JPWO2005083502A1 - Optical clock extraction apparatus and method - Google Patents

Abstract

An optical clock extraction device for obtaining an optical pulse having an oscillation frequency synchronized with a reference frequency of an incident signal light includes a saturable absorption region having a phase modulation effect and a gain region, and is applied to the saturable absorption region. A mode-locked semiconductor laser that can change the oscillation frequency that generates an optical pulse by the phase modulation effect based on voltage, and optically detects the synchronization shift between the reference frequency of signal light and the oscillation frequency of the output optical pulse of the mode-locked semiconductor laser. And an optical mixer section that obtains a phase error signal by synchronous detection, and a phase locked loop that negatively feeds back the phase error signal to the saturable absorption region.

Description

  The present invention relates to an apparatus for generating clock light used for optical communication, optical measurement, optical information signal processing, and the like. In particular, the present invention relates to an apparatus and method for generating an optical clock reference signal with low phase noise, and an optical timing pulse from an optical signal, which is independent of the polarization of the optical signal, has low jitter, and a relative The present invention relates to an optical clock extraction apparatus and method for generating or extracting an optical clock reference signal with low intensity noise (RIN) with high stability.

  A mode-locked semiconductor laser (MLLD) is relatively easy and stable, and can generate a clock pulse train having a pulse width on the order of picoseconds at an ultrafast repetition frequency of 10 to 160 GHz. It is an industrially important clock pulse light source as an optical signal processing light source, a measurement light source, and the like.

  When MLLD is used as such a clock pulse light source, a technique for stabilizing clock light without depending on the external reference signal source as well as a method for establishing synchronization with an external reference signal source such as an optical signal or an electric signal. In addition, techniques for reducing phase noise in synchronized clock signals are important.

  In MLLD, there is a phenomenon in which the pulse repetition frequency fluctuates randomly. This is called jitter. Jitter is considered to occur because the length of the optical resonator that determines the repetition frequency of the output optical pulse in MLLD fluctuates randomly. Looking in more detail, noise light generated in a region having an optical amplification function in MLLD randomly fluctuates the carrier density and refractive index in MLLD, and as a result, the effective optical resonator length changes randomly. It is considered a thing.

  Up to now, as a technique for establishing synchronization between the clock light output from the MLLD and an external reference signal source, particularly an optical signal, and a technique for reducing phase noise when regenerating the clock light from the optical signal, ( 1) An optical method that directly injects signal light into the MLLD and synchronizes it, that is, a method based on optical injection synchronization, and (2) a method that synchronizes the optical signal once converted into an electrical signal. Yes. The former method is an all-optical method because processing is performed with an optical signal as it is, and the latter method is an electric method because it is converted into an electric signal.

  For example, Japanese Patent Application Laid-Open No. 2-183236 discloses a configuration using a light injection locking technique in which signal light is directly injected into the MLLD to achieve synchronization. FIG. 1A shows an example of a configuration based on light injection locking.

  In the optical injection locking, the saturable absorption region and the gain region constituting the MLLD are forcibly modulated by the optical signal by injecting the optical signal to the MLLD 91 that passively generates the optical pulse, and the output pulse This is a technique for synchronizing in light. In the illustrated example, a band pass filter 92 is disposed at the output of the MLLD 91. In this case, the phase noise of the clock-extracted light reproduced from the MLLD generally does not become better than the phase noise of the incident optical signal and strongly depends on the optical signal that is an external signal source. Furthermore, since the MLLD itself has a polarization dependency, the phase noise strongly depends on the polarization state of the signal light incident on the MLLD in the light injection locking.

  FIG. 1B shows an example of the configuration of a technique for synchronizing an optical signal once converted into an electrical signal. In this method, a high-speed photoreceiver 93 composed of a high-speed PIN diode or the like is used, an optical signal is converted into an electric signal by the high-speed photoreceiver 93, and then an electric phase-locked loop (PLL) is applied to the electric signal. Used to synchronize.

  The PLL includes a phase comparator 94 such as an electric mixer that can handle high frequencies, a loop filter 95, and a voltage controlled oscillator (VCO) 96 that generates a frequency signal as an electrical signal corresponding to high frequencies. The phase comparator 94 compares the phase of the electric signal obtained by converting the input optical signal with the high-speed light receiver 93 and the signal from the VCO 96 to detect a frequency difference, and outputs a signal corresponding to the phase difference. To do. The signal corresponding to the phase difference is smoothed by the loop filter 95 and supplied to the VCO 96 as a control signal. The electrical high frequency signal output from the VCO 96 is fed back to the phase comparator 94 and added to the MLLD 98 via the high frequency amplifier 97 so that the MLLD 98 can be directly modulated. In this configuration, the output frequency of the VCO 96 matches the frequency of the optical signal after being converted into an electrical signal, whereby the optical signal input to the high-speed photodetector 93 and the output clock light from the MLLD 98 are Synchronization is established. In this configuration, the phase noise can be reduced by designing the loop filter that constitutes the PLL. The high-speed light receiver 93, the phase comparator 94, the loop filter 95, the VCO 96, and the high-frequency amplifier 97 constitute an electric control unit 99, that is, an electric high-frequency circuit part.

In a PLL optical clock extraction device using a high-frequency circuit such as an electric oscillator or VCO, a technique for reducing phase noise is disclosed in, for example, JB Georges et al., “Stable picosecond pulse generation at 46 GHz by modelocking of a semiconductor. laser operating in an optoelectronic phaselocked loop, "Electronics Letters, Vol. 30, No. 1, pp. 69-71, JP-A-8-340154, H. Ono et al.," Low jitter pulse train generation using a regeneratively mode-locked laser diode, "10th International Workshop on Femtosecond Technology, TP-5, pp. 154, Chiba, Japan, July 16-17, 2003.
JP-A-2-183236 JP-A-8-340154 JB Georges et al., "Stable picosecond pulse generation at 46GHz by modelocking of a semiconductor laser operating in an optoelectronic phaselocked loop," Electronics Letters, Vol. 30, No. 1, pp. 69-71 H. Ono et al., "Low jitter pulse train generation using a regeneratively mode-locked laser diode," 10th International Workshop on Femtosecond Technology, TP-5, pp. 154, Chiba, Japan, July 16-17, 2003

  In the method of establishing the synchronization between the signal light and the output clock light by the light injection synchronization, the synchronization can be achieved with a simple configuration, but the synchronization state varies depending on the polarization state of the optical signal, and can be obtained. There has been a problem that the phase noise of the clock light depends on the phase noise of the injected optical signal. The reason is that the light injection locking uses the effect that the saturable absorption region of the MLLD is optically modulated, so that the polarization state of the light oscillated by the MLLD and the polarization state of the incident light are not the same. This is because the modulation effect is not constant and stable clock light cannot be obtained. Further, the effect of stabilizing the frequency of the output clock light is not provided by the light injection locking itself.

  In the method of converting an optical signal into an electrical signal, synchronization fluctuation due to the polarization state of the optical signal does not occur, and the frequency in the output clock light is stabilized by the PLL, but in order to directly modulate the MLLD, Since a VCO using an electric circuit is used as a high-frequency reference signal source, there is a problem that it is impossible to follow an optical signal having a clock frequency of, for example, 40 GHz or more. Further, the conventional optical clock extraction device based on the electrical PLL system has a problem that it is difficult to integrate the optical clock extraction device itself into a quartz waveguide, a polymer optical waveguide (PLC), or the like. The reason is that the higher the frequency of the clock reference signal, the higher the price, power consumption, and heat generation of the high-frequency reference signal source constituting the PLL, and the more efficient the frequency of the clock reference signal is, for example, 40 GHz or more. This is because it is difficult to provide high-frequency wiring.

  SUMMARY OF THE INVENTION An object of the present invention is to provide an optical clock extraction device that can regenerate clock light that does not depend on the polarization of signal light that is a reference signal source, does not require an electric high-frequency circuit, and has low phase noise. That is.

  Another object of the present invention is to provide an optical clock extraction method that can regenerate clock light that does not depend on polarization of signal light that is a reference signal source, does not require an electric high-frequency circuit, and has low phase noise. Is to provide.

  An object of the present invention is an optical clock extraction device that obtains an optical pulse having an oscillation frequency synchronized with a reference frequency of incident signal light, comprising a saturable absorption region having a phase modulation effect and a gain region, A mode-locked semiconductor laser (MLLD) capable of changing an oscillation frequency for generating an optical pulse by a phase modulation effect based on a control voltage applied to the saturable absorption region, a reference frequency of signal light, and an output optical pulse of the MLLD Means for optically detecting the synchronization deviation of the oscillation frequency to obtain a phase error signal, and means for negatively feeding back the phase error signal to the saturable absorption region so as to form a phase locked loop, This is achieved by an optical clock extraction device that synchronizes the output light pulse of MLLD and signal light.

  Such an optical clock extraction device of the present invention typically has an optical self-feedback that directly injects at least part of an optical pulse output from one output end face from the MLLD from the other end face of the MLLD. Has a loop. In the present invention, by providing such an optical self-feedback loop, the MLLD is operated as an optical VCO, and phase noise in the optical VCO output is reduced.

  Another object of the present invention is to provide a saturable absorption region having a phase modulation effect and a gain region, and to change an oscillation frequency for generating an optical pulse by a phase modulation effect by a control voltage applied to the saturable absorption region. An optical clock extraction method for synchronizing the oscillation frequency of the output optical pulse from the MLLD with the reference frequency of the incident signal light, and optically detecting the synchronization deviation between the reference frequency of the signal light and the oscillation frequency of the output optical pulse. Synchronously detecting to obtain a phase error signal, and negatively feeding back the phase error signal to a region having a phase modulation effect to form a phase locked loop, and synchronizing the optical pulse and the incident signal light. This is achieved by an optical clock extraction method.

  According to the present invention, a phase-locked loop that does not require a high-frequency electric circuit such as an electric VCO can be constructed. As a result, downsizing, high speed, low power consumption, high integration, and operability are improved. An optical clock extractor is provided.

  According to the present invention, clock extraction can be performed without depending on the speed and polarization state of signal light. Further, other signal processing such as an optical 3R repeater and an optical DEMUX can be simultaneously performed by an optical mixer which is a phase comparator. In the present invention, for example, an optical gate switch capable of operating at high speed is used as the optical mixer. As this optical gate switch, an optical fiber type optical gate switch constructed with a polarization-independent SOA or a configuration independent of polarization. This is because phase comparison that does not depend on the polarization state of the signal light becomes possible. At this time, if the synchronization holding range of the negative feedback of the phase locked loop is appropriately designed by selecting the characteristics of the loop filter, specifically, the synchronization holding range can be made larger than the fluctuation due to the polarization dependence of the optical mixer. Thus, more stable clock extraction can be realized.

  Since the optical mixer is a high-speed optical gate switch, once synchronization is established, the optical mixer can perform signal processing at the optimal timing of the signal light and the clock light. Therefore, the optical mixer can be used simultaneously for optical 3R reproduction processing and optical DEMUX processing in addition to error signal generation.

  Furthermore, according to the present invention, optical clock extraction can be performed by PLL control in multiple stages.

It is a block diagram which shows the structure of the conventional optical clock extraction apparatus using optical injection synchronization which extracts the clock light synchronized with it from the optical signal. It is a block diagram which shows the structure of the conventional optical clock extraction apparatus using PLL which extracts the clock light synchronizing with it from the optical signal. It is a figure explaining the optical clock extraction method based on this invention which aims at reduction of the phase noise in pulse light using the optical VCO by MLLD which has a self-feedback loop. It is a block diagram explaining the optical clock extraction apparatus of Example 1 of this invention. 5 is a graph showing an RF spectrum in an optical PLL operation for reducing phase noise and an RF spectrum in a PLL operation without self-feedback in an optical VCO using an MLLD having a self-feedback loop. It is a figure which shows the sampling oscilloscope waveform at the time of the PLL oscillating operation without optical feedback, and the sampling oscilloscope waveform in the optical PLL operation | movement which aimed at the phase noise reduction in optical VCO using MLLD which has a self-feedback loop. It is a graph which shows the RF spectrum of the sideband which arises by a self-feedback loop. It is a block diagram which shows the optical clock extracting device of Example 2 which provided two MLLDs in which a wavelength differs in order to suppress a sideband spectrum in the circulation loop. It is a block diagram which shows the clock extraction apparatus of Example 3. It is a block diagram which shows the structure which suppresses a sideband spectrum using the wavelength conversion by CW (continuous wave) light. It is a block diagram which shows the structure which suppresses a sideband spectrum by the super continuum using an optical fiber. It is a block diagram which shows the structure which suppresses a sideband spectrum by arrange | positioning an optical filter in a surrounding loop. In Example 4, it is a block diagram which shows the structure which gave the phase comparison function to the optical gate part of the optical 3R repeater. FIG. 10 is a block diagram illustrating a configuration in which an electroabsorption modulator is used for a phase comparison unit in the fifth embodiment. FIG. 10 is a block diagram illustrating a configuration when PLL control is performed in multiple stages in Example 6.

  FIG. 2 is a diagram for explaining an optical clock extraction method according to the present invention. In the optical clock extraction method of the present invention, phase noise at the optical VCO frequency is reduced by using MLLD with a self-feedback loop configuration.

  The present invention includes a saturable absorption region having a phase modulation effect and a gain region, and an MLLD that can change an oscillation frequency generated by an optical pulse by a phase modulation effect by a control voltage applied to the saturable absorption region. Mode-locked semiconductor laser diode) is used. Then, when synchronizing the oscillation frequency of the output light pulse from the MLLD with the reference frequency of the incident signal light, optically synchronously detects a synchronization shift between the reference frequency of the signal light and the oscillation frequency of the output light pulse. Thus, the phase error signal of these signals is obtained, and the phase error signal is negatively fed back to the saturable absorption region of the MLLD to form a phase locked loop, and the optical pulse and the incident signal light are synchronized to extract the clock. Do. Here, the oscillation frequency of the output optical pulse corresponds to a repetition frequency as an optical pulse train.

  Since the refractive index of light in a semiconductor generally depends on the carrier density, the effective resonator length of the MLLD can be controlled via the carrier density. Thereby, the repetition frequency control of MLLD becomes possible, and MLLD can be used as a voltage / current controlled oscillator (VCO) that outputs an optical signal. However, in order to use the MLLD as the optical VCO, it is important to reduce the phase noise in the output clock light from the MLLD, that is, to reduce the jitter. Therefore, in the present invention, in order to use the MLLD as the optical VCO without requiring an electric high-frequency oscillator, as a technique for reducing the phase noise of the clock light from the MLLD, that is, reducing the jitter, as shown in FIG. A configuration is adopted in which an optical loop system is constructed in which a part of the clock light from the MLLD 100 is taken out and light is injected again into the same MLLD 100, and the clock light is self-feedbacked. In the figure, the optical signal portion is indicated by a thick line, and the electric signal portion is indicated by a thin line.

  By adjusting the optical path length so that the timing at which the clock light pulse is generated from the MLLD 100 and the timing at which the clock light pulse circulates in the optical loop and returns to the MLLD 100 is adjusted at the same time, The saturation phenomenon, that is, the gate operation becomes steep, and phase noise caused by randomness of absorption saturation and randomness of noise light in the gain region due to gain saturation is reduced. As a result, phase noise in the output clock light can be reduced, and the accuracy of the frequency of the clock light pulse train can be improved without using a method of forcibly modulating by applying an electrical high-frequency circuit.

  Further, in the present invention, in order to establish synchronization between the input signal light and the reproduction clock light, the external signal light and the reproduction clock light from the optical VCO using the MLLD 100 are converted into a semiconductor optical amplifier (SOA) or the like. The phase is compared between the external signal light and the reference signal of the optical VCO. The optical beat signal generated by the optical mixer 200 is a signal corresponding to the phase difference between the external signal light and the regenerated clock light, and this signal is converted into an electric signal by the light receiver 310 composed of a PIN diode or the like, and the loop filter It is smoothed by 320 and applied as a control voltage to the saturable region of the MLLD 100. As described above, in the present embodiment, the clock light synchronized with the external signal light can be obtained by adopting the configuration of the phase locked loop.

  In the present embodiment, among the basic components of the PLL, a portion that requires high-speed processing such as a phase comparison unit (mixer) and a voltage controlled oscillator (VCO) is optically configured, while a phase difference detection unit, A portion that performs sufficient processing with a low-speed response of the order of MHz, such as error amplification and loop filter, is electrically configured by an electric control unit 300 including a light receiver 310 and a loop filter 320. As described above, in order to suppress the frequency fluctuation caused by the amplified spontaneous emission (ASE) of the MLLD, a method of optically self-feedback looping the MLLD is introduced to significantly improve the frequency accuracy.

  As described above, according to the present embodiment, an optical clock extraction device that does not depend on the polarization state of external signal light can be realized by using an optical mixer that uses polarization-independent SOA or the like. Further, by combining the optical mixer and the phase comparator with an optical switch using nonlinear effects such as SOA and optical fiber, the operation speed can be measured. Furthermore, since the optical mixer section can have the function of optical identification signal processing at the same time, the optical phase comparison operation and the optical signal processing operations such as optical 3R regeneration and optical DEMUX can be performed simultaneously. In addition, the operation can be optimized.

  In the present embodiment, the electrical control unit is only a part that smoothes a signal corresponding to the phase difference with a loop filter, and a loop composed of a relatively low-speed PIN diode light receiver and an operational amplifier having a band on the order of MHz. It can consist of a filter. The electrical controller does not need to be a high frequency circuit, and this part can be configured as an integrated circuit (IC). Therefore, the electrical control unit can be downsized, highly integrated, and low in power consumption. As described above, the optical clock extraction device has a configuration in which components such as the MLLD, the SOA, the isolator, the PIN, and the IC circuit can be easily mounted on the PLC, and thus can be reduced in size.

  Furthermore, in this optical clock extraction device, the optical intensity of the clock light pulse that has circulated through the optical loop is adjusted by an amplifier, an attenuator, etc., arranged in a configuration for self-feedback by the optical loop system, and the optical loop length The timing can be adjusted by changing. Accordingly, the fundamental frequency of the clock optical pulse train generated from the MLLD can be variably controlled, and the amplifier, the attenuator, and the like can also be controlled as a PLL control circuit, so that a multi-stage PLL control circuit can be realized.

  Hereinafter, the present invention will be described in more detail based on examples.

[Example 1]
FIG. 3 shows an optical clock extraction apparatus having an optical VCO using MLLD with a self-feedback loop configuration, and reducing phase noise at the oscillation frequency of the optical VCO. The illustrated optical clock extraction apparatus includes an optical mixer and a loop filter together with an optical VCO, and an optical PLL is configured by the optical mixer, the optical VCO, and the loop filter.

  The MLLD 1 used as the optical VCO includes at least a gain region 2 and a saturable absorption region 3. The gain region 2 and the saturable absorption region 3 are separated from each other. A lens 4 and an isolator 5 are arranged close to each of both end faces of the MLLD 1. Then, in order to form an optical self-feedback loop in which a part of an optical pulse output from one output end face of the MLLD 1 is directly injected into the MLLD 1 from the other end face, an optical waveguide 6 that externally connects between both end faces. In the optical waveguide 6, an optical delay device 7, an optical amplifier 8, and an optical attenuator 9 are inserted. The optical delay device 7 is adjusted so that the timing at which the MLLD 1 generates an optical pulse and the timing at which the optical pulse circulates in the optical waveguide 6 and enters the other end face of the MLLD 1 are the same. With this configuration, the absorption saturation phenomenon that occurs in the saturable absorption region 3 constituting the MLLD 1, that is, the optical gate operation becomes steep, and phase noise caused by the randomness of the absorption saturation in the saturable absorption region 3 when an optical pulse is generated The phase noise in the output clock light is reduced, and the frequency accuracy of the regenerated clock light can be increased.

  In order to establish synchronization between the external signal light and the output clock light from the MLLD 1, that is, the reproduction clock light, an optical mixer (MIX) 10, an optical attenuator (ATT) 9, a balance detector 11, an error amplifier 12, a loop A filter 13 and a voltage adder 14 are provided. In the optical mixer 10, a part of the regenerated clock light extracted from the MLLD 1 and the external signal light enter the optical mixer 10, and the output light of the optical mixer 10 passes through one of the balance detectors 11 via the optical attenuator 9. The balance detector 11 detects the frequency difference between the oscillation frequency of the MLLD 1 that is the optical VCO and the reference frequency of the external signal light. A signal corresponding to the phase difference is amplified by the error amplifier 12, smoothed by the loop filter 13, and applied as a control voltage by the voltage adder 14 to the saturable region 3 of the MLLD 1 that is the optical VCO. As a result, the regenerated clock light synchronized with the external signal light is obtained from the MLLD 1.

  In the optical mixer 10, modulation according to the phase difference between the reference frequency of the external signal light and the oscillation frequency of the clock light from the MLLD 1 can be added to both the external signal light and the clock light. For example, if mutual gain modulation using SOA is used, intensity modulation corresponding to the phase difference between both external signal light and clock light can be added. When one of the intensity-modulated signals is converted into an electrical signal by one of the light receiving sections of the balance detector 11 having a low frequency characteristic on the order of several MHz, the high-speed external signal light and the clock light are DC voltage components. Since the intensity modulation component is output as an error signal component, the intensity modulation component can be separated.

  When the clock light or the external signal light is incident on the other light receiver of the balance detector 11 so that the DC voltage component is canceled, the DC voltage component is canceled and only the error signal can be extracted. This error signal is amplified by the error amplifier 12, and the high frequency component contained in the error signal is completely removed and smoothed by the loop filter 13, and the bias source modulation component is added to the saturable absorption region 3 which is the phase modulation region of the MLLD 1. Apply as At this time, if the voltage adder 14 applies a reverse bias to the saturable absorption region 3 so that the MLLD 1 passively generates pulsed light, stable optical PLL operation can be performed.

  FIG. 4 shows an optical VCO that uses an MLLD with a self-feedback loop configuration, and an RF spectrum in the optical PLL operation when the phase noise at the oscillation frequency is reduced, and a PLL operation in the absence of self-feedback. The RF spectrum of the case is shown. In FIG. 4, “self-feedback + light PLL” indicates a spectrum when the optical PLL is operated using self-feedback, and “photoelectric PLL only” indicates a spectrum when self-feedback is not used. When the jitter component is reduced by using self-feedback, a steep spectral peak is obtained, and when the jitter component is large without using self-feedback, the spectral peak broadens. Thus, it can be confirmed that the signal-to-noise ratio (SNR) in the frequency spectrum is improved and the peak is sharper when the self-feedback is used. FIG. 4 further illustrates an RF spectrum when the synchronization is electrically established and an RF spectrum when the synchronization is not established.

  FIG. 5 shows a waveform observed by the sampling oscilloscope of the regenerated clock light from the optical VCO using the MLLD with the above-described self-feedback loop configuration. The upper waveform 81 is a sampling waveform when asynchronous, that is, the optical PLL is not operating, the middle waveform 82 is a sampling waveform when the PLL is operated without self-feedback, and the lower waveform 83 is These are sampling waveforms when both the optical PLL and self-feedback are operated, that is, when the optical PLL is operated so as to reduce phase noise.

  In general, the sampling waveform appears to fluctuate as the jitter increases. However, the sampling waveform 83 when self-feedback is performed has the smallest fluctuation. This means that the effect of improving the SNR of the frequency spectrum is observed in the form of jitter reduction.

[Example 2: Sideband spectrum suppression and two-wavelength synchronous clock light generation]
In the configuration shown in the first embodiment, if the effect of self-feedback performed by self-injection on the MLLD that is an optical VCO becomes too large, a sideband spectrum that depends on the self-feedback loop length may occur. FIG. 6 shows an example of such a sideband RF spectrum, and shows a sideband caused by a self-feedback loop configuration. The sideband occurs because the wavelength corresponding to the frequency of the MLLD and the wavelength corresponding to the frequency determined by the self-feedback loop length are the same wavelength, so that a composite resonator is formed. In order to remove the sideband, it is important to make the wavelength of the optical pulse output from the MLLD 1 different from the wavelength of the optical pulse that circulates in the optical waveguide 6.

  FIG. 7 shows the configuration of the optical clock extraction apparatus according to the second embodiment, and shows a configuration in which two MLLDs having different wavelengths are inserted in the same loop to suppress the sideband spectrum. In the second embodiment, as shown in FIG. 7, two MLLD1 and MLLD100 having different wavelengths are provided in an optical loop, and MLLD1 is operated as an optical PLL, and a part of the output optical pulse is transferred to the other MLLD100. Inject light. Since the MLLD 1 outputs optical pulses having the same polarization, the light injection synchronization is stably generated in the MLLD 100 on the injection side. In this case as well, the optical delay device 7 is set so that the timing at which the clock light pulse is generated from the MLLD 1 and the timing at which the clock light pulse circulates in the optical waveguide and reaches the saturable absorption region of each MLLD are the same. When adjusted, the absorption saturation phenomenon (gate operation) becomes steep, and phase noise caused by the randomness of absorption saturation is reduced.

  At this time, if the optical filter 15 and the optical filter 150 that transmit only the optical pulse generated from each MLLD are inserted into the optical waveguide 6, the wavelength of the optical pulse output from the MLLD 1 and the optical waveguide 6 circulate. Since the wavelengths of the optical pulses injected again into the MLLD 1 are different, a synchronized optical pulse circulation can be created without generating a sideband spectrum.

  In this configuration, clock lights having different wavelengths are output from the MLLDs 1 and 100. The configuration capable of simultaneously obtaining clock light of two different wavelengths in this way is an optimum configuration as a clock light source used for optical signal processing that requires synchronized clock light of two wavelengths, such as an optical 3R repeater. is there.

[Example 3: Configuration in which wavelength converter is placed in self-feedback loop as sideband spectrum suppression]
In addition to the method shown in the second embodiment, the optical pulse output from the MLLD 1 is different from the wavelength of the optical pulse that circulates the optical waveguide 6 so that only the optical pulse having a specific wavelength does not resonate strongly. A method of inserting the wavelength conversion unit 16 into the waveguide 6 is also conceivable. The optical clock extraction device shown in FIG. 8 is the same as that shown in FIG. 3 except that an optical filter 15 is provided close to the emission end face of the MLLD 1 and a wavelength conversion unit 16 is provided in the optical waveguide 6. It is different in that it is inserted.

  FIG. 9A shows a CW (continuous wave) light source 17 that operates at a wavelength different from the oscillation wavelength of the MLLD 1 as the wavelength conversion unit 16 that suppresses the side mode spectrum, the recovered clock light from the MLLD 1, and the continuous light from the CW light source 17. Is provided with a wavelength converter 18 for inputting. The wavelength converter 18 includes an EA (electro-absorption) modulator that operates at high speed, an optical gate switch using SOA, and the like, and is inserted into the optical waveguide 6.

  FIG. 9B shows the wavelength converter 16 using wavelength conversion by supercontinuum using an optical fiber. In this configuration, the spectrum of the clock light from the MLLD 1 is broadened by a non-linear effect between the optical amplifier 8 and the supercontinuum element (SC) 19 such as an optical fiber or a photonic crystal, and a part thereof is cut out by the optical filter 15. In this way, wavelength conversion is performed. In the figure, the SC spectrum is an output spectrum from the supercontinuum element 19, and the seed corresponds to the spectrum position of the clock light before expansion. At this time, if the band of the optical filter 15 is increased and the optical pulse output from the wavelength conversion unit 16 is compressed so as to shorten the pulse width, the MLLD absorption saturation phenomenon (gate operation) becomes steeper. Therefore, phase noise caused by randomness of absorption saturation can be further reduced.

  In FIG. 9C, as the simplest configuration, a part of the optical spectrum is cut out from the clock light from the MLLD 1 by the narrow-band optical filter 15, so that the optical pulse of the MLLD 1 and the optical pulse that circulates in the self-feedback loop. With such a configuration in which the center wavelength and the band wavelength range are different, such a configuration can suppress the composite resonance effect, and the same effect as when the wavelength is changed can be obtained.

[Embodiment 4: Configuration in which optical gate portion of optical 3R repeater has phase comparison function]
In the present invention, the optical mixer includes, in addition to the SOA, for example, a polarization-separated symmetric Mach-Zender interferometer (hereinafter referred to as PD-SMZ), a symmetric Mach-Zender interferometer (hereinafter referred to as SMZ), a nonlinear High-speed optical switches such as an optical loop mirror (NOLM), a terahertz optical asymmetric demultiplexer (TOAD), and a transmission type cross phase modulation (T-XPM) can be used. At the same time, optical gate switches such as PD-SMZ, SMZ, NOLM, TOAD, and T-XPM can simultaneously perform optical signal processing such as optical 3R regeneration and optical DEMUX.

  FIG. 10 shows a configuration when a phase comparison function is provided in the optical gate portion of the optical 3R repeater. An example in which the optical clock extraction according to the present invention is applied to the optical 3R repeater using the PD-SMZ 101 will be described with reference to FIG.

  The optical clock extraction unit has the same configuration as that described in the second embodiment, and generates two clock lights having different wavelengths and small phase noise. The PD-SMZ 101 includes a polarization controller 20, a calcite (polarizer) 21, an SOA (semiconductor optical amplifier) 22, an optical phase controller 23, and an optical filter 15. The clock light output from the MLLD 1 passes through the polarization controller 20, receives a time delay at the first calcite 21, is separated into two polarization states, and enters the SOA 22. At this time, if the optical pulse of the signal light is adjusted to be incident on the SOA 22 so as to be within the delay time, the clock optical pulse that has received a time delay among the two separated optical pulses incident on the SOA 22. Only the phase is modulated. Further, the phase-modulated optical pulse and the non-phase-modulated optical pulse are passed through the second calcite 21 to cancel the time delay due to the first calcite 21. Thus, by causing interference between the two clock lights, the clock light that has been subjected to the logic optical gate operation can be obtained. The output light of the second calcite 21 reaches the optical filter 15 via the optical phase controller 23 and the polarization controller 20.

  The positive logic and negative logic at this time are controlled by the polarization plane of the polarization controller 20. In order to operate with positive logic, it is only necessary to adjust the interference condition of the PD-SMZ 101 so that only the optically gated clock light is transmitted through the polarization controller 20 only when phase modulation occurs.

  In this case, when the signal light and the clock light are not synchronized, the signal light pulse does not enter within the delay time, so that sufficient phase modulation is not performed and the interference condition is deviated. Will undergo strong intensity modulation. When the optical PLL is operated using the intensity modulation signal as an error signal and the clock extraction operation is performed, the conditions for the signal light and the clock light to be in a synchronized state are the same as the optimum conditions for the optical gate operation. This makes it possible to simultaneously perform clock extraction by the optical PLL and optimal operation of optical signal processing. In the second and subsequent stages, this optically gated optical signal and the clock light having different wavelengths shown in the second embodiment are incident on another PD-SMZ 102. Thereby, the signal processing of the optical 3R repeater can be completed.

  FIG. 10 describes an example in which the optically gated signal light is used as an error signal. As the error signal, the signal light directly output from the SOA or the clock light separated into two is used. Even in such a case, similar processing can be executed.

[Example 5: Optical PLL circuit using EA modulator as phase comparison]
FIG. 11 shows a configuration in which an electroabsorption modulator (EA modulator) 103 is used in the phase comparison unit (optical mixer unit). A saturable absorption modulator may be used instead of the EA modulator 103.

  A reverse bias voltage is applied to the EA modulator 103 via a bias T circuit 140. If the high-speed frequency signal can be extracted from the other terminal of the bias T circuit 140, when the clock light output from the MLLD 1 is incident on the EA modulator 103, the frequency component of the clock light is used. An electrical signal can be taken from that terminal of the bias T circuit 140. In this state, when external signal light is incident on the EA modulator 103, an error signal is superimposed on the electrical signal output from the bias T circuit 140. When the frequency of the error signal is amplified by the error amplifier 113 constituted by a low-speed operational amplifier or the like, the high frequency component appears as a DC component signal, so that only the error signal can be separated and extracted. The DC component can be canceled if signal light or clock light is received by a low-speed light receiver 111 or the like and balanced by an adder 112 including an operational amplifier. The error signal thus extracted is smoothed by passing through the loop filter 13 and applied as a bias source to the saturable absorption region 3 of the MLLD 1 via the bias T circuit 140, thereby forming a phase locked loop. Thus, the signal light and the clock light can be synchronized.

[Example 6]
In the first to fifth embodiments described above, the method of feeding back an error signal to the saturable absorption region having the phase modulation effect in order to feed back the error signal to the MLLD 1 has been mainly described. As a method of constructing the phase locked loop, there is a method other than feeding back an error signal to the saturable absorption region. For example, (1) the loop length of the self-feedback is changed according to the error signal, (2) the intensity of light injected into the MLLD in the self-feedback is modulated according to the error signal, and (3) applied to the gain region 2 of the MLLD By using a method such as (4) PLL control by applying a voltage to the resonator length adjustment region 27 (see FIG. 12) newly provided in the MLLD, etc. The oscillation frequency of the MLLD 1 can be changed by the PLL control of the configuration.

  In the self-feedback of the MLLD 1, when the loop length is changed by the time delay unit 7 or the like so that the timing at which the MLLD 1 oscillates the optical pulse coincides with the timing at which the optical pulse that circulates the optical waveguide is again injected into the MLLD. The oscillation frequency of the MLLD 1 is dragged within a range of several hundred MHz to a frequency that is an integral multiple of the frequency determined by the loop length. This is because the light pulse intensity in the resonator that absorbs and saturates the saturable absorption region 3 plays an important role when the MLLD 1 oscillates by self-excited light pulse. This is because the pulse also plays a major role in the self-excited light pulse oscillation of the MLLD. For this reason, frequency modulation required for PLL control can be realized by changing the loop length of the self-feedback.

  The oscillation frequency of the MLLD 1 can be controlled by an effective resonator length. An effective resonator length can be achieved by changing the refractive index of light depending on the carrier density in the semiconductor constituting the MLLD 1. That is, the carrier density in the semiconductor can be controlled and the frequency can be changed by changing the intensity of the optical pulse injected by the optical amplifier 8 or the optical attenuator 9 in the loop and the injection current of the gain region 2. Is possible.

  In addition, when an MLLD with a resonator length control region 27 including a waveguide having a grating such as a DFB (distributed feedback) structure or a DBR (distributed Bragg reflector) or a passive waveguide is constructed, the resonance is also achieved. By controlling the voltage in the device length control region 27, the refractive index inside the MLLD can be changed, and the oscillation frequency of the MLLD can be controlled.

According to the inventor's experiment, when comparing the frequency variable bandwidth for each control method,
Saturable absorption region voltage control <light intensity control <loop length control ≦ gain region current control <resonator length adjustment region voltage control.

As shown in FIG. 12, loop filters 13, 25, 26, 28, and 29 that can effectively control such a frequency variable range are designed, and PLL control is performed on MLLD 1 in multiple stages to achieve a wide range of frequencies. Synchronization range and fine synchronization establishment can be realized.

Claims (16)

An optical clock extracting device for obtaining an optical pulse having an oscillation frequency synchronized with a reference frequency of incident signal light,
A mode-locked semiconductor laser comprising a saturable absorption region having a phase modulation effect and a gain region, and capable of changing an oscillation frequency for generating an optical pulse by a phase modulation effect based on a control voltage applied to the saturable absorption region When,
Means for optically synchronously detecting a synchronization shift between the reference frequency of the signal light and the oscillation frequency of the output light pulse of the mode-locked semiconductor laser to obtain a phase error signal;
Means for negatively feeding back the phase error signal to the saturable absorption region so as to form a phase locked loop;
Have
An optical clock extraction device for synchronizing an output light pulse of the mode-locked semiconductor laser and the signal light. An optical clock extracting device for obtaining an optical pulse having an oscillation frequency synchronized with a reference frequency of incident signal light,
A mode-locked semiconductor laser comprising a saturable absorption region having a phase modulation effect and a gain region, and capable of changing an oscillation frequency for generating an optical pulse by a phase modulation effect based on a control voltage applied to the saturable absorption region When,
An optical self-feedback loop for directly injecting at least part of a light pulse output from one output end face from the mode-locked semiconductor laser from the other end face of the mode-locked semiconductor laser;
Means for optically synchronously detecting a synchronization shift between an oscillation frequency of an output light pulse output from the mode-locked semiconductor laser and a reference frequency of the signal light to obtain a phase error signal;
Means for negatively feeding back the phase error signal to the saturable absorption region so as to form a phase locked loop;
Have
An optical clock extraction device for synchronizing an output light pulse of the mode-locked semiconductor laser and the signal light. A mode-locked semiconductor laser comprising a saturable absorption region and a gain region that are electrode-separated from each other and capable of changing an oscillation frequency for generating an optical pulse by a control voltage;
When the incident signal light is synchronized using a frequency close to the repetition frequency of the mode-locked semiconductor laser as a reference signal, the phase error between the incident signal light and the optical pulse is optically detected and a synchronization error signal is optically generated. An optical mixer section to
A light receiving unit that converts the synchronization error signal into a phase error signal that is a voltage signal;
A loop filter for negative feedback of the phase error signal;
Based on the phase error signal that is negatively fed back through the loop filter, the synchronization deviation of the repetition frequency and phase of the output light pulse from the mode-locked semiconductor laser with respect to the repetition frequency and phase of the incident signal light is minimized. And a phase-locked loop for controlling the voltage applied to the electrodes of the mode-locked semiconductor laser,
An optical clock extracting device having A first mode-locking semiconductor that includes a saturable absorption region and a gain region that are electrode-separated from each other, can change an oscillation frequency for generating an optical pulse by a control voltage, and oscillates an optical pulse of a first wavelength Laser,
A second mode-locked semiconductor laser comprising a saturable absorption region and a gain region that are electrode-separated from each other, and oscillating an optical pulse having a second wavelength different from that of the first mode-locked semiconductor laser;
At least a part of an optical pulse output from one output end face of the first mode-locked semiconductor laser is directly injected from one end face of the second mode-locked semiconductor laser, and the second mode-locked semiconductor An optical self-feedback loop for directly injecting a light pulse output from the other end face of the laser from the other end face of the first mode-locked semiconductor laser;
An optical delay provided in the self-feedback loop;
When the incident signal light is synchronized with a frequency close to the repetition frequency of the first mode-locked semiconductor laser as a reference signal, the phase error between the signal light and the optical pulse is optically detected, and a synchronization error signal is optically generated. An optical mixer section to
A light receiving unit that converts the synchronization error signal into a phase error signal that is a voltage signal;
A loop filter for negative feedback of the phase error signal;
Based on the phase error signal that is negatively fed back via the loop filter, the synchronization deviation of the repetition frequency and phase of the output light pulse from the first mode-locked semiconductor laser with respect to the repetition frequency and phase of the incident signal light is minimized. A phase-locked loop that controls the voltage applied to the electrodes of the first mode-locked semiconductor laser,
An optical clock extracting device having A mode-locked semiconductor laser comprising a saturable absorption region and a gain region that are electrode-separated from each other, the oscillation frequency for generating an optical pulse can be changed by a control voltage, and an optical pulse of a first wavelength is oscillated;
A light source that oscillates continuous light of a second wavelength different from the first wavelength;
A wavelength converter for transferring the light pulse of the first wavelength to the continuous light of the second wavelength and converting it into pulse light of the second wavelength;
An optical self-feedback loop for directly injecting the pulsed light of the second wavelength converted by the wavelength converter from the other end face of the first mode-locked semiconductor laser;
An optical delay provided in the self-feedback loop;
When synchronizing the incident signal light with a frequency close to the repetition frequency of the mode-locked semiconductor laser as a reference signal, the phase error between the incident signal light and the optical pulse of the first wavelength is optically detected, and the synchronization error signal is generated. An optically generated optical mixer section;
A light receiving unit that converts the synchronization error signal into a phase error signal that is a voltage signal;
A loop filter for negative feedback of the phase error signal;
Based on the phase error signal that is negatively fed back through the loop filter, the synchronization deviation of the repetition frequency and phase of the output light pulse from the mode-locked semiconductor laser with respect to the repetition frequency and phase of the incident signal light is minimized. And a phase-locked loop for controlling the voltage applied to the electrodes of the mode-locked semiconductor laser,
An optical clock extracting device having   An optical fiber that receives an optical pulse from the mode-locked semiconductor laser and broadens the spectral band of the incident optical pulse due to a non-linear effect, and cuts a part of the spectral band of the optical pulse output from the optical fiber to cut the mode 4. The light according to claim 1, further comprising: a filter that generates an optical pulse having a wavelength different from that of the synchronous semiconductor laser, and comprising a wavelength converter capable of compressing a time width of the optical pulse. Clock extraction device.   4. The device according to claim 1, further comprising a wavelength converter that includes an optical filter that cuts off a part of a spectral band of an optical pulse from the mode-locked semiconductor laser and generates an optical pulse having a wavelength different from that of the mode-locked semiconductor laser. 2. An optical clock extracting apparatus according to claim 1.   The optical clock extraction method according to claim 3, wherein the optical mixer section has an optical signal processing function.   The optical clock extraction method according to claim 8, wherein the optical signal processing function is an optical 3R reproduction function. A mode-locked semiconductor laser comprising a saturable absorption region having a phase modulation effect and a gain region, and capable of changing an oscillation frequency for generating an optical pulse by a phase modulation effect based on a control voltage applied to the saturable absorption region When,
A light absorption modulator that is used in optical signal processing and can generate a photocurrent by absorbing the optical signal;
An optical self-feedback loop for directly injecting at least part of a light pulse output from one output end face from the mode-locked semiconductor laser from the other end face of the mode-locked semiconductor laser;
When synchronizing the oscillation frequency of the output light pulse output from the mode-locked semiconductor laser with the reference frequency of the incident signal light, the output light pulse and the signal light are incident on the light absorption modulator. Means for optically detecting a synchronization error as a photocurrent and obtaining a phase error signal;
Means for negatively feeding back the phase error signal to the saturable absorption region so as to form a phase locked loop, and synchronizing the output light pulse and the signal light;
An optical clock extraction device.   The optical clock extraction method according to claim 10, wherein the optical absorption modulator has an optical 3R regeneration function. A saturable absorption region, a gain region, and a resonator adjustment region, which are separated from each other, are provided, and the oscillation frequency for generating an optical pulse can be changed by controlling the voltage or current applied to the electrodes in each region. A mode-locked semiconductor laser capable of
An optical self-feedback loop for directly injecting at least part of a light pulse output from one output end face from the mode-locked semiconductor laser from the other end face of the mode-locked semiconductor laser;
A pulse delay provided in the self-feedback loop;
An optical amplifier provided in the self-feedback loop;
An optical attenuator provided in the self-feedback loop;
When synchronizing the oscillation frequency of the output light pulse output from the mode-locked semiconductor laser with the reference frequency of the incident signal light,
Means for obtaining a phase error signal by optically synchronously detecting a synchronization shift between an oscillation frequency of an output light pulse output from the mode-locked semiconductor laser and a reference frequency of incident signal light;
The phase error signal is negatively fed back to at least one of the gain region, the resonator adjustment region, the pulse delay device, the optical amplifier, and the optical attenuator so that phase locked loop control is performed. Means for synchronizing the optical pulse with the signal light;
An optical clock extracting device having   The optical clock extraction device according to claim 12, comprising a plurality of phase-locked loops. A mode-locked semiconductor laser having a saturable absorption region having a phase modulation effect and a gain region, and capable of changing an oscillation frequency for generating an optical pulse by a phase modulation effect by a control voltage applied to the saturable absorption region An optical clock extraction method for synchronizing the oscillation frequency of the output optical pulse with the reference frequency of the incident signal light,
Obtaining a phase error signal by optically synchronously detecting a synchronization shift between the reference frequency of the signal light and the oscillation frequency of the output light pulse;
Negatively feeding back the phase error signal to the region having the phase modulation effect to form a phase locked loop, and synchronizing the optical pulse and the incident signal light;
An optical clock extraction method. A mode-locked semiconductor laser having a saturable absorption region having a phase modulation effect and a gain region, and capable of changing an oscillation frequency for generating an optical pulse by a phase modulation effect by a control voltage applied to the saturable absorption region An optical clock extraction method for synchronizing the oscillation frequency of the output optical pulse with the reference frequency of the incident signal light,
Injecting light directly from the other end face of the mode-locked semiconductor laser, at least part of a light pulse output from one output end face of the mode-locked semiconductor laser;
When synchronizing the oscillation frequency of the output light pulse from the mode-locked semiconductor laser with the reference frequency of the signal light, optically synchronous detection of a synchronization shift between the reference frequency of the signal light and the oscillation frequency of the output light pulse And obtaining a phase error signal,
Negatively feeding back the phase error signal to the saturable absorption region to form a phase locked loop, and synchronizing the output light pulse and the signal light;
An optical clock extraction method. The optical clock extraction method according to claim 14, wherein optical signal processing is executed simultaneously when optically detecting the synchronization deviation optically.

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