WO2001096913A1 - Light modulation in whispering-gallery-mode resonators - Google Patents
Light modulation in whispering-gallery-mode resonators Download PDFInfo
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- WO2001096913A1 WO2001096913A1 PCT/US2000/020952 US0020952W WO0196913A1 WO 2001096913 A1 WO2001096913 A1 WO 2001096913A1 US 0020952 W US0020952 W US 0020952W WO 0196913 A1 WO0196913 A1 WO 0196913A1
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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
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29331—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by evanescent wave coupling
- G02B6/29335—Evanescent coupling to a resonator cavity, i.e. between a waveguide mode and a resonant mode of the cavity
- G02B6/29338—Loop resonators
- G02B6/29343—Cascade of loop resonators
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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
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/12007—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind forming wavelength selective elements, e.g. multiplexer, demultiplexer
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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
- G02F1/01—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
- G02F1/011—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 in optical waveguides, not otherwise provided for in this subclass
-
- 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
- G02F1/3132—Digital deflection, i.e. optical switching in an optical waveguide structure of directional coupler type
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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
- G02F1/01—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
- G02F1/011—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 in optical waveguides, not otherwise provided for in this subclass
- G02F1/0115—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 in optical waveguides, not otherwise provided for in this subclass in optical fibres
- G02F1/0118—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 in optical waveguides, not otherwise provided for in this subclass in optical fibres by controlling the evanescent coupling of light from a fibre into an active, e.g. electro-optic, overlay
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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
- G02F1/01—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
- G02F1/03—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 ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
- G02F1/035—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 ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect in an optical waveguide structure
-
- 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
- G02F2203/00—Function characteristic
- G02F2203/15—Function characteristic involving resonance effects, e.g. resonantly enhanced interaction
Definitions
- This application relates to modulation of optical signals, and more specifically, to methods and devices for modulating an optical signal by using electro-optical modulators.
- Optical communication systems use one or more optical carrier waves to provide high-speed and wide bandwidth signal transmission.
- An optical carrier wave can be transmitted either through the free space or in an optical waveguiding channel such as a fiber link.
- the data capacity of a fiber link can be increased by using a wavelength-division multiplexing technique which simultaneously transmits optical carriers of different wavelengths over the same fiber so that different channels of data can be sent at the same time.
- Many other non- optical communication systems such as wired networks, radio wireless networks, satellite communication systems, can be combined with optical systems to meet various communication needs and requirements .
- the present techniques and devices for optical modulation include an electro-optic light modulators formed from gallery-whispering-mode resonators .
- a modulator includes a gallery- whispering-mode resonator formed of an electro- optical material, a first optical coupler to couple an input laser beam into the resonator, a second optical coupler to couple the optical energy out of the resonator to produce an optical output, and an electrical coupler to apply a. driving electrical signal.
- the optical energy from the input laser beam is coupled to into the resonator in one of the whispering gallery modes.
- the applied electrical signal modulates the dielectric constant of the resonator and hence the mode of the whispering gallery modes. This modulates the intensity of the output from the second optical coupler.
- One configuration of various forms of the gallery-whispering-mode resonator may be a disk-like resonator formed around an equator of a sphere.
- FIG. 1 shows one embodiment of an optical modulator based on a whispering-gallery-mode resonator made of an electro-optic material.
- FIG. 3A shows optical coupling by angle- polished waveguide or fiber.
- FIGS. 4, 5, and 6 show examples of RF electrodes for a disk-like whispering-gallery-mode resonator.
- FIG. 7 shows the mode spectrum of a whispering- gallery-mode sphere resonator obtained by tuning the input laser frequency.
- FIG. 8 illustrates the effect of applied RF field on the spectrum of optical whispering-gallery modes where intensity modulation is achieved at appropriately set input laser frequencies.
- An optical resonator uses an optical feedback mechanism to store optical energy only in certain resonator modes.
- An optical wave in a supported resonator mode circulates in the resonator.
- the optical resonator operates in resonance and optical energy accumulates inside the resonator and can be transmitted through the resonator with a minimum loss. If the optical is coupled out at this resonance condition, the output of the resonator is maximized.
- the recirculating wave in the resonator has a phase delay other then N2 ⁇ , the amount of optical energy accumulated in the resonator is reduced and, accordingly, the coupled output is also reduced from its maximum value.
- phase delay in the optical cavity can be modulated, a modulation on the output from an optical resonator can be achieved.
- the modulation on the phase delay of recirculating wave in the cavity is equivalent to a shift between a resonance condition and a non-resonance condition and can be between any two different values in the phase delay.
- the initial value of phase delay i.e. detuning from resonance
- optical coupling with the resonator may be implemented with waveguides or fibers for integration with other fiber optical elements or integrated electro-optical circuits formed on substrates.
- optical modulators may be used in a variety of applications having optical modulation, including optical communication and optical signal processing.
- a whispering-gallery-mode resonator may be formed from a transparent sphere made of a dielectric material. Other geometries based on a sphere are also possible, including a disk cavity or a ring cavity.
- Optical energy can be coupled into a resonator by evanescent coupling, e.g., using an optical coupler near the sphere by less than one wavelength of the optical radiation.
- Such resonators have a special set of resonator modes known as "whispering gallery modes". These modes represent fields confined in an interior region close to the surface of the sphere around its equator due to the internal reflection of the radiation. Microspheres with 10 micron or larger diameter have a resonator dimension much larger than the wavelength of light. Thus the loss due to the finite curvature of the resonator may be negligible.
- the resonators may be designed to have a high quality factor, Q, that are only limited with attenuation of radiation in the dielectric material and the surface imhomogeneities .
- Q quality factor
- Some microspheres have been shown to have very high quality factors for light waves, exceeding 10 9 for quartz microspheres. See, e.g., Braginsky V.B., Gorodetsky M.L., Ilchenko V.S, Phys.Lett. , Vol.137, p.393(1989) and Collot et al., Europhys . Lett., Vol. 23, p.327 (1993) .
- Such high Q values may allow concentration of strong fields in the whispering gallery modes .
- High-Q microsphere resonators have been used in a number of devices, including narrow band filters, lasers, laser stabilizers, and quantum nondemolition energy measurement devices.
- the use of droplet microcavities has also been recently made to demonstrate enhanced gain in such nonlinear optical processes as Raman and Rayleigh-wing scattering, as well as in four-wave parametric oscillation.
- dielectric microspheres of materials with an electro-optic effect for the modulation of optical radiation is proposed.
- the resonator modes and quality factor, Q, at a particular wavelength of radiation may be found by solving the following equations for the TM n , m , q (z) modes :
- n is the mode index
- z x-iy
- Q x/2y
- 8 is the dielectric constant of the sphere
- J n ⁇ /2 (z) and H nT ⁇ /2 (z) are respectively the Bessel and Hankel functions. See, e.g., an example description in Lin and Campillo, Phys . Rev. Lett., Vol.73, p.2440 (1994) .
- the equation for the TE n , m , q (z) modes is:
- either the sphere resonator alone or the sphere resonator in connection with a proper electrical strip line can form an electrical resonator to support electrical energy in the same whispering gallery modes with proper phase matching conditions.
- electrical and optical waves can coexist and co-propagate in certain whispering gallery modes.
- the electrical wave can be used to alter or modulate the dielectric constant of the sphere and hence modulate the light based on the electro-optic effects.
- Equations (1) and (2) is that for certain values of the dielectric constant ⁇ and the sphere radius R, whispering gallery modes with very high Q exist, for a given wave with wavelength ⁇ .
- FIG. 1 shows an optical modulator 100 with a whispering-gallery-mode resonator 110 according to one embodiment of the disclosure. Two optical couplers 121 and 122 are placed close to the resonator 110 as optical input coupler and output coupler, respectively.
- An input optical beam 104 e.g., a laser beam from a laser 102
- An input optical beam 104 is coupled into the resonator 110 as the internally-circulating optical wave 112 in the whispering gallery modes by the coupler 121.
- the coupling may be achieved through the evanescent coupling so that the couplers 121 and 122 are placed close to the resonator 110 by a spacing less than one wavelength of the beam 104.
- the evanescent fields at the surface of the sphere decays exponentially outside the sphere. Once coupled into the resonator, the light undergoes total internal reflections at the surface of the sphere. The effective optical path length is increased by such circulation.
- the output coupler 122 couples a portion of the circulating optical energy in the resonator 110, also through the evanescent coupling, to produce an output beam 124.
- the optical coupling may be implemented by using angle-polished fibers or waveguides 391 and 392 as shown in FIG. 3A.
- the angle-polished tip is placed near the resonator 310 to effectuate the evanescent coupling.
- the index of refraction of the fibers or waveguides 391 and 392 has to be greater than that of the resonator 310, and the optimal angle of the polish has to be chosen depending on the ratio of indices (V. S. Ilchenko, X.S.Yao, L.Maleki, Opt. Lett, Vol .24, 723 (1999) .
- An electrical coupler 130 is also disposed near the resonator 110 to couple an electrical wave which causes a change in the dielectric constant ⁇ due to the electro-optic effects.
- An electronic driving circuit 140 is coupled to supply the electrical wave to the electrical coupler 130.
- a control signal 150 can be fed into the circuit 140 to modulate the electrical wave. This modulation is then transfered to a modulation in the optical output 124 of the resonator 110.
- the resonator 110 may be formed from any electro-optic material such as lithium niobate.
- the whispering gallery modes essentially exist near the equator of the sphere, the resonator 110 may be not a whole sphere but a portion of the sphere near the equator that is sufficiently large to support the whispering gallery modes.
- rings, disks and other geometries formed from spheres may be used.
- FIG. 2A shows a disk-like whispering gallery mode resonator. It is formed from a sphere by removing top and bottom portions of the sphere to leave a portion containing the sphere equator 200.
- This embodiment of the resonator 110 includes a top circular surface 210 and a bottom circular surface 220, both with diameters less than the diameter of the original sphere.
- the side surface 230 may be a spherical surface.
- the spacing, d, between the top and bottom surfaces 210 and 220 is sufficiently large that the optical and electrical modes centered at the equator 200 remain essentially undisturbed by the geometry.
- a small spacing d can be used to achieve a sufficient electrical field strength for the electro-optic modulation at a low voltage, e.g., on the order of millivolts.
- the optic axis of the electro-optic material for the resonator 110 may be in any direction.
- FIG. 2B shows a disk configuration where the optic axis c (202) is different from the axis z (201) perpendicular to the equatorial circular plane.
- the optic axis c (202) may be aligned with the axis z (201) as in FIG. 2A.
- the optical modulator 100 in FIG. 1 may support rf (i.e. mm and microwave) signals, and light, simultaneously in a sphere of material with the electro-optic effect.
- rf i.e. mm and microwave
- Lithium niobate changes its real part of the index of refraction in response to the applied electric field.
- Other materials may respond to the electric field differently.
- Multiple quantum well structures of III-V compounds for example, change their imaginary part of the index of refraction when the electric field is applied.
- the applied electrical field can be arranged to change the speed of propagation of the optical field, which propagates in a thickness of only a few microns near the perimeter of the sphere around its equator.
- the rf mode field also occupies the same region, and owing to the relatively large Q of the mode, high electrical field values can be obtained at a small input RF power, to change the index of refraction by a significant amount.
- Q 10 7
- a change in the index less than a part per million is required. This is at least two orders of magnitude smaller than the fields required in many traveling-wave electro-optic modulators.
- Another approach for estimating the required half-wave voltage V ⁇ in comparing the microsphere to the traveling wave modulator is to consider the following.
- the electrical length of the microspherical resonator is on the order of few meters, compared to the centimeter long length of the traveling wave modulator, which requires a V ⁇ of a few volts. This implies that, for the microsphere, the interaction length is increased by a factor of about 10 2 to about 10 3 . This reduces the needed V ⁇ by the same factor. This increased efficiency will also be further improved with the electric field applied in the whispering gallery mode to allow a Q multiplication (by a factor of 10 4 ) of the energy density in the sphere. Even with the built-in inefficiency (on the order of 3 dB) associated with the coupling of the rf and light power, the modulator 100 shown in FIG. 1 can be orders of magnitude more efficient than those traveling wave modulators. In addition, in the case of materials with electro-absorption, where the electric field can best be applied directly, rather than in a whispering gallery mode, again many orders of magnitude in efficiency is expected.
- FIGS. 4, 5, and 6 show examples of the microstrip line electrode 350 when the resonator 310 is similar to the disk configuration shown in FIGS. 2A and 2B.
- the electrode 350 is formed on the top surface of the resonator 310 and the another electrode 410 is formed in contact with the bottom surface of the resonator 310.
- FIG. 5 shows a half-circuit microstrip line as the top electrode 350 on the rim of the top surface.
- FIG. 6 shows two pieces of circular microstrip lines 350A and 350B (solid lines) as the top electrode 350 and two pieces of circular microstrip lines 410A and 410B as bottom electrodes (dot liens with shades) .
- FIGS. 7 and 8 show measured data from the modulator 300 in FIG.
- the resonator 310 is a whole sphere.
- the electrodes are formed at the opposite poles of the sphere.
- a commercial-grade lithium niobate crystal (Casix Inc.) is used to form the disk-like resonator 310.
- the resonator is custom fabricated and polished.
- High-quality spheres are in general difficult to fabricate from crystalline materials via fusion as with amorphous materials. Upon fusion of crystalline materials, spontaneously forming boundaries between misoriented crystalline grains, or blocks, may create significant optical inhomogeneities through the bulk of the sphere and on the surface, thus increasing the scattering losses beyond the acceptable level.
- self- organized spheres of cubic (non-birefringent) crystalline material were reported. Because of their sub-grain few-micron size, they can be used to support WG modes of reasonable Q ⁇ 10 4 -10 5 .
- To obtain high-surface quality spheres of birefringent crystalline materials one method is to machine and polish them using conventional optical methods.
- a DFB laser at about 1550nm is used to produce the optical beam and is frequency- scannable via current modulation.
- the spectral data in FIG. 7 suggests that the employed prism coupling technique has a coupling efficiency about 50% in the loaded regime.
- the observed free spectral range (FSR) of about 8.3 GHz corresponds to the sequence of successive principal mode numbers 1 for TE-type WG modes excited in the plane perpendicular to the crystal axis.
- the estimated loaded quality-factor of the modes is about 1.2xl0 6 .
- the non-Lorentzian shape of the observed resonance dips in FIG. 7 indicates the presence of clusters of slightly non-degenerate modes. It is discovered that, the character of the observed spectrum appears to critically depend on the orientation of the crystal with respect to the normal direction of the equator plane. With the excitation off the perpendicular plane to the crystal axis, the observed spectrum became dense with a reduced linewidth. This increases the Q factor. This preliminary measurement confirms that inexpensive fabrication and polishing techniques can be used to achieve the Q factor in the spheres of crystalline lithium niobate that is close to the limits defined by the material attenuation.
- FIG. 8 shows the measured optical output power (curve 820) as a function of the laser frequency detuning for the input beam to the resonator.
- Curve 810 represents the corresponding optical whispering modes of the resonator.
- the intensity modulation in the curve 820 demonstrates the low-frequency electro-optical intensity modulation by the lithium niobate sphere.
- the above electro-optical modulator based on whispering-gallery-mode resonators generally has limited operating bandwidth, though operable to produce high modulation speeds, due to the resonance conditions and mode-matching requirement.
- Such modulators may be suitable for a number of applications where optical carrier is fixed, and the cavity spectrum can be trimmed to have optical modes at the carrier frequency and the modulation sidebands.
- this inconvenience will be compensated by two serious advantages over many other optical modulators.
- the controlling- voltage analog of the half-wave voltage V ⁇
- V ⁇ can be reduced into millivolt domain.
- tiny capacity of electro-optic microspheres can simplify application of microwave fields, compared to both plane-wave bulk electro- optical modulators and integrated Mach-Zender interferometer modulators .
Abstract
Description
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CA002412384A CA2412384C (en) | 2000-06-12 | 2000-08-01 | Light modulation in whispering-gallery-mode resonators |
AU2000275712A AU2000275712A1 (en) | 2000-06-12 | 2000-08-01 | Light modulation in whispering-gallery-mode resonators |
EP00964895A EP1301814A4 (en) | 2000-06-12 | 2000-08-01 | Light modulation in whispering-gallery-mode resonators |
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US09/591,866 US6473218B1 (en) | 1999-06-11 | 2000-06-12 | Light modulation in whispering-gallery-mode resonators |
US09/591,866 | 2000-06-12 |
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EP (1) | EP1301814A4 (en) |
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US7218662B1 (en) | 2004-02-12 | 2007-05-15 | Oewaves, Inc. | Coupled opto-electronic oscillators with low noise |
US7356214B2 (en) * | 2004-03-22 | 2008-04-08 | Oewaves, Inc. | Optical waveguide coupler for whispering-gallery-mode resonators |
US7266259B1 (en) | 2004-03-24 | 2007-09-04 | Fitel U.S.A. Corp. | Optical fiber microcoil, resonant structure and method of making the same |
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US7061335B2 (en) | 2004-04-15 | 2006-06-13 | Oewaves, Inc. | Processing of signals with regenerative opto-electronic circuits |
US7362927B1 (en) | 2004-06-01 | 2008-04-22 | Oewaves, Inc. | Tunable RF or microwave photonic filters using temperature-balanced whispering gallery mode optical resonators |
US7260279B2 (en) * | 2004-06-09 | 2007-08-21 | Oewaves, Inc. | Integrated opto-electronic oscillators |
US7480425B2 (en) * | 2004-06-09 | 2009-01-20 | Oewaves, Inc. | Integrated opto-electronic oscillators |
US7630417B1 (en) | 2004-06-24 | 2009-12-08 | California Institute Of Technology | Crystal whispering gallery mode optical resonators |
US7440651B1 (en) | 2004-11-17 | 2008-10-21 | California Institute Of Technology | Single mode whispering-gallery-mode resonator |
US7693419B1 (en) | 2005-11-23 | 2010-04-06 | General Photonics Corporation | Optical spectrum analysis using optical interferometry |
US7515786B1 (en) * | 2006-07-21 | 2009-04-07 | The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration | White-light whispering gallery mode optical resonator system and method |
US7634201B2 (en) * | 2006-09-05 | 2009-12-15 | Oewaves, Inc. | Wideband receiver based on photonics technology |
US8073326B2 (en) * | 2006-12-06 | 2011-12-06 | General Photonics Corporation | Optical polarization division multiplexing in optical communication |
US7723670B1 (en) | 2007-03-26 | 2010-05-25 | General Photonics Corporation | Optical differential group delay module with folded optical path |
US7952711B1 (en) | 2007-03-26 | 2011-05-31 | General Photonics Corporation | Waveplate analyzer based on multiple tunable optical polarization rotators |
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US7982944B2 (en) * | 2007-05-04 | 2011-07-19 | Max-Planck-Gesellschaft Zur Forderung Der Wissenschaften E.V. | Method and apparatus for optical frequency comb generation using a monolithic micro-resonator |
US8124927B2 (en) * | 2007-05-29 | 2012-02-28 | California Institute Of Technology | Detecting light in whispering-gallery-mode resonators |
WO2008153559A2 (en) * | 2007-05-29 | 2008-12-18 | California Institute Of Technology | Detecting light in whispering-gallery-mode resonators |
US7929589B1 (en) | 2007-06-13 | 2011-04-19 | Oewaves, Inc. | Diffractive grating coupled whispering gallery mode resonators |
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US7965745B2 (en) * | 2007-06-13 | 2011-06-21 | Oewaves, Inc. | RF and microwave receivers based on electro-optic optical whispering gallery mode resonators |
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US8164816B1 (en) | 2007-08-31 | 2012-04-24 | California Institute Of Technology | Stabilizing optical resonators |
US7715081B1 (en) | 2007-09-24 | 2010-05-11 | Lockheed Martin Corporation | Radio frequency photonic link with differential drive to an optical resonator electro-optic modulator |
US8210044B1 (en) | 2007-10-12 | 2012-07-03 | California Institute Of Technology | Covert laser remote sensing and vibrometry |
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US8155914B2 (en) | 2007-11-13 | 2012-04-10 | Oewaves, Inc. | Measuring phase noise in radio frequency, microwave or millimeter signals based on photonic delay |
US9360626B2 (en) | 2007-11-13 | 2016-06-07 | Anatoliy Savchenkov | Fiber-based multi-resonator optical filters |
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US7945130B2 (en) | 2007-11-15 | 2011-05-17 | General Photonics Corporation | Mode scrambling apparatus for multimode fiber |
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US8111722B1 (en) | 2008-03-03 | 2012-02-07 | Oewaves, Inc. | Low-noise RF oscillation and optical comb generation based on nonlinear optical resonator |
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US8089684B1 (en) | 2008-03-14 | 2012-01-03 | Oewaves, Inc. | Photonic RF and microwave phase shifters |
WO2009137202A2 (en) | 2008-04-03 | 2009-11-12 | California Institute Of Technology | Optical sensing based on overlapping optical modes in optical resonator sensors and interferometric sensors |
WO2009140075A1 (en) * | 2008-05-13 | 2009-11-19 | Lockheed Martin Corporation | Radio frequency photonic transceiver |
US8102597B1 (en) | 2008-05-15 | 2012-01-24 | Oewaves, Inc. | Structures and fabrication of whispering-gallery-mode resonators |
US8094359B1 (en) | 2008-05-15 | 2012-01-10 | Oewaves, Inc. | Electro-optic whispering-gallery-mode resonator devices |
US8452139B1 (en) | 2008-07-25 | 2013-05-28 | Oewaves, Inc. | Wide-band RF photonic receivers and other devices using two optical modes of different quality factors |
US8331008B1 (en) | 2008-10-14 | 2012-12-11 | Oewaves, Inc. | Photonic microwave and RF receivers based on electro-optic whispering-gallery-mode resonators |
US8159736B2 (en) * | 2008-11-13 | 2012-04-17 | Oewaves, Inc. | Tunable single sideband modulators based on electro-optic optical whispering gallery mode resonators and their applications |
US8761603B1 (en) | 2009-02-25 | 2014-06-24 | Oewaves, Inc. | Dynamically reconfigurable sensor arrays |
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US20100239245A1 (en) * | 2009-03-21 | 2010-09-23 | General Photonics Corporation | Polarization Mode Emulators and Polarization Mode Dispersion Compensators Based on Optical Polarization Rotators with Discrete Polarization States |
US8498539B1 (en) | 2009-04-21 | 2013-07-30 | Oewaves, Inc. | Dielectric photonic receivers and concentrators for radio frequency and microwave applications |
US8642111B2 (en) * | 2009-05-19 | 2014-02-04 | Polytechnic Institute Of New York University | Functionalizing a sensing ribbon on a whispering gallery mode microresonator using light force to fabricate a whispering gallery mode sensor |
US8355199B1 (en) | 2009-05-21 | 2013-01-15 | Lockheed Martin Corporation | Optical RF filter wavelength locked to laser with fixed offset frequency |
US8417076B2 (en) | 2009-06-22 | 2013-04-09 | Oewaves, Inc. | Tunable photonic microwave or radio frequency receivers based on electro-optic optical whispering gallery mode resonators |
US8681068B1 (en) | 2009-09-15 | 2014-03-25 | Lockheed Martin Corporation | Highly agile wideband cavity impedance matching |
US8331409B1 (en) | 2010-01-18 | 2012-12-11 | Oewaves, Inc. | Locking of a laser to an optical interferometer that is stabilized to a reference frequency |
US8564869B1 (en) | 2010-07-15 | 2013-10-22 | Oewaves, Inc. | Voltage controlled tunable single sideband modulators and devices based on electro-optic optical whispering gallery mode resonators |
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Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5581642A (en) * | 1994-09-09 | 1996-12-03 | Deacon Research | Optical frequency channel selection filter with electronically-controlled grating structures |
WO1998053535A1 (en) | 1997-05-20 | 1998-11-26 | Northwestern University | Semiconductor micro-resonator device |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CA2068899C (en) * | 1991-09-17 | 1997-06-17 | Samuel Leverte Mccall | Whispering mode micro-resonator |
US6009115A (en) * | 1995-05-25 | 1999-12-28 | Northwestern University | Semiconductor micro-resonator device |
JP2003517625A (en) * | 1998-12-07 | 2003-05-27 | カリフォルニア・インスティテュート・オブ・テクノロジー | Resonant type light energy control apparatus and method |
-
2000
- 2000-06-12 US US09/591,866 patent/US6473218B1/en not_active Expired - Lifetime
- 2000-08-01 CA CA002412384A patent/CA2412384C/en not_active Expired - Lifetime
- 2000-08-01 WO PCT/US2000/020952 patent/WO2001096913A1/en active Application Filing
- 2000-08-01 AU AU2000275712A patent/AU2000275712A1/en not_active Abandoned
- 2000-08-01 EP EP00964895A patent/EP1301814A4/en not_active Ceased
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5581642A (en) * | 1994-09-09 | 1996-12-03 | Deacon Research | Optical frequency channel selection filter with electronically-controlled grating structures |
WO1998053535A1 (en) | 1997-05-20 | 1998-11-26 | Northwestern University | Semiconductor micro-resonator device |
Non-Patent Citations (1)
Title |
---|
See also references of EP1301814A4 |
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US6879752B1 (en) | 2002-04-03 | 2005-04-12 | Oewaves, Inc. | Film spacer for setting the gap between an optical coupler and a whispering-gallery mode optical resonator |
WO2007112279A2 (en) * | 2006-03-27 | 2007-10-04 | Hewlett-Packard Development Company, L.P. | Resonators |
WO2007112279A3 (en) * | 2006-03-27 | 2007-12-13 | Hewlett Packard Development Co | Resonators |
US7729576B2 (en) | 2006-03-27 | 2010-06-01 | Hewlett-Packard Development Company, L.P. | Modulated signal resonators |
US8068706B2 (en) | 2006-12-29 | 2011-11-29 | Massachusetts Institute Of Technology | Fabrication-tolerant waveguides and resonators |
US7903909B2 (en) | 2007-10-22 | 2011-03-08 | Massachusetts Institute Of Technology | Low-loss bloch wave guiding in open structures and highly compact efficient waveguide-crossing arrays |
US8116603B2 (en) | 2007-10-22 | 2012-02-14 | Massachusetts Institute Of Technology | Low-loss Bloch wave guiding in open structures and highly compact efficient waveguide-crossing arrays |
WO2010138849A1 (en) * | 2009-05-29 | 2010-12-02 | Massachusetts Institute Of Technology | Cavity dynamics compensation in resonant optical modulators |
US8514400B2 (en) | 2010-03-23 | 2013-08-20 | Oewaves, Inc. | Optical gyroscope sensors based on optical whispering gallery mode resonators |
Also Published As
Publication number | Publication date |
---|---|
AU2000275712A1 (en) | 2001-12-24 |
EP1301814A1 (en) | 2003-04-16 |
CA2412384C (en) | 2007-07-03 |
CA2412384A1 (en) | 2001-12-20 |
EP1301814A4 (en) | 2006-03-29 |
US6473218B1 (en) | 2002-10-29 |
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