WO2006009269A1 - 周波数シフトキーイング復調器 - Google Patents
周波数シフトキーイング復調器 Download PDFInfo
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- WO2006009269A1 WO2006009269A1 PCT/JP2005/013534 JP2005013534W WO2006009269A1 WO 2006009269 A1 WO2006009269 A1 WO 2006009269A1 JP 2005013534 W JP2005013534 W JP 2005013534W WO 2006009269 A1 WO2006009269 A1 WO 2006009269A1
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- 230000002349 favourable effect Effects 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 2
- 230000000593 degrading effect Effects 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
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Classifications
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/50—Transmitters
- H04B10/501—Structural aspects
- H04B10/503—Laser transmitters
- H04B10/505—Laser transmitters using external modulation
- H04B10/5057—Laser transmitters using external modulation using a feedback signal generated by analysing the optical output
- H04B10/50577—Laser transmitters using external modulation using a feedback signal generated by analysing the optical output to control the phase of the modulating signal
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/21—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour by interference
- G02F1/225—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour by interference in an optical waveguide structure
- G02F1/2255—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour by interference in an optical waveguide structure controlled by a high-frequency electromagnetic component in an electric waveguide structure
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/50—Transmitters
- H04B10/501—Structural aspects
- H04B10/503—Laser transmitters
- H04B10/505—Laser transmitters using external modulation
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/50—Transmitters
- H04B10/501—Structural aspects
- H04B10/503—Laser transmitters
- H04B10/505—Laser transmitters using external modulation
- H04B10/5053—Laser transmitters using external modulation using a parallel, i.e. shunt, combination of modulators
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/50—Transmitters
- H04B10/501—Structural aspects
- H04B10/503—Laser transmitters
- H04B10/505—Laser transmitters using external modulation
- H04B10/5057—Laser transmitters using external modulation using a feedback signal generated by analysing the optical output
- H04B10/50575—Laser transmitters using external modulation using a feedback signal generated by analysing the optical output to control the modulator DC bias
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/21—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour by interference
- G02F1/212—Mach-Zehnder type
Definitions
- the present invention relates to a frequency shift keying demodulator and a frequency shift keying communication system using the same.
- Optical frequency shift keying is a technology that modulates the optical frequency and transmits the difference in frequency as a signal.
- FSK signals generally have no information on their amplitude, and are therefore less susceptible to level fluctuations and noise.
- FSK systems using digital signals are already known (see, for example, Japanese Patent Application Laid-Open No. 11_1-17746). However, this technology is about shifting the frequency of digital signals as far as possible, not shifting the frequency of light.
- Optical single sideband modulators optical SSB (Single Slide-Band) modulators
- optical SSB Single Slide-Band modulators
- Optical frequency using optical SSB modulator Shifter
- IEICE Technical Report TECHNICAL REPORT OF IEICE, OCS2002-49, PS2002-33, OFT2002-30 (2002-08)
- optical FSK modulators using this optical SSB modulator are known (See T. Kawanishi and M. Izutsu, Optical FSK modulator using an integrated 1 ight wave circuit consisting of four optical phase modulators, "CPT 2004 G-2, Tokyo, Japan, 14-16 Jan. 2004).
- FIG. 4 shows the basic configuration of an FSK communication system that includes such an optical FSK modulator.
- the conventional F SK communication system consists of an F SK demodulator (101) that demodulates an optical FS signal, an optical F SK modulator (111) that generates an optical F SK signal, an optical F It consists of an optical fiber (113) that connects the SK modulator and the F SK demodulator.
- the F SK demodulator is the demultiplexer (102), and the optical F SK
- the signal was divided into (US B signal ⁇ LSB signal), the intensity of each was measured by a photodetector, converted to an electrical signal, and the difference was taken by a subtractor (106).
- a dispersive medium such as an optical fiber (113)
- the US B signal and LSB signal differ in frequency by twice that of the modulated signal. Therefore, there is a time difference (delay) before reaching the photodetectors (104) and (105) (that is, the USB signal arrives at the photodetector earlier).
- 112 indicates a light source.
- Figure 5 is a conceptual diagram for representing such a delay. Due to this delay, there is a problem that the subtracter cannot properly take the difference in intensity between the US B signal and the LSB signal. Disclosure of the invention
- An object of the present invention is to provide a novel FSK demodulator that can be used for optical information communication and the like.
- Another object of the present invention is to provide an optical FSK communication system that can be used for optical information communication and the like and can transmit information at high speed.
- the present invention has found that when an optical FSK modulator is demodulated, a delay occurs between the US B signal and the LSB signal, and the FSK signal can be demodulated more appropriately by eliminating the delay. It is based on.
- a frequency shift keying (F SK) demodulator includes means (2) for demultiplexing an optical signal according to its wavelength, and the demultiplexer. Means (3) for adjusting the delay time of the two lights demultiplexed by the means, means (4) for detecting one optical signal demultiplexed by the demultiplexer, and demultiplexing by the demultiplexer Means (5) for detecting the remaining optical signal, and the first Means (6) for calculating a difference between the output signal of the first photodetector and the output signal of the second photodetector.
- F SK frequency shift keying
- the FSK demodulator of the present invention can be demodulated appropriately.
- the optical signal in the “means for demultiplexing the optical signal according to its wavelength” is an optical FSK signal
- the “optical signal as its wavelength” is the means for demultiplexing the upper sideband (US B) signal and the lower sideband (LSB) signal of the optical FSK signal.
- the "means (3) for adjusting the delay time of the two lights to be demultiplexed by the demultiplexer (3)" determines whether the optical signal depends on its wavelength.
- the light delay time is adjusted by adjusting the optical path length of one or both of the two lights demultiplexed by ".”
- there are two methods for adjusting the delay time adjusting the delay time in the light state and adjusting the delay time after using light as an electrical signal. Of these, the latter cannot be adjusted easily because the electric signal circuit system must be reset.
- the former is preferable because a delay time can be easily adjusted by changing the optical path length by preparing multiple mirrors and adjusting the mirror position.
- a preferred embodiment of the FSK demodulator according to the present invention is such that the “means (3) for adjusting the delay time of two lights to be demultiplexed by the demultiplexer” can change the delay time to be adjusted. is there.
- Such an FSK demodulator is preferable because the delay time can be adjusted according to changes in the modulation signal of the optical FSK modulator and the type and length of the dispersive medium.
- a more specific adjustment method is to change the optical path length by changing the mirror position.
- the “means for adjusting the delay time of two lights demultiplexed by the demultiplexer (3)” has a delay time of a predetermined time. To be adjusted. For example, only two types of modulation frequencies are used In some cases, it is not necessary to be able to adjust the delay time in an analog (continuous) manner. Therefore, a device that can adjust the delay time by a certain time can be used favorably for such applications.
- the F SK communication system of the present invention includes an optical F SK modulator, the FSK demodulator described above, the optical F SK modulator, and the optical F And a dispersive medium connecting the SK demodulator.
- a first sub Mach-Zehnder waveguide (MZ A ), a second sub-Mach-Zehnder waveguide (MZ B ), MZ and a a and the MZ B a light input unit, a main Mach-Zehnder waveguide and an output portion of the modulated light (MZ c), radio frequency to the two arms composing the MZ a
- the first RF electrode (RF A electrode) that inputs the (RF) signal, and the second RF electrode (RF B electrode) that inputs the RF signal to the two arms constituting the MZ B are input.
- the FSK communication system uses an optical FSK modulator that modulates the frequency of light output from the output unit.
- Such an optical FSK modulator can change the US B signal and LSB signal at high speed, and can provide an optical FSK communication system that can transmit information at high speed.
- Means for adjusting the delay time of two light beams to be demultiplexed (3)
- An FSK communication system having means for controlling the length of the delay time to be adjusted.
- the control means automatically adjusts the delay time according to the frequency of the modulation signal of the optical FSK modulator, the length of the dispersive medium, and the dispersion of the dispersive medium. Therefore, the delay time is automatically adjusted and favorable FSK demodulation is achieved.
- a preferred usage mode of the FSK communication system of the present invention is the above-described FS communication system, wherein the distance between the optical F SK modulator and the F SK demodulator, and the modulation frequency of the optical F SK signal. And the dispersion of the dispersive medium from the delay time of the light. That is, the distance between the optical FSK modulator and the FSK demodulator, the modulation frequency of the optical FSK signal, the delay time of the light, and the dispersion of the dispersive medium are predetermined. By using this relationship and information other than the dispersion of the dispersive medium, the dispersion of the dispersive medium can be found.
- a preferred mode of use of the FS communication system according to the present invention is the above-described FS communication system, wherein the dispersion of a dispersive medium existing between the optical FS modulator and the FS demodulator is
- the distance between the optical FS modulator and the F SK demodulator is calculated from the modulation frequency of the optical F SK signal and the optical delay time. That is, there are predetermined distances between the distance between the optical F SK modulator and the F SK demodulator, the modulation frequency of the optical F SK signal, the delay time of the light, and the dispersion of the dispersive medium.
- the distance between the optical FS modulator and the FS demodulator can be obtained from this relationship and information other than the distance between the optical F SK modulator and the FS demodulator.
- the FSK demodulator of the present invention is an FSK demodulator with an unconventional configuration, the present invention can provide a novel F S ⁇ demodulator that can be used for optical information communication and the like.
- the “means for adjusting the delay time of the two lights demultiplexed by the demultiplexer” adjusts the delay time between the US ⁇ signal and the LSB signal. It is possible to provide an FSK modulator that compensates for the delay of the optical FSK modulation signal due to the optical signal and that can appropriately demodulate the FSK signal.
- FIG 1 shows the basic configuration of the FSK demodulator of the present invention.
- Figure 2 is a schematic diagram showing the basic configuration of an optical SSB modulator.
- Figure 3 is a graph showing the relationship between the Q-factor and offset in Example 1.
- FIG. 4 shows the basic configuration of an FSK communication system that includes an optical FSK modulator.
- Figure 5 is a conceptual diagram for representing the delay.
- FIG. 1 shows the basic configuration of the FSK demodulator of the present invention.
- the FSK demodulator (1) of the present invention includes a means (2) for demultiplexing an optical signal transmitted from the transmitter according to its wavelength, and a demultiplexer. Means for adjusting the delay time of the two light beams (3), means for detecting one optical signal demultiplexed by the demultiplexer (4), and demultiplexing by the demultiplexer Means (5) for detecting the remaining optical signal, and means (6) for calculating a difference between the output signal of the first photodetector and the output signal of the second photodetector. To do.
- a demultiplexer As a “means for demultiplexing an optical signal transmitted from a transmitter according to its wavelength”, a demultiplexer is mentioned (hereinafter, this means is also called “demultiplexer”).
- a known duplexer such as an interleaver can be used as the duplexer (2). Since the light demultiplexed by the demultiplexer is an optical F SK signal, one that is demultiplexed into the upper side band (US B) signal and the lower side band (LSB) signal of the optical F SK signal is used.
- the interleaver can demultiplex incident wavelength-multiplexed optical signals into two sets of signal sequences whose wavelength intervals are twice, and conversely, combine two sets of wavelength-multiplexed signals into one signal sequence whose wavelength intervals are half. Then 2005/013534
- the interleaver includes a fiber type interleaver including a plurality of fiber force bras, a multilayer film type interleaver including a multilayer film and a prism, and a birefringent plate type including a birefringence plate and a polarization separation element.
- Interleavers and waveguide interleavers using waveguides are examples. More specifically, there are interleavers such as Nova-Interleavers manufactured by Optoplex, OC-192 manufactured by Nexfon, and 0C-768.
- An example of a “means for adjusting the delay time of two lights demultiplexed by a demultiplexer” is a known delay adjustment device (hereinafter, this means is also referred to as a “delay adjustment device”).
- An example of such a delay adjustment device is a delay adjustment device that consists of multiple mirrors and can adjust the optical path length. The delay time (and hence the mirror position) of this delay adjustment device may be automatically adjustable as appropriate, or may be fixed.
- subtractor As a “means for calculating the difference between the output signal of the first photodetector and the output signal of the second photodetector (6)”, there is a known subtractor. Also called “subtractor”.
- An example of a subtractor is a device that includes a calculation circuit that calculates the difference between the output signal of the first photodetector and the output signal of the second photodetector.
- the FSK demodulator of the present invention may include a known configuration other than the above used in the demodulator.
- a dispersion compensator is provided in the optical path after the duplexer (2). This is because such a dispersion compensator can compensate for the light dispersed by an optical fiber.
- an optical amplifier is provided after the duplexer (2).
- the amplitude of the optical signal output from a duplexer such as an interleaver may decrease. Therefore, by recovering the amplitude with an optical amplifier, it is possible to withstand long distance communications.
- Such an optical amplifier is preferably provided for each of the US B signal and the LSB signal.
- the F SK demodulator (1) receives the optical F SK signal. Then, the demultiplexer (2) demultiplexes the optical signal transmitted from the transmitter according to its wavelength, and demultiplexes it into the US B light and the LSB light ( ⁇ 2 ).
- the delay adjuster (3) eliminates the delay time between the US B light ( ⁇ ⁇ and LSB light ( ⁇ 2 ), for example, by adjusting the optical path length according to the delay time.
- the detector (4) detects one optical signal demultiplexed by the demultiplexer and converts it into an electric signal, and the second photodetector (5) demultiplexes by the demultiplexer.
- the remaining optical signal is detected and converted into an electrical signal
- the subtractor (6) calculates the difference between the output signal of the first photodetector and the output signal of the second photodetector. Yes.
- the signal obtained by the subtracter is output to a monitor (not shown). In this way, it is possible to demodulate the FSK signal, which eliminates the optical delay problem due to optical dispersion.
- the optical FSK communication system of the present invention consists of an optical FSK modulator (11), a light source (12), an FSK demodulator (1), and an optical FSK modulation. And a dispersive medium (13) connecting the FSK demodulator and control means (14).
- the FSK modulator described above can be used.
- An optical FSK modulator is one that changes the laser oscillation wavelength itself by changing the current supplied to the tunable laser light source.
- the optical S S B modulator can be improved to obtain the optical F S K signal without changing the frequency of the light source.
- the optical FSK modulator like the latter is preferable because the FSK signal cycle can be shortened and information can be loaded at high speed.
- the optical S S B modulator is described first, and then an optical F SK modulator improved from such an optical S S B modulator.
- Figure 2 shows a schematic diagram showing the basic configuration of the optical SSB modulator.
- the optical SSB modulator (41) consists of the first sub Mach-Zehnder waveguide (MZ A ) (42) and the second sub-Mach-Zehnder waveguide (MZ B ) ( 43), the main Mach-Zehnder waveguide (MZ C ) (44), the first bias adjustment electrode (DC A electrode) (45), the second bias adjustment electrode (DC B electrode) (46), A first modulation electrode (RF A electrode) (47), a second modulation electrode (RF B electrode) (48), and a third bias adjustment electrode (DC e electrode) (49).
- the main Mach-Zehnder waveguide (MZ C ) (44) is a Mach-Zehnder waveguide including MZ A and MZ B as both arms.
- First bias adjustment electrode (DC A electrode) (45) by controlling the bias voltage of between 2 Tsunoa over arm (Pathl and Path3) constituting the MZ A, propagating two arms of the MZ A It is an electrode for controlling the phase of light.
- the second bias adjustment electrode (DC B electrode) (46) controls a bias voltage between two arms composing the MZ B (Path2 and Path4), propagating the two arms of the MZ B It is an electrode for controlling the phase of light.
- the DC A and DC B electrodes are preferably usually DC or low frequency electrodes.
- “low frequency” in the low frequency electrode means, for example, a frequency of 0 Hz to 500 MHz.
- First modulation electrode (RF A electrode) (47) is an electrode for inputting a la-di O Frequency (RF) signal to the two arms composing the MZ A.
- the second modulation electrode (RF B electrode) (48) is an electrode for inputting RF signals to the two arms composing MZ B.
- RF A electrode and the RF B electrode a traveling wave electrode or a resonance electrode can be mentioned, and a resonance electrode is preferable.
- the RF A electrode and the RF B electrode are preferably connected to a high frequency electrical signal source.
- the high-frequency electrical signal source is a device for controlling the signal transmitted to the RF A electrode and RF B electrode, and a known high-frequency electrical signal source can be used.
- RF A electrode, and the frequency of the high frequency signal input to the RF B electrode (f m, or f FSK) as include, for example, 1 GH z ⁇ 100 GHz.
- the output of a high-frequency electric signal source includes a sine wave having a constant frequency.
- the RF A electrode and the RF B electrode are composed of, for example, gold or platinum.
- the width of the RF A electrode and RF B electrode is 1 ⁇ m to 10 im, and specifically 5 zm.
- the length of the RF A electrode and the RF B electrode is 0.1 to 0.9 times the wavelength of the modulation signal (4), 0.18 to 0.22 times, or 0.67 to 0.70 times, and more preferably. Is 20 to 25% shorter than the resonance point of the modulation signal. This is because the combined impedance with the stub electrode remains in an appropriate range. More specific RF A electrode and RF B electrode Examples of pole lengths include: Below, the resonant electrode and the traveling wave electrode are described.
- a resonant photoelectrode is an electrode that modulates using the resonance of the modulation signal.
- Known resonant electrodes can be used.
- Japanese Patent Laid-Open No. 2002-268025 “Tetsuya Kawanishi, Satoshi Oikawa, Masayuki Izutsu”, “Planar Resonant Optical Modulator”, IEICE Technical Report, TECHNICAL REPORT OF IEICE, IQE2001-3 (2001-05) J can be used.
- a traveling wave electrode is an electrode (modulator) that modulates light while guiding light waves and electrical signals in the same direction (for example, Hiroshi Nishihara, Haruna) Masamitsu and Toshiaki Sugawara, “Optical Integrated Circuits” (Revised Supplement) Ohm, pp. 119-120).
- the traveling wave type electrode a known one can be adopted.
- JP 11-295674 A, JP 11-295674 A, JP 2002-169133 A, JP 2002-40381 A, JP 2000 A -267056, JP 2000-471159, JP 10-133159, etc. can be used.
- a so-called symmetrical ground electrode arrangement (having at least a pair of ground electrodes on both sides of the traveling wave signal electrode) is preferably used.
- the high frequency output from the signal electrodes is easily applied to the ground electrodes placed on the left and right of the signal electrodes. The radiation to the side is suppressed.
- Third bias adjustment electrode (DC C electrode) (49) is the order of electrodes for controlling the phase of the light propagating in the MZ A and MZ B by controlling the Baiasu voltage of MZ A ⁇ Pi MZ B .
- the third bias adjustment electrode (DC C electrode) is usually a direct current or low frequency electrode.
- the RF electrode may serve as both an RF signal electrode and a DC signal electrode.
- either or both of the RF A electrode and RF B electrode are connected to a feed circuit (bias circuit) that supplies a mixture of DC and RF signals.
- the optical SSB modulator of this aspect is Since the RF electrode is connected to the feed circuit (bias circuit), RF signal (radio frequency signal) and DC signal (DC signal: signal related to bias voltage) can be input to the RF electrode, and the optical SSB modulator described above. Can function as well. (3. 1. 2. Operation of optical SSB modulator)
- optical SSB modulators The operation of optical SSB modulators is described, for example, in “Tetsuya Kawanishi, Masayuki Izutsu,“ Optical Frequency Shifter Using Optical SSB Modulator ”, IEICE Technical Report, TECHNICAL REPORT OF IEICE, OCS2002-49, PS2002-33, OFT2002-30 (2002-08) J, “Hisumi et al., X-Katsuri-Muniobium Optical SSB Modulator, Electron Letter, vol. 37, 515-516 (2001)”.
- the optical S S B modulator it is possible to obtain an upper sideband signal (US B) and a lower sideband signal (L S B) with a predetermined amount of frequency shifted positively.
- Light F SK modulator in order to realize the code switching at high speed, which was replaced with electrode corresponding to the DC C of the optical SSB modulator and RF (radio frequency) electrodes, or bias adjustment electrodes and RF electrodes is there.
- One that uses only the RF electrode is one in which the RF electrode is connected to a feed circuit (bias circuit) that supplies a mixture of DC and RF signals.
- the RF electrode a traveling wave electrode that supports high-speed switching can be used.
- the RF electrode is an electrode that supports input and output of the RF frequency.
- the FSK modulator can also output by switching the upper side wave component and the lower side wave component by switching the signal voltage of the RF c electrode.
- An optical F SK signal consists of an upper sideband (US B) signal and a lower sideband (LSB) signal for the carrier wave (f.).
- the width of frequency modulation by the optical FSK modulator (that is, the frequency of the RF modulation signal from the modulator) is ⁇ / FSK .
- the center frequency of the carrier wave is f.
- the center frequency of the US B signal is f. + A / FSK
- center frequency of LSB signal is f. _ ⁇ f FSK . (3. 2. Light source)
- the light source (12) is a device that generates light, such as a laser, that is input to the optical FSK modulator.
- the laser wavelength generated from the laser light source is changed.
- the frequency is shifted by the optical modulator, so that the output of the laser light source itself can be kept constant.
- Examples of dispersive media include optical fiber, gas, and air.
- Single-mode fiber is an example of optical fiber.
- the length of the optical fiber is 10 km to 20 km.
- the dispersion of single-mode fiber is approximately 17 ps / nm * km. In other words, light with a wavelength difference of 1 nm causes a time difference of about 17 ps when it travels 1 km.
- the control means is a means for controlling the delay time. That is, a preferable aspect of the FSK communication system of the present invention is that the “demultiplexer” is used in accordance with the frequency of the modulation signal of the optical FSK modulator, the length of the dispersive medium, and the dispersion of the dispersive medium. Means for adjusting the delay time of two light waves (3) An FSK communication system having means for controlling the length of the delay time adjusted by “3”. In such a system, the control means automatically adjusts the delay time according to the frequency of the modulation signal of the optical FSK modulator, the length of the dispersive medium, and the dispersion of the dispersive medium. Since an instruction is issued, the delay time is automatically adjusted and favorable FSK demodulation is achieved.
- the delay time should be adjusted according to these equations.
- the length of the adjustment to the optical path ⁇ 1 and (El) may be a ⁇ 1 I ⁇ t I ⁇ c X 1 0- 12 [m] and. Specifically, since the USB signal reaches the detector early, it is only necessary to lengthen the optical path by ⁇ 1 minutes.
- This adjustment of the optical path length may be performed based on the above logical expression, or the optical path length may be adjusted by applying a test pulse to the system and detecting the signal, for example.
- the FSK demodulator of the present invention can be used in fields such as optical information communications as a new demodulator that demodulates the optical FSK signal from the optical FSK modulator.
- a preferred mode of use of the FSK communication system of the present invention is the above FSK communication system, wherein the distance between the optical FSK modulator and the FSK demodulator, the modulation frequency of the optical FSK signal, Measure dispersion of dispersive medium from light delay time Is the method. That is, there is a predetermined relationship between the distance between the optical FSK modulator and the FSK demodulator, the modulation frequency of the optical FSK signal, the delay time of the light, and the dispersion of the dispersive medium. Therefore, by using this relationship and information other than the dispersion of the dispersive medium, the dispersion of the dispersive medium can be obtained.
- a preferred mode of use of the FSK communication system of the present invention is that the above FSK communication system is used, the dispersion of the dispersive medium existing between the optical FSK modulator and the FSK demodulator, and the modulation of the optical FSK signal.
- This is a method for obtaining a distance between the optical FSK modulator and the FSK demodulator from the frequency and the optical delay time based on the optical delay time. That is, there is a predetermined relationship among the distance between the optical FSK modulator and the FSK demodulator, the modulation frequency of the optical FSK signal, the delay time of the light, and the dispersion of the dispersive medium. From the relationship and information other than the distance between the optical FSK modulator and the FSK demodulator, the distance between the optical FSK modulator and the FSK demodulator can be obtained.
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Abstract
Description
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Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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US11/658,127 US8170422B2 (en) | 2004-07-20 | 2005-07-19 | Frequency shift keying demodulator |
Applications Claiming Priority (2)
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JP2004211185A JP4533999B2 (ja) | 2004-07-20 | 2004-07-20 | 周波数シフトキーイング復調器 |
JP2004-211185 | 2004-07-20 |
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WO2006009269A1 true WO2006009269A1 (ja) | 2006-01-26 |
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PCT/JP2005/013534 WO2006009269A1 (ja) | 2004-07-20 | 2005-07-19 | 周波数シフトキーイング復調器 |
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US (1) | US8170422B2 (ja) |
JP (1) | JP4533999B2 (ja) |
WO (1) | WO2006009269A1 (ja) |
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JP5168685B2 (ja) * | 2007-09-18 | 2013-03-21 | 独立行政法人情報通信研究機構 | 直交振幅変調信号発生装置 |
JP6052580B2 (ja) * | 2012-07-25 | 2016-12-27 | 国立研究開発法人情報通信研究機構 | Fsk変調器によるrf信号の周波数測定装置 |
JP6627640B2 (ja) * | 2016-05-16 | 2020-01-08 | 富士通株式会社 | 光送信機 |
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JPH05206952A (ja) * | 1991-08-15 | 1993-08-13 | General Instr Corp | 振幅変調光ファイバ通信用低ひずみレーザシステム |
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JPH06224882A (ja) * | 1992-10-03 | 1994-08-12 | Canon Inc | 光fsk受信器及びそれを用いた光fdm−fsk伝送システム |
JPH1117746A (ja) | 1997-06-20 | 1999-01-22 | Oi Denki Kk | 周波数シフトキーイングを用いた変調方法 |
US6359716B1 (en) * | 1999-02-24 | 2002-03-19 | Massachusetts Institute Of Technology | All-optical analog FM optical receiver |
US6959154B1 (en) * | 2000-11-28 | 2005-10-25 | At&T Corp. | Diversity receiver for mitigating the effects of fiber dispersion by separate detection of the two transmitted sidebands |
US7526209B2 (en) * | 2003-10-10 | 2009-04-28 | National Institute Of Information And Communications Technology | Optical frequency shift keying modulator |
JP2005210537A (ja) * | 2004-01-23 | 2005-08-04 | National Institute Of Information & Communication Technology | 光fsk変調器を用いたuwb信号の発生装置 |
JP3843322B2 (ja) * | 2004-02-16 | 2006-11-08 | 独立行政法人情報通信研究機構 | 光波長多重fsk変調方法 |
JP3867148B2 (ja) * | 2004-03-16 | 2007-01-10 | 独立行政法人情報通信研究機構 | 光ssb変調器又は光fsk変調器のバイアス調整方法 |
JP4524482B2 (ja) * | 2004-03-24 | 2010-08-18 | 独立行政法人情報通信研究機構 | 光ssb変調器 |
JP4696264B2 (ja) * | 2005-08-24 | 2011-06-08 | 独立行政法人情報通信研究機構 | 強度バランス機能を有する光fsk/ssb変調器 |
JP4465458B2 (ja) * | 2005-09-20 | 2010-05-19 | 独立行政法人情報通信研究機構 | 位相制御光fsk変調器 |
-
2004
- 2004-07-20 JP JP2004211185A patent/JP4533999B2/ja not_active Expired - Fee Related
-
2005
- 2005-07-19 WO PCT/JP2005/013534 patent/WO2006009269A1/ja active Application Filing
- 2005-07-19 US US11/658,127 patent/US8170422B2/en not_active Expired - Fee Related
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JPH0352341A (ja) * | 1989-07-20 | 1991-03-06 | Fujitsu Ltd | コヒーレント光通信用受信装置 |
JPH05206952A (ja) * | 1991-08-15 | 1993-08-13 | General Instr Corp | 振幅変調光ファイバ通信用低ひずみレーザシステム |
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Also Published As
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JP2006033556A (ja) | 2006-02-02 |
US20080304827A1 (en) | 2008-12-11 |
US8170422B2 (en) | 2012-05-01 |
JP4533999B2 (ja) | 2010-09-01 |
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