All-optical signal processing method and device

Abstract

A device for processing of an optical input signal includes at least a first data signal. A first optical resonator provides a reference signal by optical filtering of the optical input signal. The first optical resonator is matched with a predetermined reference wavelength of the first data signal. A second optical resonator provides a sideband signal by optical filtering of the optical input signal. The second optical resonator is non-matched with the predetermined reference wavelength of the first data signal. An optical combiner combines the sideband signal with the reference signal to form an optical output signal.

Description

FIELD OF THE INVENTION

The present invention relates to optical signal processing.

BACKGROUND OF THE INVENTION

Signals have been traditionally processed in the electrical domain. However, conversion of optical signals to electrical signals is non-trivial at high modulation frequencies. Optical processing of optical signals provides an efficient and cost-effective approach at high modulation frequencies, e.g. when the modulation frequency is in the order of 40 GHz or higher.

Optical signal processing may be used e.g. for the recovery of clock frequency from an optical data signal.

The article “Optical Tank Circuits Used for All-Optical Timing Recovery”, by M. Jinno and T. Matsumoto, IEEE Journal of Quantum Electronics Vol. 28, No. 4 Apr. 1992, pp. 895-900, discloses a method for optical clock recovery. An optical clock signal synchronized to an incoming data stream is generated by extracting line spectral components in the incoming data stream using an optical resonator whose free spectral range is equal to the incoming data bit rate.

SUMMARY OF THE INVENTION

The object of the invention is to provide an optical signal processing device and an optical signal processing method.

According to an aspect of the invention, there is a method to process an optical input signal comprising at least a first data signal, said method comprising:

• • optical filtering of said optical input signal by using a first optical resonator to provide a reference signal, said first optical resonator being substantially matched with a predetermined reference wavelength of said first data signal,
  • optical filtering of said optical input signal by using a second optical resonator to provide a sideband signal, said second optical resonator being substantially non-matched with said predetermined reference wavelength of said first data signal, and
  • optically combining said reference signal with said sideband signal to form an optical output signal.

An optical resonator is a device which has a capability to wavelength-selectively store optical energy carried at one or more wavelengths. Because the optical resonator has the capability to store optical energy, an optical output signal may be provided also during periods when no optical energy is coupled to the optical resonators.

When the optical input signal comprises several data signals, the method according to the present invention allows considerable freedom to select the spectral positions of the data signals and/or the clock frequencies of the data signals.

In an embodiment, the device and the method may be used to recover at least one clock frequency associated with the optical input signal.

BRIEF DESCRIPTION OF THE FIGURES

FIG. 1 shows a block diagram of an optical communication system,

FIG. 2 shows, by way of example, the spectral composition of an optical signal comprising two modulated data signals

FIG. 3 shows, by way of example, the spectral composition of a modulated optical signal having a completely suppressed sideband,

FIG. 4 shows, by way of example, the spectral composition of a modulated optical signal having a suppressed carrier component,

FIG. 5 shows, by way of example, a modulated optical signal having a completely suppressed carrier component,

FIG. 6 shows a block diagram of an optical signal processing device according to the present invention,

FIG. 7 shows schematically an optical resonator based on a cavity defined by reflectors,

FIG. 8 shows by way of example a return-to-zero modulated data signal consisting of a sequence of rectangular pulses, and a clock signal associated with said data signal,

FIG. 9 shows the frequency decomposition of the data signal according to FIG. 8,

FIG. 10 shows an optical data signal modulated according to FIG. 8,

FIG. 11 shows schematically filtering and combination of optical signals in the wavelength domain,

FIG. 12 shows by way of example a return-to-zero modulated optical input signal, the temporal evolution of a sideband signal and the temporal evolution of an output signal corresponding to said input signal,

FIG. 13 shows schematically an optical resonator based on a fiber optic grating,

FIG. 14 shows schematically an optical resonator based on two gratings,

FIG. 15 shows schematically an optical resonator based on a micro ring,

FIG. 16 shows schematically an optical resonator based on a plurality of optically coupled micro rings,

FIG. 17 shows a block diagram of an embodiment of the optical signal processing device, said device comprising a polarization controller to control the polarization of the optical input signal,

FIG. 18 shows a block diagram of an embodiment of the optical signal processing device, said device comprising pre-processing unit to generate further spectral components based on a primary signal,

FIG. 19 shows a block diagram of the pre-processing unit,

FIG. 20 shows a block diagram of an embodiment of the optical signal processing device, said device comprising an output stabilization unit,

FIG. 21 shows, by way of example, an output signal which is stabilized with respect to the beat amplitude,

FIG. 22 shows schematically processing of an optical signal consisting of three modulated data signals,

FIG. 23 shows a block diagram of an embodiment of the optical signal processing device comprising a wavelength demultiplexer,

FIG. 24 shows a block diagram of a communication system comprising means to transmit control information to an optical transmitter, and

FIG. 25 shows, by way of example, an optical combiner implemented on a substrate using periodic structures.

DETAILED DESCRIPTION OF THE INVENTION

Referring to FIG. 1, an optical communication system 300 comprises an optical transmitter 200, an optical receiver 280 and an optical transmission path 240. The optical transmission path 240 may be e.g. an optical fiber. The optical signal B_IN sent by the transmitter 200 is carried through the transmission path 240. The modulation of the optical signal B_IN is controlled by a clock signal S_CLK,0 provided by a clock 220. The optical communication system 300 may comprise a splitter 260 to divide the optical signal B_IN into parts. The clock 220 may be a part of the transmitter 200. In case of multi-channel transmission, the clock signal S_CLK,0 may consist of several signals having different frequencies.

The optical signal B_IN may be processed using optical signal processing device 100 according to the present invention.

Advantageously, the optical signal processing device 100 according to the present invention is used to recover at least one clock signal S_CLK associated with the optical signal B_IN. The receiver 280 may be synchronized with the optical signal B_IN by using the recovered one or more clock signals S_CLK.

Referring to FIG. 2, an optical signal B_IN may consist of several modulated data signals B_IN,A, B_IN,B.

Modulation of a signal generates one or more spectral sidebands. Typically, a modulated data signal exhibits of a spectral component at a carrier wavelength and two spectral components at sideband wavelengths. For example a data signal modulated according to the return to zero (RZ) format exhibits a spectral composition belonging to this category.

However, the spectral component at the carrier wavelength may also be suppressed in order to save bandwidth and/or signal power.

Herein, in those cases when the spectral component at the carrier wavelength is not substantially suppressed, the term “reference wavelength” refers to the carrier wavelength of a modulated signal. In those cases when the spectral component at the carrier wavelength is substantially suppressed, the term “reference wavelength” refers to one of the sideband wavelengths.

“Sideband wavelength” refers to an other of the sideband wavelengths such that the sideband wavelength is different from the reference wavelength. Spectral components manifest themselves as spectral peaks in frequency plots.

In FIG. 2, the modulated data signal B_IN,A has a spectral component at the reference wavelength λ_0,A, and two sideband components at the wavelengths λ_−1,A, λ_1,A, on both sides of the reference wavelength λ_0,A. The wavelength λ_1,A may be selected to be the sideband wavelength.

Respectively, the modulated data signal B_IN,B has a spectral component at the reference wavelength λ_0,B, and two sideband components at the wavelengths λ_−1,B, λ_1,B on both sides of the reference wavelength λ_0,B. The wavelength λ_1,B may be selected to be the sideband wavelength.

The separation between the reference wavelengths λ_0,A and λ_0,B is ≢λ_AB. The separation between the sideband wavelength λ_1,A and the reference wavelength λ_0,A is ≢λ_A. The separation Δλ_A depends on the modulation frequency of the modulated data signal B_INA. The separation between the sideband wavelength λ_1,B and the reference wavelength λ_0,B is Δλ_B, respectively

Referring to FIG. 3, one or more of sideband components of the signal B_IN,A may be suppressed such that the modulated data signal has sidebands on only one side of the carrier component at the reference wavelength λ_0,B. In FIG. 3, the sideband component is at the wavelength λ_1,A.

Referring to FIG. 4, the signal B_IN,A may have at least two sideband components such that the carrier component is substantially suppressed. One of the sidebands components is now at the reference wavelength λ_0,A, and another is at the sideband wavelength λ_1,A. A signal modulated according to the carrier suppressed return to zero format (CSRZ) exhibits a spectral composition belonging to this category.

Referring to FIG. 5, the spectral component at the carrier wavelength may be completely suppressed.

FIG. 6 shows a block diagram of the signal processing device 100. An optical input signal B_IN is split into at least two parts by splitter 60. The parts are subsequently filtered by at least two optical resonators OR1, OR2. Mirrors M may be used to guide light. The splitter 60 may be a polarizing splitter or a non-polarizing splitter.

An optical resonator is a device which has a capability to wavelength-selectively store optical energy carried at one or more wavelengths. Because the optical resonator has the capability to store optical energy, it may provide an optical output signal also during periods when no optical energy is coupled into the resonator. The optical resonator may be matched with a predetermined wavelength, which means that one pass band of the optical resonator substantially coincides with said predetermined wavelength such that the optical resonator stores optical energy carried at said wavelength. The term non-matched means that the pass bands of the optical resonator do not coincide with said predetermined wavelength.

In FIG. 6, the first optical resonator OR1 is matched with a reference wavelength of the optical input signal B_IN and the second optical resonator OR2 is non-matched with the reference wavelength of the optical input signal B_IN. The first optical resonator OR1 provides a signal B_REF, which is herein called as the reference signal. The second optical resonator OR2 provides a signal B_SIDE, which is herein called as the sideband signal. The optical signals provided by the at least two resonators are combined by a combiner 80 to provide an output B_OUT.

The second optical resonator OR2 may be matched with the sideband wavelength. When the outputs of the first and the second optical resonators OR1, OR2 are combined by the combiner 80, the combined output exhibits B_OUT a beat at a frequency which depends on the difference between the sideband wavelength and the reference wavelength.

Referring to FIG. 7, the optical resonators OR1, OR2 may be implemented using an optical cavity 7 defined between two reflectors 5, 6. The optical length of the cavity 7 is L. The optical length L is equal to the distance between the reflectors 5, 6 multiplied by the refractive index of the cavity medium. The resonators OR1, and OR2 act as band pass filters having a plurality of pass bands (see the second curve from the top in FIG. 4). The reflectors 5, 6 may be e.g. planar or spherical reflective surfaces. In case of planar reflective surfaces, adjacent pass bands in the vicinity of a wavelength λ are separated by a separation range Δλ_SR given by $\begin{array}{cc}{\mathrm{\Delta \lambda }}_{\mathrm{SR}}=\frac{{\lambda }^2}{2L}.& \left(1\right)\end{array}$

Optical wavelength λ in vacuum and optical frequency ν are coupled by the equation λ=c/nλ, where c is the speed of light in vacuum and n is the index of refraction. The separation range Δν_SR may also be expressed in the frequency domain: $\begin{array}{cc}\Delta v_{\mathrm{SR}}=\frac{c}{2L}.& \left(2\right)\end{array}$

The separation range Δλ_SR may be substantially constant over a predetermined wavelength range. In order to implement a constant separation range, the cavity 7 may be non-dispersive. Alternatively, the resonators OR1 and/or OR2 may comprise further elements to compensate dispersion. On the other hand, the resonator OR1 and/or OR2 may also be dispersive to provide a varying separation range Δλ_SR. Such a resonator may be used e.g. in applications where the pass bands should coincide with several optical channels which have non-equal separations in the frequency domain.

Referring to the upper curve of FIG. 8, a data signal DATA may consist of a sequence of rectangular pulses. The data signal DATA shown in FIG. 8 is modulated according to the return-to-zero (RZ) format. t denotes time and A denotes amplitude. At this stage the data signal DATA may be an optical signal or it may be an electrical signal. The timing of the data pulses is controlled the clock pulses CLK, which are shown by the lower curve of FIG. 8. The time period between two consecutive clock pulses is T_CLK. The frequency ν_CLK of the clock is equal to 1/T_CLK, respectively.

FIG. 9 shows the frequency decomposition of the data signal DATA according to FIG. 8. ν denotes frequency. The ordinate and the abscissa values are shown in logarithmic scale. The frequency decomposition exhibits several distinctive spectral peaks ν_A, ν_B, ν_C, . . . In this case the spectral position of the peak ν_A is equal to the clock frequency ν_CLK associated with the data sequence according to FIG. 8.

FIG. 10 shows schematically an optical input signal B_IN. The optical input signal B_IN may be formed in the remote optical transmitter 200 (FIG. 1) by multiplying a continuous optical signal having wavelength λ₀ with the data signal DATA. The wavelength decomposition of the optical input signal B_IN exhibits a central component at the wavelength λ₀ and also sideband components according to FIG. 9.

The uppermost curve of FIG. 11 shows the spectral composition of the optical input signal B_IN in the wavelength domain. In this example the optical input signal B_IN consists of data transmitted at one optical channel only, i.e. is consists of only one data signal. The spectrum of the optical input signal B_IN exhibits a component at least at the reference wavelength λ₀ and at the sideband wavelength λ₁. There may also be further spectral components, such as the component at the wavelength λ₋₁. Also the wavelength λ₋₁ could be selected as the sideband wavelength, instead of the wavelength λ₁.

A data signal may have several sideband components. However, based on the known format of modulation, the person skilled in the art is able to select a sideband spectral component and a reference spectral component such that their spectral separation Δλ_A (=λ₁−λ₀) corresponds to the clock frequency of the data signal.

Referring to the second curve F1 from the top in FIG. 11, the spectral transmittance of the first optical resonator OR1 (FIG. 6) may have several adjacent pass bands PB. The separation of the pass bands PB is equal to the separation range Δλ_SR. One of the pass bands PB is tuned or set at least approximately to the reference wavelength λ₀. TR denotes the transmittance, i.e. the ratio of the transmitted intensity to the input intensity.

Referring to the third curve F2 from the top in FIG. 11, one of the pass band PB of the second resonator OR2 (FIG. 6) is tuned or set at least approximately to the sideband wavelength λ₁.

The pass bands PB may also be tuned simultaneously to the both sideband wavelengths λ₋₁ and λ₁, provided that the integer multiple of the separation range Δλ_SR of the second optical resonator OR2 (FIG. 6) is substantially equal to the separation between the sideband wavelengths λ₋₁ and λ₁.

Referring to the fourth curve from the top in FIG. 11, the spectral component at the reference wavelength is transmitted by the first optical resonator OR1 (FIG. 6) to provide the reference signal B_REF.

Referring to the fifth curve from the top in FIG. 11, the sideband of the input signal B_IN is transmitted by the second optical resonator OR2 (FIG. 6) to provide the sideband signal B_SIDE.

Referring to the lowermost curve in FIG. 11, the combined output of the optical resonators OR1, OR2 (FIG. 6) comprises the reference signal B_REF and the sideband signal B_SIDE.

The reference wavelength λ₀ corresponds to a reference frequency ν₀ which is equal to c/nλ₀. The sideband wavelength λ₁ corresponds to a sideband frequency ν₁ which is equal to c/nλ₁. The intensity of the output signal B_OUT exhibits now periodic variations, i.e. beat in a frequency which is equal to the difference between the sideband frequency ν₁ and the reference frequency ν₀. Thus, the output signal B_OUT may be used as an optical clock signal.

The electric field E_OUT of the optical output signal B_OUT is a superposition E_OUT(t)=E₁ exp(j2πν₁t)+E₀ exp(j2πν₀t),  (3) where E₁ is the amplitude of the field of the sideband signal B_SIDE after the combiner 80 (FIG. 6) and E₀ is the amplitude of the electric field of the reference signal B_REF after the combiner 80. The intensity I_OUT of the output signal B_OUT is given by I_OUT(t)∝E_OUT(t)E_OUT*(t)  (4) I_OUT(t)∝E₁²+E₀²+2E₁E₀ cos[2π(ν₁−ν₀)t].  (5) I_OUT(t)∝E₁²+E₀²+2E₁E₀ cos(2πσ_CLKt)  (6)

The output intensity exhibits a substantially sinusoidal beat at the frequency ν₁−ν₀, i.e. at the frequency ν_CLK of the clock. The last term in the equations (5) and (6) is herein called as the beating term.

The output signal B_OUT is a vector sum of the sideband signal B_SIDE and the reference signal B_REF. When the sideband signal B_SIDE and the reference signal B_REF are combined by the combiner 80, the polarization (i.e. the orientation of polarization) of the sideband signal B_SIDE may be at any angle with respect to the polarization of the reference signal B_REF. Parallel polarization provides maximum beating amplitude.

The orientation of the polarization of the reference signal B_REF and/or the sideband signal B_SIDE may be adjusted or set such that the polarization of the reference signal B_REF is parallel to the polarization of the sideband signal B_SIDE.

The relative contribution of the beating term may be maximized by setting the intensity of the reference signal B_REF to be approximately equal to the average intensity of the sideband signal B_SIDE, i.e. by setting E₁≈E₀.

The relative intensities of the reference signal B_REF and the sideband signal B_SIDE may be controlled e.g. by adjusting the angular orientation of a polarizer positioned in the optical path and/or by using an optical attenuator in combination with the first optical resonator OR1. The polarizer may be positioned before or after the optical resonator. One or more optical amplifiers may be used in combination with the resonators. The intensity of the reference signal B_REF and/or the sideband signal B_SIDE may be controlled by adjusting the amplification.

The optical resonator has a capability to store optical energy. This phenomenon is now discussed with reference to the resonator according to FIG. 7. However, the discussion is relevant also regarding other types of optical resonators. Photons coupled into the resonator according to FIG. 7 pass, in average, several times back and forth between the reflectors 5, 6 before escaping from the cavity 7. Thus, the resonator OR1 can sustain its state for some time regardless of perturbations of the optical input signal B_IN. The time constant τ of the optical resonator according to FIG. 7 is given by the equation $\begin{array}{cc}\tau =\frac{L}{-c\ln \left(r\right)},& \left(7\right)\end{array}$ where L is the optical length of the cavity 7 (physical distance multiplied by the refractive index) between the reflectors 5, 6, c is the speed of light in vacuum and r is the reflectance of the reflectors 5, 6. For example, by selecting the parameters r=0,99 and L=1 mm, the time constant τ of the resonator is 332 picoseconds.

The time constant τ may be selected to be greater than or equal to the average time period during which the optical input signal B_IN does not change its state.

The time constant τ may be selected to be greater than or equal to the average time period during which the optical input signal B_IN remains at zero.

FIG. 12 shows the temporal behavior of the sideband signal S_SIDE and the output signal B_OUT corresponding to a return-to-zero-modulated (RZ) input signal B_IN. The uppermost curve shows the input signal B_IN. The second curve from the top shows the temporal behavior of the reference signal B_REF. The intensity of the reference signal B_REF decreases when no optical energy is delivered to the first optical resonator OR1, i.e. the second optical resonator OR1 is discharged. The intensity of the sideband signal B_REF increases when optical energy is delivered to the first optical resonator OR1, i.e. the second optical resonator OR1 is charged. Referring to the third curve from the top in FIG. 12, the sideband signal B_SIDE exhibits similar type of fluctuations as the sideband signal B_REF.

The lowermost curve shows the temporal behavior of the output signal B_OUT. The output signal B_OUT exhibits a beat at a frequency corresponds to the difference between the reference wavelength and the sideband wavelength. It this case the reference wavelength and the sideband wavelength are selected such that the output signal B_OUT exhibits a beat at the clock frequency ν_CLK. The envelope ENV of the output signal B_OUT fluctuates according to the fluctuating signals B_SIDE, B_REF. It is emphasized that although the envelope ENV of the output signal intensity fluctuates, the amplitude of the beating of the output signal B_OUT approaches zero only if the input signal B_IN is at zero for a long time. Thus, the beating output signal B_OUT can be used as an uninterrupted clock signal.

The signal processing device 100 may further comprise an output stabilization unit to provide an output signal which is stabilized with respect to the beat amplitude, and reshaped (See FIGS. 20 and 21 and the related discussion).

The first optical resonator OR1 and/or the second optical resonator OR2 may be implemented using optical resonators known by the person skilled in the art. Suitable optical resonators are disclosed e.g. in an article “Optical Tank Circuits Used for All-Optical Timing Recovery” by M. Jinno, T. Matsumoto, IEEE Journal of Quantum Electronics, Vol. 28, No. 4 Apr. 1992 pp. 895-900.

Referring to the resonator shown in FIG. 7, the wavelength position of the pass bands PB of the first optical resonator OR1 and/or the second optical resonator OR2 may be set by adjusting the distance between the reflectors 5, 6. The setting may be also performed by other methods known by the person skilled in the art. The methods comprise e.g. controlling temperature, pressure, electric field, voltage, current, deformation of the cavity or displacement of the reflectors 5, 6.

An optical resonator may have active feedback means to tune the wavelength position of the pass bands PB. An optical resonator may be manufactured to provide the desired positions of the passbands PB. An optical resonator may be selected from among several resonators to provide the desired positions of the passbands PB. An optical resonator may have a replaceable component to implement the desired positions of the passbands PB.

Referring to FIG. 13, the first optical resonator OR1 and/or the second optical resonator OR2 may be implemented using a fiber optic grating. The grating comprises a portion of optical waveguide 8 comprising a plurality of periodic features 9.

Referring to FIG. 14, the first optical resonator OR1 and/or the second optical resonator OR2 may be implemented using two or more gratings, said gratings defining a cavity between them. The gratings may be Bragg gratings.

Referring to FIG. 15, the first optical resonator OR1 and/or the second optical resonator OR2 may be implemented using a micro ring resonator. Waveguides 11, 12 may be arranged to couple light in and out from a micro ring 13, said micro ring 13 forming an optical resonator. Light may be coupled to and from the waveguides and other optical components, such as the ring resonators 13, by evanescent coupling.

Referring to FIG. 16, the first optical resonator OR1 and/or the second optical resonator OR2 may be implemented using a plurality of optically coupled optical resonators, e.g. micro ring resonators.

The first optical resonator OR1 and/or the second resonator OR2 may also be implemented using a resonator formed based on a fiber loop or a portion of a fiber defined between two reflectors (not shown).

The first optical resonator OR1 and/or the second resonator OR2 may be based on a grating based device, a monochromator, an arrayed waveguide grating, a periodic microstructure, a stack of thin films, or a combination thereof.

The first optical resonator OR1 and/or the second resonator OR2 may comprise a cavity 7, which comprises gas, such air. The cavity 7 may comprise transparent solid or liquid. The cavity 7 may be a vacuum cavity. The resonators OR1, OR2 may e.g. comprise a pair of dielectric-coated mirrors separated by a gas air, such as air, or vacuum. The first optical resonator OR1 and/or the second resonator OR2 may be implemented using free-space optical components, integrated optics and/or fiber optical components. The first optical resonator OR1 and/or the second optical resonator OR2 may be used in the transmissive mode or in the reflective mode.

The first resonator OR1 and the second resonator OR2 may be implemented using a birefringent structure, e.g. a cavity 7 comprising birefringent medium. Thus, two different optical lengths may be implemented simultaneously using a single physical unit. The input signal B_IN may be divided into two parts having e.g. vertical and horizontal polarizations inside the birefringent resonator. The optical length of the cavity 7 corresponding to the vertical polarization may be adjusted to provide a pass band at the reference wavelength λ₀. The optical length of the cavity 7 corresponding to the horizontal polarization may be adjusted to provide a pass band at the sideband wavelength λ₁.

The birefringent medium may comprise liquid crystals. Thus, the optical properties of the medium may be controlled by applying an electric field over the medium.

The combiner 80 may be a semitransparent reflector, a beam splitter or a beam coupler based on fiber optics, an integrated optical Y-coupler, a directional coupler, a filter, a grating-based coupler, a polarizer PBS2 or a spatial multiplexer. The combiner 80 may also be a combination of these and/or related optical elements. The combiner may combine the signals at a ratio 50% to 50%.

Referring to FIG. 17, the signal processing device 100 may comprise a polarization controlling element 95. The polarization controlling element 95 may be adapted to select a portion of an optical primary input signal B_IN1 having a predetermined polarization, i.e. orientation of polarization. The polarization controlling element 95 is advantageously used when the optical primary signal B_{IN 1} is unstable or unknown. The polarization controlling element 95 may also be adapted to change the polarization of the primary signal B_IN1.

One or more polarization controlling elements 95 may be positioned before the first optical resonator OR1, between the first optical resonator OR1 and the combiner 80, or after the combiner 80.

One or more polarization controlling elements 95 may be positioned before the second optical resonator OR2, between the second optical resonator OR2 and the combiner 80, or after the combiner 80.

The splitter 60 may be a polarization controlling element 95. The combiner 80 may be a polarizing combiner PBS2.

The polarization controlling element 95 may be any type of polarizer or polarization controller known by the person skilled in the art. The polarization controlling element 95 may be a fiber-based polarization controller, a set of waveplates, a polarizing crystal, or a polarizing foil. The polarization controlling element 95 may comprise a combination of optical components.

Referring to FIG. 18, the signal processing device 100 may comprise a pre-processing unit 110.

Pre-processing of an optical primary input signal B_IN1 may comprise modifying the polarization, intensity, phase, and/or change of the reference wavelength. The pre-processing may be performed individually in a wavelength-dependent way for each optical data channel.

A primary optical input signal B_IN1 may be modulated in such a way that it does not originally comprise spectral components corresponding to the clock. Pre-processing of an optical primary input signal B_IN1 may comprise providing an optical input signal B_IN which comprises spectral components associated with the clock frequency of the primary optical input signal B_IN1. The primary optical input signal B_IN1 may be modulated e.g. according to the non-return-to-zero (NRZ) format.

Referring to FIG. 19, the pre-processing unit 110 may comprise a delay line to provide a delay signal by delaying said primary optical input signal, and an optical combiner to provide an exclusive-OR function of said delay signal and said primary optical input signal. Consequently, an optical input signal B_IN may be provided which comprises frequency components associated with the clock frequency. Such an arrangement is disclosed e.g. in an article “All-Optical Clock Recovery from NRZ Data of 10 Gb/s”, by H. K. Lee, J. T. Ahn, M.-Y. Jeon, K. H. Kim, D. S. Lim, C.-H. Lee, IEEE Photonics Technology Letters, Vol. 11 No.6 June 1999 pp. 730-732. The pre-processing unit 110 may also be implemented by non-linear devices such as disclosed e.g. in U.S. Pat. No. 5,339,185.

Referring to FIGS. 20 and 21, the signal processing device 100 may further comprise an output stabilization unit 85 to provide an output signal B_OUT,STAB which is stabilized and/or reshaped with respect with respect to the beat amplitude. The stabilization unit 85 may be based on an optical resonator exhibiting optical bistability. The stabilization unit 85 may be based on an optically saturable element. The stabilization unit 85 may be based on the use of one or more semiconductor optical amplifiers.

Referring to the uppermost curve in FIG. 22, the signal processing device 100 may be used to simultaneously recover clock frequencies of several modulated data signals B_IN,A, B_IN,B, B_IN,C. There are three reference wavelengths λ_0,A, λ_0,B and λ_0,C. The wavelengths λ_1,A, λ_1,B, and λ_1,C are selected as the sideband wavelengths. The spectral components at the wavelengths λ_−1,A, λ_{1, B} and λ_−1,C are not used. The sideband wavelengths λ_1,A, λ_1,B, and λ_1,C correspond to three different clock frequencies.

The second curve F2 of FIG. 22 shows the pass bands PB of the second resonator OR2. One of the pass bands is set at least approximately to the sideband wavelength λ_1,A, one of the pass bands is set at least approximately to the sideband wavelength λ_−1,B and one of the pass bands is set at least approximately to the sideband wavelength λ_1,C.

Referring to the lowermost curve F1 of FIG. 14, the passbands PB of the first optical resonator OR1 are adapted to match with the three reference wavelengths λ_0,A, λ_0,B and λ_0,C.

Combination of the transmitted sideband signal B_SIDE and transmitted reference signal B_REF provides an output signal B_OUT which is a superposition of the spectral components at the wavelengths λ_0,A, λ_0,Bλ_0,C, λ_0,A, λ_0,B and λ_0,C.

Referring to FIG. 23, the signal processing device 100 may comprise a spectral demultiplexer 120 to separate the spectral components associated with the different data signals. The demultiplexer may be based on a grating device, an arrayed waveguide grating, or further optical resonators. The output B_OUT,A of the demultiplexer exhibits beat at the clock frequency of the first data signal B_IN,A, the output B_OUT,B of the demultiplexer exhibits beat at the clock frequency of the first data signal B_IN,B, and the output B_OUT,C of the demultiplexer exhibits beat at the clock frequency of the first data signal B_IN,C.

The pass bands PB of the second optical resonator OR2 may be simultaneously adapted to correspond to a set of frequencies ν_q given by: ν_q=ν_0,A+qΔν_SR+ν_CLK,A,  (8) where q is an integer ( . . . −2, −1, 0, 1, 2, 3, . . . ), ν_0,A is the optical frequency (=c/nλ₀) corresponding to the reference wavelength λ₀ of a predetermined optical channel A, Δν_SR is the separation between the pass bands of the second resonator OR2 in the frequency domain and ν_CLK,A is the clock frequency.

Instead of the equation (8), the pass bands PB of the second optical resonator OR2 may be also be simultaneously adapted to correspond to a set of frequencies ν_q given by: ν_aq=ν_0,A+qΔν_SR−ν_CLK,A,  (9)

For example, the separation between the reference wavelengths may be 100 GHz, the separation range Δν_SR may be 50 GHz and the lowest clock frequency ν_CLK,A may be 10 GHz. In that case, according to the equation (8), the second optical resonator OR2 may be adapted to simultaneously filter frequencies ν_0,A−140 GHz ν_0,A−90 GHz, ν_0,A−40 GHz, ν_0,A+10 GHz, ν_0,A+60 GHz, ν_0,A+110 GHz, ν_0,A+160 GHz, ν_0,A+210 GHz . . . Consequently, several clock frequencies associated with different optical channels, i.e. associated with several reference wavelengths may be recovered simultaneously, providing that the sideband wavelentghs coincide with the pass bands of the second optical resonator OR2. An example of a possible combination of reference frequencies and clock frequencies is presented in Table 1.

TABLE 1
A example of a possible combination of reference frequencies,
clock frequencies and pass band positions.
			Positions of	Positions of
Data Signal	Reference	Clock	2nd resonator	1st resonator
No.	frequency	frequency	passbands	passbands
1	ν0,A − 200	GHz	10 GHz	ν0,A − 190	GHz	ν0,A − 200	GHz
2	ν0,A	40 GHz	ν0,A − 40	GHz	ν0,A
13	ν0,A + 200	GHz	10 GHz	ν0,A + 210	GHz	ν0,A + 200	GHz
4	ν0,A + 1000	GHz	160 GHz	ν0,A + 1160	GHz	ν0,A + 1000	GHz

In multi-channel processing, the separation range Δλ_SR of the first optical resonator OR1 may be selected to be equal to an integer multiple of the separation range of the second optical resonator OR2.

The separation between adjacent reference wavelengths λ_0,A, λ_0,B may be selected to be substantially equal to the separation range Δλ_SR of the first resonator OR1 multiplied by an integer number.

The separation between adjacent reference wavelengths λ_0,A, λ_0,B may be selected to be substantially equal to the separation range Δλ_SR of the second resonator OR2 multiplied by an integer number.

It is emphasized that the separation between adjacent reference wavelengths λ_0,A, λ_0,B does not need not to correspond an integer multiple of the clock frequency. Thus, the method according to the present invention allows considerable freedom to select the spectral positions of the modulated data signals and/or the clock frequencies.

Referring to FIG. 24, an optical communication system may comprise:

• • means to provide control information related to the spectral position of at least one spectral component of the optical input signal B_IN with respect to the position of at least one pass band PB of the optical resonator OR1 or OR2,
  • means to send the control information to the optical transmitter 200, and
  • means to adjust the spectral position of said at least one spectral component based on said control information, preferably to match with said at least one pass band PB.

In general, the signal processing device 100 is understood to comprise optical paths between the optical components, said paths being implemented by free-space optical links, liquid or solid-state optical waveguides, and/or optical fibers. The optical paths and the optical components of the signal processing device 100 may be implemented using free-space optical components, integrated optics and/or fiber optical components. The signal processing device 100 may be implemented with methods of integrated optics on a solid-state substrate using miniaturized components. The spectral demultiplexer 120, the optical resonators 100, and further optical components may be integrated on the same substrate.

Referring to FIG. 25, also optical splitters or optical combiners may be implemented by microstructures.

The signal processing device 100 may further comprise light-amplifying means to amplify the input signal B_IN, the output signal B_OUT, the sideband signal B_SIDE and/or the reference signal B_REF. The light amplifying means may be implemented by e.g. rare-earth doped materials or waveguides. The light amplifying means may be a semiconductor optical amplifier.

The signal processing device 100 may be used in combination with optical data receivers, repeaters, transponders or other type of devices used in fiber optic networks. The signal processing device 100 may be used in combination with optical data receivers, repeaters, transponders or other type of devices used in optical communications systems operating in free air or in space.

The optical input signal B_IN or the optical primary input signal B_IN1 may comprise data sent at several optical channels, i.e. associated with different reference wavelengths.

Wavelengths for optical channels in fiber optic networks have been standardized e.g. by the International Telecommunication Union within the United Nations System. The separation between two reference wavelengths (λ_0,A, λ_0,B) may be e.g. 100 GHz in the frequency domain.

The signal processing device 100 and the method according to the present invention may be used to process simultaneously, i.e. parallel in time domain, a plurality of optical signals having different reference wavelengths and/or data rates and/or different formats of modulation.

The optical input signal coupled to the signal processing device may be amplitude-modulated, phase-modulated, quadrature-modulated or modulated according to a further format known by the person skilled in the art. The primary optical input signal may comprise several modulated data signals at different wavelengths, i.e. at different optical channels. The data signals may be modulated in different ways. The data rates associated with the different data signals may be different.

A data signal may also have other modulation frequencies than the clock frequency. Also the further frequencies may be processed by the first and the second optical resonators, and recovered by selecting at least two respective spectral components of said data signal. For example, a data signal may have a clock frequency 40 GHz, but it may also have modulation at a lower frequency 10 GHz. Also the lower frequency 10 GHz may be recovered, instead of the clock frequency 40 GHz. This type of sub-harmonic all-optical recovery may be used in synchronization of optical time division multiplexing (ODTM) systems.

For the person skilled in the art, it will be clear that modifications and variations of the optical signal processing devices and methods according to the present invention are perceivable. The particular embodiments described above with reference to the accompanying drawings and tables are illustrative only and not meant to limit the scope of the invention, which is defined by the appended claims.

Claims

1. A device for processing of an optical input signal, which optical input signal comprises at least a first data signal, said device comprising: a first optical resonator to provide a reference signal by optical filtering of said optical input signal, said first optical resonator being matched with a predetermined reference wavelength of said first data signal, a second optical resonator to provide a sideband signal by optical filtering of said optical input signal, said second optical resonator being non-matched with said predetermined reference wavelength of said first data signal, and an optical combiner to combine said sideband signal with said reference signal to form an optical output signal.

2. The device according to the claim 1, wherein said device is adapted to recover at least a first clock frequency associated with said first data signal, one pass band of said second optical resonator being substantially matched with a first spectral component of said optical input signal, which first spectral component is associated with the clock frequency of said first data signal.

3. The device according to the claim 2, wherein said device is adapted to recover a second clock frequency associated with a second data signal, one pass band of said second optical resonator being substantially matched with a second spectral component of said optical input signal, which second spectral component is associated with the clock frequency of the second data signal.

4. The device according to the claim 1, wherein said device further comprises a spectral demultiplexer to separate from said optical output signal spectral components associated with said first data signal.

5. The device according to the claim 1, wherein the time constant of said optical resonators is greater than or equal to an average time period during which said first data signal does not change its state.

6. The device according to the claim 1, wherein the wavelength position of at least one pass band of said second resonator is adjustable such that it may be adjusted to coincide with a sideband wavelength of said first data signal.

7. The device according to the claim 3, wherein the separation range of said second resonator is adapted such that the separation between the reference wavelength of the first data signal and the reference wavelength of a second data signal is substantially equal to the separation range of said second resonator multiplied by an integer number.

8. The device according to the claim 1, wherein said first and/or said second resonator comprises an optical cavity defined by at least two reflectors.

9. The device according to the claim 1, wherein said first and/or said second resonator is selected from the group of a micro ring resonator, a sphere resonator and a toroid resonator.

10. The device according to the claim 1, wherein said first and/or said second resonator comprises several optical resonators which are coupled together, preferably a series of micro ring resonators.

11. The device according to the claim 1, wherein said first and/or said second resonator comprises at least one periodic structure.

12. The device according to the claim 1, wherein said first and/or said second resonator comprises a closed optical loop to which light is coupled by evanescent coupling.

13. The device according to the claim 1, wherein said device comprises means to control the relative contribution of the reference signal with respect to the sideband signal.

14. The device according to the claim 1, wherein said device comprises means to control the polarization of the reference signal with respect to the polarization of the sideband signal.

15. The device according to the claim 1, wherein the polarization of the sideband signal is adapted to be substantially parallel to the polarization of the reference signal.

16. The device according to the claim 1, wherein the combiner is selected from the group of a semitransparent reflector, a bifurcated optical fiber element, an Y-coupler, a directional coupler, a filter, a grating based coupler, a polarizer and a spatial multiplexer.

17. The device according to the claim 1, wherein said device further comprises an output stabilization unit to provide an output signal which is stabilized with respect to the beat amplitude.

18. The device according to the claim 1, wherein said device further comprises an output stabilization unit to stabilize the waveform of the output signal.

19. The device according to the claim 18, wherein said intensity stabilizing unit comprises an optical resonator exhibiting optical bistability.

20. The device according to the claim 18, wherein said intensity stabilizing unit comprises an optically saturable element.

21. The device according to the claim 18, wherein said intensity stabilizing unit comprises a semiconductor optical amplifier.

22. The device according to the claim 1, wherein said device further comprises a polarization controlling element to control the polarization of the optical input signal, said polarization controlling element consisting of one or more components selected from the group of fiber-based polarization controller, set of waveplates, Wollaston prism, Glan-Focault polarizer, Nicol prism, Rochon prism, polarizer comprising dielectric coating, wire grid polarizer, polymer-based film polarizer, fiber transmitting single polarization mode only, and photonic crystal polarization separator.

23. The device according to the claim 1, wherein said device further comprises a pre-processing unit to generate one or more further spectral components based on an optical primary signal.

24. The device according to the claim 23, wherein said pre-processing unit is adapted to process an optical primary signal modulated according to the non-return-to-zero (NRZ) format.

25. The device according to the claim 23, wherein said pre-processing unit comprises: a delay line to provide a delay signal by delaying said primary signal, and an optical combiner to provide an exclusive-OR function of said delay signal and said primary signal.

26. A method for processing of an optical input signal, which optical input signal comprises at least a first data signal, said method comprising: optical filtering of said optical input signal by using a first optical resonator to provide a reference signal, said first optical resonator being substantially matched with a predetermined reference wavelength of said first data signal, optical filtering of said optical input signal by using a second optical resonator to provide a sideband signal, said second optical resonator being substantially non-matched with said predetermined reference wavelength of said first data signal, and optically combining said reference signal with said sideband signal to form an optical output signal.

27. The method according to the claim 26, wherein said method further comprises recovering at least a first clock frequency associated with said first data signal, one pass band of said second optical resonator being substantially matched with a first spectral component of said optical input signal, which first spectral component is associated with the clock frequency of the first data signal.

28. The method according to the claim 27, wherein said optical input signal further comprises a second data signal, said method further comprising recovering a second clock frequency associated with the second data signal, one pass band of said second optical resonator being substantially matched with a second spectral component of said optical input signal, which second spectral component is associated with the clock frequency of the second data signal.

29. The method according to the claim 26, wherein said method further comprises spectrally separating from said output signal spectral components associated with the first data signal.

30. The method according to the claim 26, wherein the time constant of the first optical resonator is greater than or equal to the average time period during which the state of said first data signal remains unchanged.

31. The method according to the claim 26 further comprising adjusting the position of at least one pass band of the second resonator such that it coincides with at least one sideband of said first data signal.

32. The method according to the claim 26, further comprising: monitoring the spectral position of the reference wavelength with respect to at least one pass band of the first optical resonator, sending control information to an optical transmitter, said transmitter being adapted to transmit the first data signal, said control information being based on said spectral position, and tuning the spectral position of the first data signal based on said control information.

33. The method according to the claim 26, wherein the spectral position of the reference wavelength is tuned such that it substantially coincides with said at least one pass band of the first optical resonator,

34. The method according to the claim 26, wherein said first data signal is amplitude modulated.

35. The method according to the claim 26, wherein said first data signal is phase-modulated.

36. The method according to the claim 26, wherein said first data signal is modulated according to the return-to-zero format.

37. The method according to the claim 26, wherein said method further comprises pre-processing of an optical primary signal to generate further frequencies.

38. The method according to the claim 37, wherein said primary signal comprises at least one data signal which is modulated according to the non-return-to-zero format, at least one of said further frequencies being associated with the clock frequency of the non-return-to-zero modulated data signal.

39. The method according to the claim 37, wherein said pre-processing comprises: providing a delay signal by delaying said primary signal, and providing an optical signal based on exclusive-OR function of said delay signal and said primary signal.

40. The method according to the claim 26, wherein said first data signal is modulated according to the carrier suppressed return-to-zero format

41. The method according to the claim 28, wherein the difference between the reference wavelength of the first data signal and the reference wavelength of the second data signal is substantially equal to the separation range of the second resonator multiplied by an integer number.

42. The method according to the claim 28, wherein the separation between the reference wavelength of the first data signal and the reference wavelength of the second data signal is selected according to a standard set for optical telecommunications channels in fiber optic networks by the International Telecommunication Union within the United Nations System.

43. The method according to the claim 28, wherein the separation between the reference wavelength of the first data signal and the reference wavelength of the second data signal substantially correspond to an integer multiple of the frequency 100 GHz in the frequency domain.

44. The method according to the claim 28, wherein the first data signal and the second data signal are modulated according to a different format.

45. The method according to the claim 28, wherein the first data signal and the second data signal have different clock frequencies.