Method and apparatus for frequency modulating a semiconductor laser, and an optical communication system using the same

BACKGROUND OF THE INVENTION

Field of the Invention

0001The present invention relates to a driving method and a driving apparatus for a semiconductor laser, and an optical communication method and system using the driving method and apparatus. The present invention also relates to a modulation method for a semiconductor laser that is used as a light source for optical communications, in which a modulation signal for driving the laser is caused to be in-phase with an optically modulated signal radiated from the laser over a wide modulation frequency band. The present invention further relates to a driving method for a semiconductor laser for stabilizing and narrowing the spectral line-width of an oscillation wavelength of the laser even if the frequency of fluctuation of the spectrum of oscillation wavelength or optical frequency is low. Within the spectral line-width, the oscillation wavelength of the laser fluctuates with time.

Related Background Art

0002Conventionally, a distributed feedback laser (DFB laser), that radiates in a single longitudinal or axial mode, has been developed as a light source for optical communications, for example.

0003In a direct optical intensity or amplitude modulation system, which is presently put into practice using the above laser (also referred to as LD hereinafter), the amplitude of a modulation current required for driving LD needs to be set around several tens of mA. In addition, the bias current point of LD needs to be close to its threshold. As a result, the resonance frequency due to relaxation vibration is low, and hence such LD is unsuitable for high-frequency modulation of more than several Gbps. The phenomenon of such resonance is observed in the high-frequency modulation of LD. Furthermore, the fluctuation of the oscillation wavelength during the modulation of LD is large, leading to the problem of wavelength dispersion of signals during long-distance transmissions through an optical fiber and the problem of crosstalk between channels in wavelength division multiplexing (WDM) communications.

0004On the other hand, in a direct frequency modulation system, which utilizes modulation current injection into LD, the amplitude of modulation current is small, e.g. about several mA, and the bias current point of LD is above its threshold. Thus, LD is constantly modulated while oscillating. Therefore, a direct frequency modulation system is capable of modulation in a wide bandwidth, and its oscillation wavelength fluctuation is small. Thus, the direct frequency modulation system is promising for use in long-distance transmissions and wavelength division multiplexing communications.

0005When coherent optical communication is employed to apply that direct frequency modulation system to super long-distance transmissions or high-density optical frequency division multiplexing systems, the spectral line-width of a light source should be narrowed and the oscillation wavelength of the light source should be highly stabilized. Narrowing and stabilization can be achieved by an electrical negative feedback control. Also, in this case, the direct frequency modulation characteristic of LD is utilized. Such techniques for stabilization may also be applied to optical measurements.

0006The direct frequency modulation characteristics of the laser are, however, degraded in a low-frequency range less than several MHz. This is a considerable problem. For example, when a single-electrode DFB laser as shown in Fig. 1 is modulated with a sinusoidal wave current, the relationship between modulation frequency and modulation efficiency (the amount of an optical frequency shift caused by a change in current of 1mA) varies with modulation efficiency increasing as modulation frequency enters the low frequency region. as shown in Fig. 2. The relationship between modulation frequency and phase difference (a phase difference between modulation current injected into LD and modulation optical signal emitted by LD) also varies, with phase difference increasing to approximately 180 degrees, as modulation frequency decreases to the low frequency region, as illustrated in Fig. 3. It can be seen therefrom that the modulation efficiency fluctuates in a frequency band range less than several MHz and the phase difference also fluctuates and exibits a reverse or anti-phase (a phase shift by about 180 degrees) response as the modulation frequency decreases from approximately 10 MHz and and approaches zero. The reason therefor is that the laser's direct frequency modulation characteristics result from the superposition of competing physical mechanisms; an anti-phase refractive index variation due to heat (a change in the refractive index due to a change in heat in LD shifts in phase relative to the change in heat by 180 degrees), which has a cutoff frequency around several MHz, and the effect of an in-phase refractive index variation due to carrier density (no phase shift of a change in the refractive index due to a change in carrier density in LD occurs relative to the phase of the change in carrier density), which is flat or unchanged up to the resonance frequency. Since the effect of heat is dominant in a low-frequency band range, the flatness of the modulation characteristic is destroyed as discussed above.

0007Various problems arise when those adverse characteristics appear. First of all, in the case of frequency shift keying (FSK) in which digital signals are transmitted as a frequency modulation, an optically modulated waveform is phase shifted, causing a transmission error, when a modulation frequency falls below several MHz. Figs. 4A and 4B show such an example. As illustrated in Fig. 4A, the optically modulated pulse width thins when the modulation pulse width is around 1MHz, and as shown in Fig. 4B the optical waveform is inverted or in an anti-phase with the modulation signal when the modulation frequency is aroud 100kHz. Therefore, there is a limit to modulation frequency in a low frequency band range, and a freedom in coding is therefore restricted.

0008Furthermore, when the spectral line-width of LD is narrowed by applying an electric negative feedback thereto, the phase of a change in the total refractive index shifts from the desired if its oscillation wavelength fluctuation has a frequency less than several MHz. Hence the negative feedback control of LD becomes difficult to achieve.

0009Several methods for improving a semiconductor laser apparatus have been proposed to solve those problems. For example, a three-electrode structure is built as shown in Fig. 5 and a current, injected through end electrodes or central electrode 1045, is modulated to suppress the effect of heat mentioned above (see Yuzo Yoshikuni, et al., IEEE J. Lightwave Technol., vol. LT-5, No. 4, 516, April, 1987). In this case, however, its behaviour varies depending on the amount of bias current injected through each electrode, and variation among devices exists. Thus, such a structure is difficult to put into a practical use. In Fig. 5, reference numeral 1041 designates a substrate, reference numeral 1042 designates an active layer, reference numeral 1043 designates a clad layer, and reference numeral 1044 designates a grating.

0010Another conventional device has a λ/4-shifted diffraction grating 1052, with the depth of the diffraction grating 1052 at a central portion 1056, being larger than that at peripheral portions as shown in Fig. 6. In this device, current injected through a central electrode 1055 is modulated, causing the effects of carrier density mentioned above to exhibit an anti-phase response so as to be in-phase with the effects of heat. As a result, the phase shift of the change in the total refractive index from the desired is eliminated, and further the effect of heat can be reduced. Thus, the characteristic in a low modulation frequency band range is improved (see H. Shoji, et al., Informal Paper of 1992 Vernal Conference of Japan Applied Physics Society, 30a-SF-8). This device, however, has the problem that its manufacturing is complicated, leading to poor yield and a high manufacturing cost. In Fig. 6, reference numeral 1051 designates a substrate, reference numeral 1053 designates a light guide layer, and reference numeral 1054 designates an active layer.

0011Further prior art is known from the publication "Vector Modulation Of Split Contact DFB Lasers" in IEE Proceedings J. Optoelectronics. Vol. 138, No. 2, April 1991 by W. B. Hale et. al., and document EP-A-0 477 987.

SUMMARY OF THE INVENTION

0012It is an object of the present invention to solve the above problems by a relatively simple driving method and a driving apparatus of a semiconductor laser and an optical communication method and system using the driving method and apparatus. The object of the present invention is achieved by the following driving method for a semiconductor laser as set out in claim 1, a driving apparatus for driving a semiconductor laser as defined in claim 15, a coherent optical communication method as recited in claim 48, and an optical communication method as set out in claim 50, as well as by a wavelength division multiplexing transmission type of optical communication method defined in claims 51 and 52, respectively, and an optical, cable television system as defined in claim 53.

0013Further preferred embodiments of the present invention are set out in the respective dependent claims.

0014The advantages of the present invention will be more readily understood in connection with the following detailed description of the preferred embodiments in conjunction with the drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

0015Fig. 1 is a perspective, cross sectional view illustrating a single-electrode distributed feedback laser.

0016Fig. 2 is a graph illustrating a prior art frequency modulation characteristic.

0017Fig. 3 is a graph illustrating a prior art phase characteristic.

0018Figs. 4A and 4B are respectively views illustrating prior art FSK response characteristics.

0019Fig. 5 is a cross section view illustrating a prior art three-electrode distributed feedback laser.

0020Fig. 6 is a cross section view illustrating a prior art distributed feedback laser which has a grating having an uneven depth.

0021Fig. 7 is a perspective cross section view showing a distributed feedback semiconductor laser which is used in a driving method of the present invention.

0022Fig. 8 is a graph illustrating a modulation characteristic when current injected only through one of two electrodes is frequency-modulated.

0023Fig. 9 is a schematic block diagram illustrating a driving circuit, according to a first embodiment of the present invention.

0024Fig. 10 is a graph illustrating a modulation characteristic when frequency modulation is performed according to a driving method of the present invention.

0025Fig. 11 is a schematic block diagram illustrating a driving circuit, according to a second embodiment of the present invention.

0026Fig. 12 is a schematic block diagram illustrating a driving circuit for narrowing spectral line-width according to a third embodiment of the present invention.

0027Fig. 13 is a schematic block diagram illustrating a driving circuit, according to a fourth embodiment of the present invention.

0028Fig. 14 is a view illustrating the principle of a driving method of the fourth embodiment of the present invention.

0029Fig. 15 is a schematic block diagram illustrating a driving circuit, according to a fifth embodiment of the present invention.

0030Fig. 16 is a schematic block diagram illustrating a driving circuit for narrowing spectral line-width according to a sixth embodiment of the present invention.

0031Fig. 17 is a block diagram illustrating a transmission system for performing coherent optical communication according to the present invention.

0032Fig. 18 is a graph illustrating a wavelength changeable characteristic of a distributed feedback semiconductor laser.

0033Fig. 19 is a block diagram illustrating a transmission system for performing wavelength division multiplexing transmission according to an eighth embodiment of the present invention.

0034Fig. 20 is a transmission spectrum, illustrating wavelength multiplexed signals according to the present invention.

0035Fig. 21 is a view of a ninth embodiment of the present invention, showing an optical node .

0036Fig. 22 is a block diagram of an optical local area network (LAN) according to the present invention.

0037Fig. 23 is a block diagram of an optical cable television (CATV) system according to the present invention.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

First Embodiment

0038A first embodiment of the present invention will be described with reference to Figs. 7-10. Fig. 7 shows a two-electrode DFB laser which is used for performing a driving method of the present invention. Fig. 9 shows a driving system of the first embodiment.

0039In Fig. 7, reference numeral 101 is an n-type GaAs substrate, reference numeral 102 is an n-type Al_xGa_1-xAs (x=0.45) clad layer, reference numeral 103 is a multiple quantum well active layer comprising five i(intrinsic)-GaAs well layers (thickness: 6nm) and six i-Al_xGa_1-xAs barrier layers (x=0.22, thickness: 10nm), which are layered alternately, reference numeral 104 is a p-type Al_xGa_1-xAs (x=0.15) light guide layer, reference numeral 105 is a p-type Al_xGa_1-xAs (x=0.45) clad layer, reference numeral 106 is a p-type Al_xGa_1-xAs (x=0.05) contact layer, reference numeral 107 is a p-type Al_xGa_1-xAs (x=0.4) burying layer, reference numeral 108 is an n-type Al_xGa_1-xAs (x=0.4) burying layer, reference numeral 109 is a p-type electrode, and reference numeral 110 is an n-type electrode. A grating g having a pitch of 245 nm and a depth of 100nm is formed on the light guide layer 104, and an antireflection coating 111 is provided on one of light-emerging end faces. The p-electrode 109 and the contact layer 106 are each divided into two portions by a space, provided at the device's center as shown in Fig. 7.

0040Bias current I₁ is caused to flow through the electrode 109 on the side nearest the antireflection coating 111, and bias current I₂ is caused to flow through the electrode 109 on the other side. The oscillation in a DFB mode is caused by a threshold of approximately I₁ +I₂=30mA (I₁, I₂>10mA). In the oscillated state, a high-frequency modulation current ΔI₁ is superposed only on the bias current I₁ by a bias T, which is a means for alternating current (AC) coupling, to perform the frequency modulation. The modulation characteristic at this time is illustrated in Fig. 8. The modulation efficiency remains flat or constant at about 0.6GHz/mA over a range of the modulation frequency from several MHz to several GHz. It can be seen from Fig. 8 that the modulation efficiency increases when the modulation frequency is in a range less than several MHz. This results from the fact that the effect of heat is great and dominant in a low modulation frequency range as described above. The phase difference characteristic is similar to that of a conventional device shown in Fig. 3.

0041Therefore, compensation current ΔI₂ is superposed on the bias current I₂ by using a structure as shown in Fig. 9. In the structure of Fig. 9, a modulation signal from a modulation electric source 409 is divided into two current output portions having a 1:1 ratio by a power divider 408. One output is provided to an inverting type wideband video amplifier 406 whose gain and cutoff frequency are respectively approximately 10 and 10GHz. Then, the amplified current, ΔI₁, is superposed on a DC current I₁, provided by a DC current source 403 by means of a bias T 402 which is constructed from a solenoid and a capacitor, having component values chosen to provided a low frequency cutoff of about 1kHz. The capacitor further allows DC components, such as offsets, to be removed from the amplified current ΔI₁. The thus-superposed current (I₁+ΔI₁) drives a semiconductor laser 401. The laser 401 is depicted by using a pair of diodes. The other current output of the power divider 408 is input into a non-inverting type operational amplifier 407 whose gain and cutoff frequency are respectively about 3 and 10MHz. Similarly, its amplified current ΔI₂ is superposed on DC current I₂ from a DC current source 405 by a bias T 404, and another superposed current (I₂+ΔI₂) also drives the laser 401. In this case, the output of the modulation electric source 409 is variable, and a modulation index is adjusted by varying the output of modulation source 409. The modulation index is a ratio between maximum and minimum current of the superposed modulation current.

0042In the first embodiment, to effectively suppress the phase difference due to the effect of heat in a low modulation frequency band range and render the modulation operation optimum, the gain of the inverting wideband video amplifier 406 is fixed at a value of about 10, and the gain of the non-inverting operational amplifier 407 is varied until the desired characteristics are achieved. As a result, the gain of the non-inverting operational amplifier 407 is preferably about 3. The gain values will differ depending on the device structure, material, packaging configuration and the like, and therefore, they need to be adjusted to optimum values for each application.

0043When frequency modulation is performed according to the above embodiment, the low-frequency band modulation characteristic is highly improved as illustrated in Fig. 10. Thus, a flat modulation characteristic is obtained over a range down to several kHz. At the same time, the phase difference characteristic exhibits an in-phase response in a range from several kHz to about 1GHz. Consequently, even a simple-structure DFB laser can achieve a frequency modulation with a square wave signal, whose frequency is from several kHz to several GHz, or FSK transmission.

0044Further, the wideband video amplifier 406 is preferably an inverting type and the operational amplifier 407 is preferably a non-inverting type in the first embodiment. This is only because an inverting type wideband amplifier has generally superior noise and offset characteristics than other types. However, a non-inverting wide band video amplifier and an inverting operational amplifier may alternatively be used without departing from the invention.

0045As described above, the above-discussed problem can be solved without complicating the structure of a device very much.

0046The principle of operation will briefly be summarized using a concrete example. A two-electrode DFB laser as shown in Fig. 7 is prepared. When current is injected only through one electrode, the modulation characteristic is as shown in Fig. 8. In this case, the effect of heat in a low-frequency band range is reduced compared with the laser as shown in Fig. 1, but yet the desirable flat region extends only down to about several MHz. Therefore, a phase-shifted or anti-phase signal synchronized with the modulation signal is injected through another electrode when the modulation frequency is in a low-frequency (less than several tens MHz) band range. The magnitude of the phase-shifted current varies depending on material, structure and packaging configuration of devices. This magnitude is adjusted to an optimum value by adjusting the gains of the respective amplifiers 406 and 407 so that the phase difference between the modulation current injected through the first electrode and a light output from the laser ia maintained at zero over a low-frequency band range. Then, the low-frequency characteristic can be extended down to several kHz as shown in Fig. 10.

0047Such a means for generating an anti-phase signal can be constructed in various manners. Such means can be readily realized since only a low-frequency band range, extending from about DC to about 10-20 MHz, needs to be considered. One example is shown in Fig. 9.

Second Embodiment

0048A second embodiment of the present invention will be described with reference to Fig. 11. A laser device used in connection with this embodiment is substantially the same as the two-electrode DFB laser used in the first embodiment.

0049In this embodiment, no bias T's having a low-frequency cutoff are used, and instead a conventional laser driver integrated circuit (IC) is preferably used as a voltage-current converter, which is a coupling device that can be modulated, to reduce the size of the entire driving system. The voltage-current converter supplies driving current by using a voltage signal. In respective driver ICs 503 and 504, DC current sources I_b1 and I_b2 and modulation current sources I_p1 and I_p2 are connected in a parallel arrangement, and modulation currents ΔI₁ and ΔI₂ having DC offset currents I₁ and I₂ can be supplied respectively therefrom by inputting thereinto a modulation signal from a modulation signal source 505. The modulation index and bias current amount can be controlled on the IC side, respectively, as described above.

0050Next, a particular driving method will be described. The output of a modulation current source 505 is supplied to the driver ICs 503 and 504. When the signal from the modulation electric source 505 is divided into two portions, no power divider is necessary if the division is conducted immediately before the two driver ICs 503 and 504. The driver IC 503 supplies an in-phase output, which is in-phase with the modulation signal input, to a laser 501 as driving current I₁+ΔI₁. The driver IC 504 supplies an anti-phase output which is anti-phase with the modulation signal input. This can be performed by a single driver IC which can supply in-phase and anti-phase outputs. The anti-phase output is input into a low pass filter 502, which has a cutoff frequency of about 10MHz, and the output of the low pass filter 502 is supplied to a laser 501 as driving current of I₂+ΔI₂. The current magnitude ratio between ΔI₁ and ΔI₂ is made optimum at about 10:3, similar to the first embodiment. The driver IC is preferably designed as shown in Fig. 11, wherein the laser 501 is grounded on its upper side to draw current thereinto, so that a high-speed modulation operation can be obtained. Therefore, in this embodiment, the conduction type of the laser 501 is opposite to that shown in Fig. 7. That is, a p-type substrate is used and the electrode is divided into two portions on the side of an n-type electrode.

0051When the driving system is constructed as above, the entire system can be made very compact in size, and can be put into a single box as a module. While the lower limit of a low modulation frequency range is limited by the cutoff frequency of the bias T in the first embodiment, there is no lower limit concerning a low modulation frequency range in the second embodiment. As a result, the low modulation frequency characteristic can be further improved, and the modulation frequency characteristic can be flattened over a modulation frequency range between about 100Hz and several GHz. Thus, when FSK transmission is conducted, information can be coded by using No Return Zero (NRZ) signal whose frequency and continuity are respectively 3Gbps and more than 2²⁰-1, for example. Consequently a very high-speed transmission can be attained.

Third Embodiment

0052In a third embodiment of the present invention, the driving circuit of the first embodiment for improving the low modulation frequency range characteristic of a laser includes means for narrowing the spectral line-width of oscillation wavelength of a laser by an electric feedback. When a period of oscillation wavelength fluctuation is longer than a predetermined value, a general feedback method for narrowing the spectral line-width cannot be applied because the above-discussed phase shift due to the effect of heat occurs. This embodiment can cope with such a problem. A driving system is shown in Fig. 12.

0053A light beam from a semiconductor DFB laser 601 is input into an optical frequency discriminator 610 to convert fluctuation of the wavelength of radiated light beam to fluctuation of a light intensity, and the fluctuation of the light intensity is converted to an electric signal by a photodetector 609. In this embodiment, a Fabry-Perot etalon, whose free spectral range and finesse are respectively 5GHz and 50, is preferably used as the optical frequency discriminator 610. A GaAs pin photodiode is preferably employed as the photodetector 609. The electric signal so provided is superposed on injection current into the laser 601. The output of photodetector 609 is provided as an input to a power divider 608, in a similar manner as the modulation signal source 409 of the first embodiment, and the feedback control is performed. The feedback ratio can be adjusted by varying the gains of amplifiers 606 and 607 and the light power incident on the photodetector 609. In this case, the gains of the amplifiers 606 and 607 are respectively set to about 100 and 30, and an optimum feedback adjustment is achieved with light power in a range between about 10 µW and about 100 µW. Further, a long optical path length of the feedback system may limit the top of the high modulation frequency band, so the path length is restricted to about 10cm and the frequency, at which a resonance occurs owing to a time delay of the feedback signal, is moved away to 3GHz.

0054As a result, while the spectral line-width is around 15MHz under non-feedback control condition, the spectral line-width can be narrowed to about 200kHz, i.e. about a hundredth of 15MHz, in this embodiment. This level is a practical level for making the laser usable as a light source of coherent optical communications.

0055In addition, when modulation current is further superposed, FSK transmissions can be conducted by using the driving system and method of the first or second embodiment.

Fourth Embodiment

0056A fourth embodiment of the present invention will be described with reference to Figs. 13 and 14. The fourth embodiment is different from the first embodiment in the following point. In Fig. 13, the same reference numerals as those in Fig. 9 designate the same members or devices.

0057The gain of amplifier 407 is made variable, and automatically adjusted to suppress the effect of heat in a low modulation frequency band range.

0058A sinusoidal wave oscillator 410 outputs two signals of approximately 5kHz. One sinusoidal wave signal is input into a modulation electric source 409 and superposed on a modulation signal generated by the modulation electric source 409, and the other signal is mixed, by a balanced modulator 411, with a signal which is produced as follows: A portion of the output of a laser 401 is extracted by a beam splitter 414. The extracted light is transmitted through a frequency discriminator 415, such as preferably a Fabry-Perot etalon, and converted to an electric signal output by a photodetector 413. A signal component of about 5kHz is picked out from the photodetector output signal by a band pass filter 412. The other oscillator signal is mixed, by the balanced modulator 411, with the approximately 5kHz signal from the band pass filter 412.

0059A DC component of the mixed output from the balanced modulator 411 is selected out by a low pass filter 416, and provided as a gain control signal to amplifier 407 which is automatically gain controlled by this DC signal. This principle will be described with reference to Fig. 14.

0060When the laser 401 is modulated at intervals of 5kHz, the frequency modulation occurs substantially only due to the effect of heat. Three cases exist depending on a difference in magnitude of the effect of heat at the two electrodes 109 of the laser 401. In the case where an oscillation frequency fluctuation Δf₂ caused by the effect of heat due to an injected current ΔI₂ is smaller than an oscillation frequency fluctuation Δf₁ caused by the effect of heat due to an injected current ΔI₁, as shown in a portion (a) of Fig. 14, the frequency fluctuation of output light is in-phase with Δf₁ or anti-phase with ΔI₁. In the opposite case thereto where Δf₁ is less than Δf₂, as shown in a portion (c) of Fig. 14, the frequency fluctuation of output light is in-phase with ΔI₁, or anti-phase with Δf₁. Further, in the case where the oscillation frequency fluctuation Δf₂ is substantially equal to the frequency fluctuation Δf₁ as shown in a portion (b) of Fig. 14, no output oscillation frequency fluctuation exists due to mutual elimination. If the frequency fluctuation is detected by a positive slope of the frequency discriminator's signal and its output is mixed with the sinusoidal wave signal, a positive DC output is obtained from balanced modulator 411, when the photodetector output is in-phase with the sinusoidal wave signal or anti-phase with ΔI₁ which is provided by the inverting amplifier 406, as shown in the portion (a) of Fig. 14. Inversely, if the photodetector output is in an anti-phase with the sinusoidal wave signal as shown in the portion (c) of Fig. 14, a negative DC output is obtained from balanced modulator 411. If no frequency fluctuation exists as shown in the portion (b) of Fig. 14, the mixed output is zero. The case where the output is zero as shown in the portion (b) of Fig. 14 is an optimum point where the effect of heat at the two electrode regions eliminates each other. The deviation on either side from that optimum point is detected in the fourth embodiment, so that an automatic gain control of the amplifier 407 becomes possible. Therefore, the amplitude ratio between ΔI₁ and ΔI₂ can always be controlled automatically to be optimum.

0061When transmission is conducted, the sinusoidal wave component of 5kHz, which is used for the above-discussed automatic gain control, is removed at the signal receiver side. In this embodiment, the frequency of the sinusoidal wave is preferably 5kHz, which is cosen because its frequency value is low enough to cause frequency modulation solely due to the effect of heat and large enough to enable transmission through a bias T without attenuation due to a low cutoff frequency.

0062The principle of this embodiment will be summarized. In this embodiment, a low-frequency signal, for which the effect of heat is dominant, is superposed on each current injected into the laser. Thus, a feedback control is performed. Two electrodes are respectively modulated by low-frequency signals, such as sinusoidal wave signals of about 100Hz, for which the effect of heat is dominant, with those signals having the same amplitude and being in an anti-phase with each other, a portion of output signal from the laser is picked out, only a component of about 100Hz is selected by a band pass filter, and the selected component is combined with the sinusoidal wave signal of 100Hz which modulates the laser. When its DC component is picked out by a low pass filter, a positive, zero or negative DC output can be obtained depending on the magnitude of modulation factor due to the effect of heat at regions of the two electrodes. The feedback control is performed based on that DC output, and the modulation current amplitude provided at one of the two electrodes is adjusted by a gain controlled amplifier or attenuator, operating in response to the DC signal.

Fifth Embodiment

0063A fifth embodiment of the present invention will be described with reference to Fig. 15. The fifth embodiment is different from the second embodiment in the following point.

0064The current ratio between and ΔI₁ ΔI₂ is made variable, by adjusting the modulation current amplitude of driver IC 504, in the same manner as the fourth embodiment. In particular, the modulation current amplitude I_p of the driver IC 504 is automatically controlled by a mixed output of a low pass filter 511 which is produced by the superposition of a sinusoidal wave signal of 100Hz from a sinusoidal wave oscillator 506 and an output from a band pass filter 508 derived from a laser 501 in the same manner as the fourth embodiment. The frequency of the sinusoidal wave signal is preferably as low as possible to increase the continuity of NRZ signal. In this embodiment, this frequency is set at about 100Hz because there is no limiting low-frequency cutoff due to a bias T such as was described in the fourth embodiment. In Fig. 15, reference numeral 507 designates a balanced modulator, reference numeral 509 designates a photodetector, and reference numeral 510 designates an optical frequency discriminator. The operation of this embodiment is substantially the same as that of the fourth embodiment.

Sixth Embodiment

0065A sixth embodiment of the present invention will be described with reference to Fig. 16. The sixth embodiment is different from the third embodiment in the following point.

0066An electric signal detected by a photodetector 609 is input into a band elimination filter or trap circuit 612, whose output is superposed on the injection current into a laser 601 in a manner similar to the fourth embodiment to provide feedback control. The gain of the amplifier 607 is variable.

0067In this control system, the gain of amplifier 607 is rendered optimum by the antomatic control in the same manner as the fourth embodiment. A 5kHz signal, from a sinusoidal wave oscillator 611 is input into each of amplifiers 606 and 607. The output of photodetector 609 is further input into a band pass filter 613, whose output is mixed with the sinusoidal wave provided by balanced modulator 614. The mixed signal is transmitted through a low pass filter 615, and provided as a gain control signal which automatically controls the gain of the amplifier 607 to cancel the effect of heat mentioned above. It is necessary to prevent the occurrence of oscillation which would be caused when a signal, that is produced from the fluctuation of oscillation wavelength due to the sinusoidal wave signal, would be fed back without any change. The band elimination filter 612 serves to remove that component of frequency (the sinusoidal wave oscillation frequency) which will cause the oscillation.

Seventh Embodiment

0068Fig. 17 shows a structure in which an optical transmission system is assembled including a light source which is driven by the above-discussed driving method of the first embodiment, the combination of first and third embodiments, the fourth embodiment, the combination of fourth and sixth embodiments or the like. A light beam emitted from a light source 701 is coupled to a single mode optical fiber 702 to be transmitted therethrough. On a receiver side, a laser 703 is provided as a local oscillator which emits an oscillating light beam having the same wavelength as that of the light source 701, and an optical beat signal is generated by using the light beams from the both lasers 701 and 703. The beat signal is detected by a photodetector 705 using a delayed detection method. The oscillation wavelength of the laser 703 is stabilized by a conventional phase-locked loop (PLL) control circuit 706, using a signal created from the beat signal detected by a photodetector 705 as a control source.

Eighth Embodiment

0069In an eighth embodiment of the present invention, the tunable characteristic or wavelength-changeable characteristic of a laser is utilized to perform wavelength or frequency division multiplexing transmissions. In the two-electrode DFB laser described in the first embodiment, the oscillation wavelength can be changed by controlling the magnitudes of current injected through the respective electrodes. The tunable characteristic is illustrated in Fig. 18. When the amounts of bias current injected through the respective electrodes are maintained to be equal to each other, i.e. I₁=I₂, and the current I₁ is changed from 20mA to 60mA, the oscillation wavelength can be continuously changed over a bandwidth of about 1nm from 835nm to 836nm. In this embodiment, this property is utilized and a center of the oscillation wavelength spectrum is determined by controlling the bias current. Frequency modulation is conducted as described in the first embodiment or the like. The oscillation spectral line-width also may be narrowed as described in the third embodiment, the combination of first and third embodiments, the sixth embodiment, or the combination of fourth and sixth embodiments.

0070Turning to Fig. 19, a method for performing wavelength division multiplexing communication by using the driving method of this embodiment is illustrated. In Fig. 19, reference numeral 901 is a light source for optical communications, which is modulated by FSK system using the present invention. In the light source 901, the oscillation wavelength can be changed in a range having a width of 1nm as described above. In this embodiment, a frequency deviation amount of 5GHz of FSK system can be obtained by setting the modulation current amplitude to about 8.3mA. Therefore, when channels are arranged at intervals of about 10GHz or 0.02nm to perform the wavelength multiplexing, crosstalk among adajacent channels can be eliminated. Thus, when this light source apparatus is used, the wavelength or frequency multiplexing having about 1/0.02=50 channels is possible.

0071A light beam emitted from the light source 901 is coupled to a single mode optical fiber 902 to be transmitted therethrough. The signal light transmitted through the optical fiber 902 is received by a receiver apparatus. There, light of a desired wavelength is selectively demultiplexed by an optical filter 903, and the signal is detected by a photodetector 904. In this embodiment, a laser having the same structure as that of DFB laser of the first embodiment is used as the optical filter 903, and bias current having a magnitude below its threshold is injected thereinto. By changing the current ratio at the two electrodes of the optical filter 903, the transmission wavelength can be varied by 1nm while the transmission gain is maintained at 20dB. The 10dB-down transmission width of the filter 903 is approximately 10GHz or 0.02nm, and thus this filter 903 has sufficient bandwidth characteristic to attain the wavelength multiplexing having the intervals of 0.02nm as descrived above.

0072For detection of an FSK signal, the transmission characteristic of the filter 903 is utilized. As shown in Fig. 20, when the peak transmission wavelength of the filter 903 is tuned to a mark frequency (corresponding to a "1" of an FSK signal) of a desired channel, e.g. CH2, in the wavelength multiplexed signals, "1" and "0" can be detected at an extinction ratio of 10dB after transmission through the filter 903 since a space frequency (corresponding to a "0" of an FSK signal) is remote from the mark frequency by the frequency deviation amount of 5GHz as described above.

0073As an alternative to optical filter 903, other filters such as a Mach-Zehnder type filter and a fiber Fabry-Perot type filter, may be used. Furthermore, in this embodiment, a single light source and a single receiver apparatus are preferred, but a plurality of light sources and a plurality of receiver apparatuses respectively connected by optical couplers or the like may be used for optical communications.

0074Alternatively, a receiver for wavelength multiplexed signals may be a coherent system as described in the seventh embodiment, other than the method of this embodiment.

0075In the foregoing, a laser of GaAs series is described, but equivalent materials such as InP series may be used.

Ninth Embodiment

0076Fig. 21 shows an opto-electric conversion unit (node) which is connected to each terminal when a driving method of a light source for optical communications of the present invention and an optical communication system using this driving method are applied to a wavelength or frequency division multiplexing optical LAN system. Fig. 22 shows an example of an optical LAN system in which the node is utilized.

0077An optical signal is taken into the node through an optical fiber 1001 externally connected thereto, and a portion of the signal is caused to enter a receiving device 1003 having a tunable filter such as filter 903 of Fig. 19, discussed above, through a branching device 1002. In this apparatus, only an optical signal at a desired wavelength is selected out by the above method, and the selected signal is detected. An alternative receiving method may use coherent system as discussed in reference with Fig. 17 above, and in this case a local oscillation laser is provided in place of the optical filter.

0078On the other hand, when an optical signal is transmitted from the node, light from a tunable DFB laser 1004, which is driven in accord with the invention and modulated in FSk system, is caused to enter the light transmission line 1001 through an isolator 1005 and a branching device 1006.

0079Further, a plurality of tunable DFB lasers and a plurality of tunable optical filters may respectively be arranged so that the changeable wavelength range can be widened.

0080The optical LAN system shown in Fig. 22 is a bus type network, and nodes 1011, 1012, 1013 are connected along A and B directions so that multiple terminals 1021, 1022, 1023 and centers, which constitute a network, can be provided. When multiple nodes are connected, it is necessary to serially connect an optical amplifier on the transmission line 1001 to compensate for attenuation of transmitted light. Further, two nodes may be connected to each terminal to build two transmission lines, so that a bidirectional transmission is possible by DQDB system or the like.

0081In such an optical network system, using the driving method of the present invention, a high-density wavelength or frequency division multiplexing transmission network, which has a wavelength multiplicity of 50, can be constructed as described above.

0082Furthermore, a loop type network can be constructed by connecting A and B in Fig. 22, and a star type network and a compound-configuration type network may be established.

Tenth Embodiment

0083An optical CATV, as shown in Fig. 23, can be constructed using the apparatus and optical communication system of the present invention. In a CATV center 1031 or sub-center 1032, a tunable laser is modulated in accord with the invention as described above, and a wavelength multiplexing light source is constructed also in accord with the invention. On the side of a subscriber 1033 who is a receiver, a receiver apparatus having a tunable filter such as described in connection with Fig. 19, is used.

0084Conventionally, it is difficult to use a DFB filter in such a system due to influences of dynamic fluctuation of oscillation wavelength, but it becomes possible according to the present invention.

0085Further, a bidirectional CATV is possible in the following manner. The subscriber 1033 has an external modulator (an example of simple bidirectional optical CATV, see, for example, Ishikawa and Furuta "LiNbO₃ Optical Wavelength Modulator For Bi-directional Transmission in Optical CATV Subscriber Systems", OCS 91-82 1991), and a signal from the subscriber 1033 is received as a reflected light (reflected light of a signal light transmitted to the subscriber 1033) from its external modulator. Thus, a star type network as shown in Fig. 23 is constructed, and highly improved functions of services can be obtained.

0086According to the present invention, a modulation frequency band range on a low-frequency side can be greatly expanded when a semiconductor laser is frequency-modulated, and hence a high-speed transmission becomes possible. In particular cases, this can be achieved irrespective of changes in laser's packaging configuration, environment and the like.

0087Furthermore, a band range can be widened when an oscillation spectral line-width is narrowed by an electric feedback method, so that a spectral line width, which is narrower than that of a conventional one, can readily be attained. Thus, a light source, which is suitable for a coherent optical communication, can be provided, for example.

0088Except as otherwise disclosed herein, the various components shown in outline or block form in the Figures are individually well known in the optical semiconductor device, its driving method and optical communication arts, and their internal construction and operation are not critical either to the making or using of this invention or to a description of the best mode of the invention.

0089While the present invention has been described with respect to what are presently considered to be the preferred embodiments, it is to be understood that the invention is not limited to the disclosed embodiments. The present invention is intended to cover various modifications and equivalent arrangements included within the scope of the appended claims.

0090A driving method of the present invention drives a semiconductor laser which is provided with at least first and second electrodes through each of which current is injected into the semiconductor laser. Varying current is injected through the first electrode when the frequency of the varying current is in a high frequency band. Varying current is injected through the first electrode while phase-shifted current, whose phase is shifted relative to the varying current, is injected through the second electrode, when the frequency of the varying current is in a low frequency band which is lower than the frequency of the high frequency band. Feedback-control may be performed for controlling a ratio between amplitudes of the modulation current and the phase-shifted current based on a light output from the semiconductor laser. The varying current includes at least modulation current modulated according to a predetermined signal or negative feedback current produced by an electric signal obtained by detecting fluctuation of oscillation wavelength of a light output from the semiconductor laser. Thus, an optical signal radiated from the laser can be desirably stabilized over a wide frequency band range.