in an optic coupler
- Fig. 4a shows a coated D-fiber structure of the twin-core type
- Fig. 4b shows a planar wave guide structure with a layer of a non-linear optic material
- Fig. 5a shows a partially coated D-fiber for use as a laser.
- Figs. 5b and 5c show alternative coating arrangements which may be suitable for use in lasers
- Fig. 6 schematically shows a laser arrangement utilizing a coated D-fiber
- Fig. 7 schematically shows a laser arrangement utilizing a structure having two wave guide cores.
- a device comprising a D-shaped fiber 1 having a core 3 and a cladding 5 and coated on its flat surface over some length of the fiber with a thin layer 7 of a material that is highly nonlinear, such as a semiconductor.
- the length of the coating in the longitudinal direction of the fibre may as illustrated correspond to about the exterior diameter of the D- fiber and the coating may cover whole the flat surface of the fiber in the transverse direction. The length may however be adapted to the particular field of use and the materials used to obtain the desired effects to be discussed below.
- the D-fiber 1 may have dimensions matching ordinary single-mode communication fiber, e.g. have an outer cladding diameter of approximately 125 ⁇ m and a core diameter of 8 - 10 p, and should also ideally be single mode at the wavelength of interest.
- the core-flat surface distance d in the D-shaped fiber 1 should be such that the evanescent field of the light propagating through the fiber 1 can interact with the film 7, this meaning that the core-flat distance d is only a small portion of the core diameter.
- the D-fiber to be used should then in practical cases have a core-air distance d of a few micrometers or less, that is this distance d of the core 3 to the flat surface of the fiber 1 can be for instance of the magnitude of order 2 ⁇ m.
- the thickness of the coating film 7 is uniform and is normally much smaller than the diameter of the core. It may be typically 1 ⁇ m or less, for instance 0.1 - 0.5 ⁇ m. A thicker film cannot be used since it will not adhere permanently to the flat surface of the D-fiber due to different dilatation coefficients.
- the coating material in the layer 7 can be GaAs, InP, InGaAsP, and other III-V semiconductors, silicon and germanium based materials, such as amorphous Si, amorphous Ge, silicon carbide, porous Si, etc., II-VI semiconductors such as CdTe, CdS, CdSe and composites, and materials such as LiF, NaF, NaCl and other halogen alkalides.
- a preferred material for the film of many devices may be amorphous Si.
- the material can be deposited by some ordinary method such as some CVD technique and it is generally not necessary to grow the material in situ. It can also be further processed by ion or e-beam bombardment or UV irradiation.
- the fabrication of the device might also include an annealing process where the deposited material is heated and then cooled to the ambient temperature in order to alter the properties of the material, such as the recombination time of the charge carriers thereof.
- Structures comprising multiple thin films such as a single and multiple quantum well structures of III-V or other semiconductors can also be deposited on the flat surface of the fiber 1 and act as the highly nonlinear medium.
- the material deposited can either be amorphous or crystalline.
- Other materials of interest, such as films of rare-earth metals can be used.
- the film 7 as made of a semiconductor material, but all other materials described above are in the spirit of the invention.
- SCF Semiconductor Coated Fiber
- the wave propagating in the longitudinal direction of the fiber 1 can have its field extending into the material 7.
- the transverse mode of the propagating light depends on the real and imaginary parts of the linear and nonlinear susceptibilities of the material of the film 7.
- the properties of the material determine the effective refractive index experienced by the light propagating in the fiber, the chromatic dispersion, absorption, gain, polarization properties, and nonlinear effects such as phase modulation and frequency conversion for the light.
- signal light and control light corresponding to the terms “first light” and “second light”.
- the signal light has a photon energy close to or below the energy which is necessary to promote electrons from the valence (low mobility) to the conduction (higher mobility) band, i.e., the deposited material is "transparent" to the signal light.
- the photon energy exceeds the energy band gap of the material.
- light at a wavelength 0.85 ⁇ m can be used as control light for a film of InGaAs (bandgap for instance typically 1.3 - 1.55 ⁇ m) .
- the absorption of the control light photons creates mobile electrons in the material, temporarily affecting its properties. It can strongly alter the refractive index, and also shift the band gap through the Stark effect. Even the creation of mobile electrons through heat can induce a change in the refractive index.
- materials are used, the optical properties of which for a particular wavelength, i.e. that of the signal light, are changed when the materials interact with the control light in some way, for example as above by absorption of photons creating electron-hole pairs, by absorption creating heat in the material increasing its temperature.
- the materials preferred are optically homogeneous, for example amorphous, resulting in structures which can be manufactured easily and non-costly.
- a change in the refractive index of the coating material can be exploited amongst others, for switching, for modulation, and for mode-locking lasers. It can be advantageous to make use of an interferometric arrangement such as that disclosed in the patent US-A 4,973,122 and also in US-A 4,962,987.
- There an optical cross-coupled interferometer is disclosed where the control light is fed to one of the ports of the coupler and two parallel ports are join by a loop. Incoming light is split in two parts (generally of the same power) , which suffer different phase shifts depending on the presence of the control light. When they are recombined, even a small influence of the control light can greatly affect the amplitude of the emerging signal light.
- a coupler 9 has two parallel ports A and D at one side and two parallel ports B and C at the other side.
- the signal light P s is coupled into the port A of the coupler 9 that divides the signal light P s into two components of approximately equal power, to the ports B and C at the other side of the coupler.
- a device 11 of the kind illustrated in Fig. 1 is at one end connected to one of these ports like B. The other end of the device 11 is then joined to the other parallel port C at the same side. In this way, half of the signal light leaving the coupler 9 travels through first port B, through the device 11 and then to port C.
- a set of fiber strainers 13 such those designated as Manual Polarisation Controllers, manufactured by the company BT & D, can be provided along one of the paths, e.g. as illustrated in the path joining the device 11 with port C.
- the fiber strainers 13 can be adjusted so that all signal light recombines at the coupler 9 and returns through the input port A. In this state, no signal light exits through port D, that is the port which is parallel to port A and at the same side of the coupler.
- control light P c e.g. as obtained from a light source comprising a laser 13 and a lens system 15 and illuminating the surface of the film of the device 11, the refractive index of the deposited material in the coating film in the device 11 is altered.
- the relative phase shift introduced between the signal light components can lead to all signal light recombining at the coupler 9 being directed to port D.
- the exact position of the device 11 in the loop joining ports B and C can be important, particularly if the control light is continuous and not pulsed.
- control light may also be injected by port A and D producing the same change of refractive index of the coating in the device 11.
- Two D-shaped fibers 1 can also be placed with the flat surfaces in a back-to-back arrangement, with the semiconductor film 7 lying between the two cores 3, as shown in Fig. 3a.
- the fixtures can be used, each one with one fiber.
- the fixtures can be made of a softer material than glass, such as a plastics material or soft metal.
- One possible way to make the fixtures is to use a D-fiber as a mould for a liquid phase solution of the fixture. The D-fiber should be kept straight. After solidifying the solution, the fixture is ready to accommodate one of the D-fibers used in the double structure SCF.
- the fixtures can be glued together.
- the nonlinearity of the semiconductor film 7 can in this case be exploited by sending control light P c of appropriate wavelength through an input control port D of the device as illustrated in Fig. 3a used as a controlled coupler 17, c.f. Fig. 3b, having ports A and D at one end thereof and ports B and C at the other end.
- Signal light P s entering port A in parallel to the aforementioned control light P c can be affected by the control light P c entering port A.
- the signal light P s leaves the device 17 at either port B or C as in a conventional coupler, see "Optical Waveguide Theory", A.W. Snyder, J.D. Love, Chapman and Hall, London 1983, pps.
- control light P c In the presence of control light P c , the fraction of the light leaving ports B and C can be controlled. Even a weak signal P c can substantially modify the transfer function of the coupler, and therefore a weak signal P c can control a stronger signal P c as in a transistor.
- the nonlinear coupler described above can also be used as a high speed optical modulator.
- a continuous wave signal (signal light) P s coupled into port A of the device can be switched on and off in ports B and C by a control light pulse P c coupled into port D.
- the device operates as a switch. Since the device is relatively insensitive to the wavelength of the control light P c , even heavily chirped light pulses can be used to control the spectrally pure signal P s coupled into port A.
- the high speed of the device is based on the fact that the free-carriers photoinduced in the semiconductor in the film 7 in the device 17, by the absorption of the control light pulse can relax rapidly, so that bit rates of several Gbits/s should be achieved.
- the optical signal that leaves the device through ports B and C can therefore have a narrow bandwidth and high speed modulation.
- a twin-core D-shaped fiber can have the coupling characteristics controlled by the activation of a semiconductor film, as illustrated in figure 4a.
- the D-fiber 19 has two cores 3' , 3", which are disposed in parallel symmetrically and centrally, close to the center line of the circular-cylindrical outer surface of the fiber 19 and as above close to the flat surface.
- the evanescent field of the control light propagating in one of the fiber cores 3', 3" penetrates the semiconductor film 7 coated on the flat surface, altering its properties, and thus the propagation characteristics of signal light travelling in the other core.
- the twin-core structure of Fig. 4a can be used like the double D-fiber of Fig. 3a, e.g. in the coupler as illustrated in Fig. 3b.
- a pair of waveguides 21 can be fabricated on a glass substrate 23 by ion implantation or thermal indiffusion. Further evaporation of a layer 25 of silicon oxides SiO/Si0 2 might be desirable, leaving the waveguides 21 immersed in the glass matrix. A film 7 of semiconductor material is then deposited on the top surface of the buried waveguides 21, so that the evanescent field of the light in the waveguides 21 extends into the semiconductor material 7.
- Fig. 4b can be used like the double D- fiber of Fig. 3a.
- Semiconductors are widely used as laser materials. Generally, laser pumping is electrical, but light has also been used to pump laser structures. The pump light should have enough photon energy to be absorbed by the film, creating an excess of electrons in the excited state and an excess of holes in the lower energy band. Upon radiative recombination, the semiconductor will luminesce. Provided the pump light is sufficiently intense it will cause stimulated emission and laser action in the semiconductor film. The high refractive index of the semiconductor material favours guiding of light in the plane of the semiconductor film.
- Gain guiding is often sufficient to ensure that the device operates above laser threshold. Since the pump field overlaps the semiconductor film only in the region neighbouring the core of the fiber, the width of the film where laser operation is taking place, is limited to less than approximately 10 ⁇ m. A structure similar to that depicted in Fig. 1 can be used as is illustrated in Fig. 5a.
- the unpumped region of the semiconductor may be removed by lithographic processes, as illustrated in Fig. 5b.
- the D-shaped fiber can have its cross sectional profile altered as shown in Fig. 5c.
- the semiconductor film 7" is deposited in the groove 27. This will ensure that only the narrow strip 1 ' or 7" of semiconductor material guides light.
- Figs. 5b and 5c will be able to provide laser action even in the absence of end mirrors, provided that the gain is sufficient. End mirrors may otherwise be provided by the use of coated or uncoated fiber end surfaces or by Bragg reflection.
- the active length of the laser can be as long as several centimetres corresponding to the longitudinal length of the coating 7 (Fig. 5a) . Typical materials that can be employed would be those which have a high quantum efficiency for luminescence. III-V semiconductors such as GaAs deposited by MOVCD or MBE techniques, for example, can be used, as well as ternary compounds.
- the wavelength for laser operation will be those associated with the material bandgap (e.g. 0.85 ⁇ m for GaAs) .
- halogen alkalide films with colour centers such as the f-center of LiF or Lil.
- Such materials have a number of luminescence peaks in the visible and near infrared. The light generated in such a laser is guided along the film, but the near presence of the core of the fiber can also lead to light guidance in the core.
- a laser arrangement is schematically illustrated in Fig. 6.
- Pump light 29 from a suitable source 31 focused by a lens system as illustrated at 33 is injected to one end of the D-fiber 1.
- laser light 35 is emitted from the other end of the D-fiber and it can be parallelized by a lens system as illustrated at 37.
- the geometry with two parallel wave guide cores as illustrated in Figs. 3a and 3b and also in Figs. 4a and 4b can also be used as a laser device, where the laser output would be collected along the output ports B and C, cf. Fig. 7, with the pump light injected along port A.
- the pump light P p is absorbed by the semiconductor film 7 in the coupler 17 ' , it may as above by a proper choice of parameters and materials give rise to an excess of electrons in the excited state band and an excess of holes in the lower energy band. Upon radiative recombination, the semiconductor material will luminesce.
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- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Integrated Circuits (AREA)
- Optical Couplings Of Light Guides (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
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Priority Applications (10)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DK94924436T DK0664894T3 (en) | 1993-08-13 | 1994-08-15 | Increasing the non-linearity of an optical waveguide |
NZ271160A NZ271160A (en) | 1993-08-13 | 1994-08-15 | Optical waveguide with core and evanescent field affecting non linear layer |
EP94924436A EP0664894B1 (en) | 1993-08-13 | 1994-08-15 | Enhancing the nonlinearity of an optical waveguide |
KR1019950701418A KR100326582B1 (en) | 1993-08-13 | 1994-08-15 | Optical device with waveguide with nonlinear optical characteristics |
US08/416,718 US5642453A (en) | 1993-08-13 | 1994-08-15 | Enhancing the nonlinearity of an optical waveguide |
AU74701/94A AU690574B2 (en) | 1993-08-13 | 1994-08-15 | Enhancing the nonlinearity of an optical waveguide |
JP50690495A JP3718523B2 (en) | 1993-08-13 | 1994-08-15 | Enhancement of nonlinearity of optical waveguide |
AT94924436T ATE197194T1 (en) | 1993-08-13 | 1994-08-15 | INCREASING THE NONLINEARITY OF AN OPTICAL WAVEGUIDE |
DE69426190T DE69426190T2 (en) | 1993-08-13 | 1994-08-15 | INCREASING THE NONLINEARITY OF AN OPTICAL WAVE GUIDE |
GR20000402332T GR3034673T3 (en) | 1993-08-13 | 2000-10-26 | Enhancing the nonlinearity of an optical waveguide. |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
SE9302634-2 | 1993-08-13 | ||
SE9302634A SE514675C2 (en) | 1993-08-13 | 1993-08-13 | Optical coupler or modulator and laser including a waveguide |
Publications (1)
Publication Number | Publication Date |
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WO1995005617A1 true WO1995005617A1 (en) | 1995-02-23 |
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Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/SE1994/000745 WO1995005617A1 (en) | 1993-08-13 | 1994-08-15 | Enhancing the nonlinearity of an optical waveguide |
Country Status (15)
Country | Link |
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US (1) | US5642453A (en) |
EP (1) | EP0664894B1 (en) |
JP (1) | JP3718523B2 (en) |
KR (1) | KR100326582B1 (en) |
CN (1) | CN1047238C (en) |
AT (1) | ATE197194T1 (en) |
AU (1) | AU690574B2 (en) |
DE (1) | DE69426190T2 (en) |
DK (1) | DK0664894T3 (en) |
ES (1) | ES2151931T3 (en) |
GR (1) | GR3034673T3 (en) |
NZ (1) | NZ271160A (en) |
PT (1) | PT664894E (en) |
SE (1) | SE514675C2 (en) |
WO (1) | WO1995005617A1 (en) |
Cited By (13)
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WO1997021141A1 (en) * | 1995-12-01 | 1997-06-12 | The University Of Sydney | A method for inducing nonlinearities in active optical materials and apparatus for the use thereof |
WO2000049434A1 (en) * | 1999-02-19 | 2000-08-24 | Protodel International Limited | Optical fibre attenuator and method of attenuating light transmitted through an optical fibre |
US6191224B1 (en) | 1998-08-25 | 2001-02-20 | Molecular Optoelectronics Corporation | Dispersion-controlled polymers for broadband fiber optic devices |
US6205280B1 (en) | 1998-08-25 | 2001-03-20 | Molecular Optoelectronics Corporation | Blockless fiber optic attenuators and attenuation systems employing dispersion controlled polymers |
KR20010041065A (en) * | 1998-02-20 | 2001-05-15 | 케빈 알. 스튜어트 | Fiber optic attenuators and attenuation systems |
US6301426B1 (en) | 1999-03-16 | 2001-10-09 | Molecular Optoelectronics Corporation | Mechanically adjustable fiber optic attenuator and method employing same |
WO2002052312A1 (en) * | 2000-12-26 | 2002-07-04 | Ion Beam Services | Optically active waveguide device comprising a channel on an optical substrate |
US6483981B1 (en) | 2000-06-28 | 2002-11-19 | Molecular Optoelectronics Corp. | Single-channel attenuators |
US6489399B1 (en) | 2000-07-31 | 2002-12-03 | Molecular Optoelectronics Corp. | Dye-appended polymers for broadband fiber optic devices |
US6611649B2 (en) | 2001-03-19 | 2003-08-26 | Molecular Optoelectronics Corporation | Variable optical attenuator with polarization maintaining fiber |
US6681073B2 (en) | 2001-03-19 | 2004-01-20 | Molecular Optoelectronics Corporation | Fiber optic power control systems and methods |
US6785461B2 (en) | 1998-08-25 | 2004-08-31 | Molecular Optoelectronics Corp. | Blockless fiber optic attenuators and attenuation systems employing dispersion tailored polymers |
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Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0254509A1 (en) * | 1986-07-22 | 1988-01-27 | BRITISH TELECOMMUNICATIONS public limited company | Wavelength sensitive optical devices |
US4927223A (en) * | 1987-07-17 | 1990-05-22 | Thomson-Csf | Optic fiber correlator |
Family Cites Families (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4557551A (en) * | 1983-09-28 | 1985-12-10 | Andrew Corporation | Non-linear optical fiber coupler and a method of making same |
US4778237A (en) * | 1984-06-07 | 1988-10-18 | The Board Of Trustees Of The Leland Stanford Junior University | Single-mode fiber optic saturable absorber |
CA1298113C (en) * | 1986-10-20 | 1992-03-31 | Nicholas John Doran | Optical device |
GB8728854D0 (en) * | 1987-12-10 | 1988-01-27 | British Telecomm | Optical device |
US4815817A (en) * | 1988-04-06 | 1989-03-28 | Raynet Corporation | D-shaped fiber |
IT1248844B (en) * | 1990-06-13 | 1995-01-30 | Telettra Spa | SYSTEM AND DEVICE FOR THE OPTICAL CONTROL OF THE COUPLING / DE-COUPLING BETWEEN DIELECTRIC WAVE GUIDES |
GB9119734D0 (en) * | 1991-09-16 | 1991-10-30 | British Telecomm | Optical grating device |
US5285508A (en) * | 1992-01-14 | 1994-02-08 | Pioneer Electronic Corporation | Optical wavelength converter |
DE4220135A1 (en) * | 1992-06-15 | 1993-12-16 | Bosch Gmbh Robert | Process for coupling photo elements to integrated optical circuits in polymer technology |
-
1993
- 1993-08-13 SE SE9302634A patent/SE514675C2/en not_active IP Right Cessation
-
1994
- 1994-08-15 AT AT94924436T patent/ATE197194T1/en not_active IP Right Cessation
- 1994-08-15 NZ NZ271160A patent/NZ271160A/en not_active IP Right Cessation
- 1994-08-15 KR KR1019950701418A patent/KR100326582B1/en not_active IP Right Cessation
- 1994-08-15 AU AU74701/94A patent/AU690574B2/en not_active Ceased
- 1994-08-15 JP JP50690495A patent/JP3718523B2/en not_active Expired - Lifetime
- 1994-08-15 DE DE69426190T patent/DE69426190T2/en not_active Expired - Lifetime
- 1994-08-15 EP EP94924436A patent/EP0664894B1/en not_active Expired - Lifetime
- 1994-08-15 WO PCT/SE1994/000745 patent/WO1995005617A1/en active IP Right Grant
- 1994-08-15 PT PT94924436T patent/PT664894E/en unknown
- 1994-08-15 ES ES94924436T patent/ES2151931T3/en not_active Expired - Lifetime
- 1994-08-15 US US08/416,718 patent/US5642453A/en not_active Expired - Lifetime
- 1994-08-15 CN CN94190599A patent/CN1047238C/en not_active Expired - Lifetime
- 1994-08-15 DK DK94924436T patent/DK0664894T3/en active
-
2000
- 2000-10-26 GR GR20000402332T patent/GR3034673T3/en not_active IP Right Cessation
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0254509A1 (en) * | 1986-07-22 | 1988-01-27 | BRITISH TELECOMMUNICATIONS public limited company | Wavelength sensitive optical devices |
US4927223A (en) * | 1987-07-17 | 1990-05-22 | Thomson-Csf | Optic fiber correlator |
Cited By (18)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1997021141A1 (en) * | 1995-12-01 | 1997-06-12 | The University Of Sydney | A method for inducing nonlinearities in active optical materials and apparatus for the use thereof |
KR20010041065A (en) * | 1998-02-20 | 2001-05-15 | 케빈 알. 스튜어트 | Fiber optic attenuators and attenuation systems |
US6370312B1 (en) | 1998-02-20 | 2002-04-09 | Molecular Optoelectronics Corporation | Fiber optic attenuation systems, methods of fabrication thereof and methods of attenuation using the same |
US6335998B2 (en) | 1998-08-25 | 2002-01-01 | Molecular Optoelectronics Corporation | Blockless fiber optic attenuators and attenuation systems employing dispersion tailored polymers |
US6205280B1 (en) | 1998-08-25 | 2001-03-20 | Molecular Optoelectronics Corporation | Blockless fiber optic attenuators and attenuation systems employing dispersion controlled polymers |
US6268435B1 (en) | 1998-08-25 | 2001-07-31 | Molecular Optoelectronics Corporation | Dispersion-controlled polymers for broadband fiber optic devices |
US6303695B1 (en) | 1998-08-25 | 2001-10-16 | Molecular Optoelectronics Corporation | Dispersion-controlled polymers for broadband fiber optic devices |
US6191224B1 (en) | 1998-08-25 | 2001-02-20 | Molecular Optoelectronics Corporation | Dispersion-controlled polymers for broadband fiber optic devices |
US6785461B2 (en) | 1998-08-25 | 2004-08-31 | Molecular Optoelectronics Corp. | Blockless fiber optic attenuators and attenuation systems employing dispersion tailored polymers |
US6444756B2 (en) | 1998-08-25 | 2002-09-03 | Molecular Optoelectronics Corporation | Dispersion-controlled polymers for broad band fiber optic devices |
WO2000049434A1 (en) * | 1999-02-19 | 2000-08-24 | Protodel International Limited | Optical fibre attenuator and method of attenuating light transmitted through an optical fibre |
US6301426B1 (en) | 1999-03-16 | 2001-10-09 | Molecular Optoelectronics Corporation | Mechanically adjustable fiber optic attenuator and method employing same |
US6483981B1 (en) | 2000-06-28 | 2002-11-19 | Molecular Optoelectronics Corp. | Single-channel attenuators |
US6489399B1 (en) | 2000-07-31 | 2002-12-03 | Molecular Optoelectronics Corp. | Dye-appended polymers for broadband fiber optic devices |
WO2002052312A1 (en) * | 2000-12-26 | 2002-07-04 | Ion Beam Services | Optically active waveguide device comprising a channel on an optical substrate |
US6611649B2 (en) | 2001-03-19 | 2003-08-26 | Molecular Optoelectronics Corporation | Variable optical attenuator with polarization maintaining fiber |
US6681073B2 (en) | 2001-03-19 | 2004-01-20 | Molecular Optoelectronics Corporation | Fiber optic power control systems and methods |
WO2010080352A3 (en) * | 2008-12-18 | 2011-03-24 | Corning Incorporated | Semiconductor core, integrated fibrous photovoltaic device |
Also Published As
Publication number | Publication date |
---|---|
SE9302634L (en) | 1995-02-14 |
DE69426190D1 (en) | 2000-11-30 |
PT664894E (en) | 2001-04-30 |
SE514675C2 (en) | 2001-04-02 |
CN1113394A (en) | 1995-12-13 |
JP3718523B2 (en) | 2005-11-24 |
EP0664894B1 (en) | 2000-10-25 |
CN1047238C (en) | 1999-12-08 |
GR3034673T3 (en) | 2001-01-31 |
AU690574B2 (en) | 1998-04-30 |
KR950703748A (en) | 1995-09-20 |
AU7470194A (en) | 1995-03-14 |
JPH08502607A (en) | 1996-03-19 |
DK0664894T3 (en) | 2000-11-20 |
SE9302634D0 (en) | 1993-08-13 |
ES2151931T3 (en) | 2001-01-16 |
DE69426190T2 (en) | 2001-03-22 |
ATE197194T1 (en) | 2000-11-15 |
EP0664894A1 (en) | 1995-08-02 |
US5642453A (en) | 1997-06-24 |
NZ271160A (en) | 1998-02-26 |
KR100326582B1 (en) | 2002-07-27 |
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