Method of optical transmission and optical transmitter used in the same

Abstract: A method of optical transmission comprises steps of generating a light signal, controlling a wavelength of the light signal in accordance with a correcting signal, and modulating an intensity of the light signal supplies from a light source (1) to generate an output light signal in accordance with a modulating signal. The wavelength change of the light signal generated by the light source (1) coincides with the wavelength change which occurs during the modulating step, so that the wavelength change is cancelled in the output light signal. An optical transmitter used in the method comprises a light source (1) which generates a light signal, a correcting signal generating circuit (3) which supplies the light source (1) with a correcting signal for changing the wavelength of the light signal generated by the light source(1) and an optical modulator (2) which modulates an intensity of the light signal supplied from the light source (1) to generate an output light signal in accordance with a modulating signal.

Description: This invention relates to a method of optical transmission and an optical transmitter used in the same, and more particularly to a method of optical transmission used in a digital optical communication using an optical fiber, and an optical transmitter used in the same. In an optical communication in which information is transferred by a light signal through an optical fiber, a dispersion of the wavelength of the light signal occurs during the transmission. The dispersion of the wavelength causes waveform degradation of the light signal, so that faulty information may be transferred. As result, the transmission distance over which correct information is transferred is limited by the wavelength dispersion. Therefore, it is necessary to narrow the wavelength spectrum of the light signal to lengthen the transmission distance. In order to obtain a light signal having a narrow wavelength spectrum, the external modulation method. in which a light signal emitted from a semiconductor laser is modulated by an optical modulator, is applied. A conventional optical modulator has been described on page 4-193 of "Part 4, Spring term National Conference Record, 1989, The Institute of Electronics, Information and Communication Engineers of Japan", titled as "High performance optical intensity modulator monolithically integrated with a DFB laser". The conventional optical modulator is an electroabsorption type optical modulator which is monolithically integrated with a semiconductor laser. The optical modulator and the semiconductor laser are fabricated on a common substrate having a common electrode on a first surface thereof. The optical modulator comprises a light absorption layer among epitaxial layers grown on a second surface of the substrate, and a modulator electrode provided on a cap layer which is a top layer in the epitaxial layers, and the semiconductor laser comprises an active layer among epitaxial layers grown on the second surface of the substrate, and a laser electrode provided on a cap layer in the epitaxial layers, such that the absorption layer and the active layer are coupled by a butt-joint, and opposite facets of the optical modulator and the semiconductor laser are coated with anti-reflection layers. In operation, the semiconductor laser emits a laser light having a uniform optical intensity and a uniform oscillation wavelength. Then. the optical modulator modulates the intensity of the light signal supplied by the semiconductor laser by changing the absorption coefficient of the optical modulator. By using the optical modulator, the dispersion of the wavelength spectrum of the light signal becomes one fifth of that in a former method in which a semiconductor laser emits a light signal modulated in intensity. Therefore, the transmission distance which is limited by the dispersion of the wavelength spectrum becomes five times as long as that in the former method. In the conventional optical modulator, however, there is a disadvantage in that extension of the wavelength spectrum of the light signal still occurs due to a minute phase modulation generated during the intensity modulation by the optical modulator. WO-A-89/08356 discloses a method and apparatus for modulating a semiconductor laser in which a light frequency is modulated by a differentiating signal of an input signal. The modulated light is applied to a light interference device, from which an intensity-modulated signal is obtained. Telecommunications and Radio Engineering, Vol. 44, No. 7, July 1989, pages 119 to 122 discloses a method of compensating the non-linear distortions of light-emitting and laser diodes in broadband analog communications systems in which a predistortion function is generated which uses its approximation by an exponential polynomial. Journal of Lightwave Technology, Vol. 6, No. 1, January 1988, pages 87 to 93 discusses frequency chirping in external modulators and proposes a general formula which expresses said frequency chirping. It is an object of the invention to provide a method of optical transmission and an optical transmitter used in the same, in which a transmission distance in which correct information is transferred is significantly long. This object is achieved by the method of optical transmission and the optical transmitter according to the claims. The invention will be described in more detail in conjunction with appended drawings, wherein: Fig. 1 is a perspective view illustrating a conventional optical modulator; Fig. 2 is a block diagram of an optical transmitter in a first preferred embodiment according to the invention; Fig. 3 is a timing chart of operation in the first preferred embodiment according to the invention; Fig. 4 is a block diagram of an optical transmitter in a second preferred embodiment according to the invention; and Fig. 5 is a block diagram of an optical transmitter in a third preferred embodiment according to the invention. Before describing a method of optical transmission and an optical transmitter used in the method according to the invention, the conventional optical modulator briefly described before will be explained in conjunction with Fig. 1. Fig. 1 shows the conventional optical modulator. The conventional optical modulator comprises an electroabsorpotion type optical modulator 2 which is monolithically integrated with a semiconductor laser 1. The semiconductor laser 1 and the optical modulator 2 are fabricated on a common semiconductor substrate 11 which is provided with a common electrode 15 on a first surface thereof. The semiconductor laser 1 comprises epitaxial layers including an active layer 12 grown on a second surface of the substrate 11, and a laser electrode 16 provided on a cap layer which is a top layer in the epitaxial layers. In a similar structure, the optical modulator 2 comprises epitaxial layers including a light absorption layer 13 grown on the second surface of the substrate 11, and a modulator electrode 17 provided on a cap layer in the epitaxial layers. The active layer 12 and the absorption layer 13 are coupled to provide an optical coupling therebetween by a butt-joint 14, and opposite facets of the semiconductor laser 1 and the optical modulator 2 are coated with anti-reflection (AR) layers 18. In operation, a predetermined current is applied across the laser and common electrodes 16 and 15 to provide light emitted from the active layer 12, and the light is absorbed in the absorbing layer 13 in accordance with an absorption coefficient changing dependent on a voltage applied across the modulator electrode 17 and the common electrode 15. Thus, an intensity modulated light is obtained from the optical modulator 2. Next, an optical transmitter in a first preferred embodiment according to the invention will be explained in Fig. 2. The optical transmitter comprises a semiconductor laser 1 which generates a laser light signal in accordance with a direct bias current 1b, electroabsorption type optical modulator 2 which modulates an intensity of the light signal supplied from the semiconductor laser 1 in accordance with a modulating signal Im, a delay circuit 5 which supplies the optical modulator 2 with a delayed signal of the modulating signal Im, and a differentiating circuit 3 which supplies the semiconductor laser 1 with a differentiated signal of the modulating signal Im. In operation, the current Ib is supplied to the semiconductor laser 1 to generate a laser light having uniform intensity and wavelength. On the other hand, the delayed signal of the modulating signal Im is supplied to the optical modulator 2, where the intensity of the light supplied from the semiconductor laser 1 is modulated dependent on an electric field to change an optical absorption coefficient of the optical modulator 2 in accordance with the modulating signal Im. In this state, an output light signal Pout which is supplied from the optical modulator 2 will be an intensity modulated signal having an expanded wavelength spectrum because of the wavelength shift caused by a phase modulation, if the differentiating circuit 3 is not provided. In order to cancel the wavelength shift, the differentiated signal of the modulating signal Im is supplied from the differentiating circuit 3 to the semiconductor laser 1 as well as the current Ib. In this case, the light signal generated by the semiconductor laser 1 has a wavelength change corresponding to the wavelength shift which occurs in the optical modulator 2, so that the wavelength shift in the optical modulator 2 is cancelled when the light signal is supplied to the optical modulator 2. As a result, the output light signal Pout has an uniform wavelength. The extension of the wavelength spectrum of the output light signal Pout can be minimized by adjusting a balance between a time in which the modulating signal Im reaches the optical modulator 2 and a time in which the differentiated signal of the modulating signal Im reaches the semiconductor laser 1. In an optical transmission experiment using the optical transmitter in the first preferred embodiment which is carried out under a condition that a wavelength of a light signal is 1.5 µ m and a transmission velocity is 4. 8 Gb/s, it is confirmed that the extension of the wavelength spectrum of the modulated light signal becomes 0. 03 Å , which is approximately one fifth as narrow as that in the conventional method or apparatus, so that an allowable dispersion of the light signal during transmission through an optical fiber becomes 2500 ps/nm, which is five times as wide as that in the conventional method. As a result, an optical transmission over a distance of 120 km using an optical fiber having a characteristic of the wavelength dispersion which is 17 ps/nm · km at a wavelength of 1.55 µm is carried out without any fault of transferred information codes. Fig. 3 is a timing chart of operation in the first preferred embodiment according to the invention. In Fig. 3, the light generated by the semiconductor laser 1 is modulated in intensity by the optical modulator 2 to provide the output light signal Pout as an intensity modulated light signal having a waveform as shown in (A). The wavelength of the intensity modulated light signal Pout changes between + Δ λ and - Δ λ as shown in (B). In order to cancel this wavelength change, a current I added to the bias current Ib which is supplied to the semiconductor laser 1 is changed as shown in (C) to compensate the change in the wavelength of the light signal Pout as shown in (D). As a result, the light signal Pout supplied from the optical modulator 2 has a uniform wavelength as shown in (E). In this case, the wavelength change shown in (B) is proportional to a differentiated value of the intensity of the modulated light signal shown in (A). Therefore, it is able to cancel the wavelength change caused in the optical modulator 2, when the wavelength of the light signal generated by the semiconductor laser 1 is changed by the compensation signal which is a differentiated signal of the modulating signal Im supplied to the optical modulator 2. Consequently, the dispersion of the wavelength spectrum of the intensity modulated light signal supplied by the optical modulator 2 is limited significantly. Fig. 4 is a block diagram of an optical transmitter in a second preferred embodiment according to the invention. A structure of the optical transmitter is the same as that in Fig. 2, except that the electroabsorption optical modulator 2 is replaced by a Mach-Zehnder type optical modulator 4. The Mach-Zehnder type optical modulator 4 comprises two electrodes 20 and 21, and two optical waveguides 22 and 23. In the optical modulator 4, the intensity of the light signal which transmits through the optical waveguides 22 and 23 is modulated by applying an electric field across the electrodes 20 and 21 to change optical path length of the optical waveguides 22 and 23. The operation of the optical transmitter is the same as that in Fig. 2. That is, a modulating signal Im is divided into first and second modulating signals. The first modulating signal is supplied through the delay circuit 5 to the electrode 21 of the Mach-Zehnder type modulator 4, and the second modulating signal is differentiated in the differentiating circuit 3 to be supplied to the semiconductor laser light source 1. In the Mach-Zehnder type modulator 4, a wavelength shift occurs in accordance with a difference between electric fields applied across the optical waveguides 22 and 23. The polarity of the differentiating circuit 3, a delay time of the delay circuit 5, etc. are adjusted, so that a wavelength shift generated in the Mach Zehnder modulator 4 is cancelled to minimize the extension of a wavelength spectrum of the light output Pout. In an optical transmission experiment using the optical transmitter in the second preferred embodiment which is carried out under a condition that a wavelength of a light signal is 1.5 µm and a transmitting velocity is 4.8 Gb/s, it is confirmed that the extension of the wavelength spectrum of the modulated light signal becomes 0.005 nm, which is half as narrow as that in the conventional method or apparatus, so that an allowable dispersion of the light signal during transmission by an optical fiber becomes 5000 ps/nm, which is approximately twice as wide as that in the conventional method. As a result, an optical transmission over a distance of 250 km using an optical fiber having a characteristic of the wavelength dispersion which is 20 ps/nm · km at a wavelength of 1.55 µ m is carried out without any fault of transferred information codes. Fig. 5 is a block diagram of an optical transmitter in a third preferred embodiment according to the invention. The optical transmitter comprises a semiconductor laser 1 which generates a laser light in accordance with a direct bias current Ib, an electroabsorption type optical modulator 2 to modulate an intensity of the light supplied from the semiconductor laser 1 in accordance with a modulating signal Im, and a differentiating circuit 3 which supplies the semiconductor laser 1 with a differentiated signal of a clock signal CLK. In this preferred embodiment, any circuit having a function of generating a differentiated signal of the clock signal CLK can be used as the differentiating circuit 3. For instance, the differentiating circuit 3 may be a phase shift circuit in a case that the clock signal CLK is a sine wave. In operation, the differentiating circuit 3 supplies a differentiated signal of the clock signal CLK to the semiconductor laser 1 in addition to a direct bias current Ib to generate a laser light signal having a compensating wavelength in accordance with a frequency of the clock signal CLK. On the other hand, the modulating signal Im which is a RZ code signal is supplied to the optical modulator 2 to modulate an intensity of the light signal supplied from the semiconductor laser 1. In this case, the differentiating circuit 3 supplies the differentiated signal by adjusting a time constant to change the wavelength of the light signal to cancel the wavelength change of the light signal during the modulation in the optical modulator 2 to minimize extension of the wavelength spectrum of the output light signal Pout. As the modulating signal Im is a RZ code signal, when the modulating signal Im is zero, the optical output Pout becomes also zero, so that the output light signal Pout is not affected by the wavelength change of the light signal supplied from the semiconductor laser 1. In an optical transmission experiment using the optical transmitter in the third preferred embodiment which is carried out under a condition that a wavelength of a light signal is 1.5 µ m and a transmission velocity is 4. 8 Gb/s, it is confirmed that the extension of the wavelength spectrum of the modulated light signal becomes one fifth as narrow as that in the conventional method or apparatus, and an allowable dispersion of the light signal during transmission by an optical fiber becomes 2000 ps/nm. As a result, an optical transmission over a distance of 120 km using an optical fiber having a characteristic of the wavelength dispersion which is 17 ps/nm · km at a wavelength of 1.55 µ m is realized with excellent transmission characteristics. Although the invention has been described with respect to specific embodiments for complete and clear disclosure, the appended claims are not to thus limited and alternative constructions may occur to one skilled in the art which fairly fall within the basic teaching herein set forth. For instance, any optical modulator is applicable in the invention instead of an electroabsorption type optical modulator and a Mach-Zehnder optical modulator, as far as the optical modulator is such that the wavelength change during the intensity modulation can be indicated as a differentiated signal of the modulation signal. Furthermore, the operation of differentiation in the differentiating circuit can be conducted by adjusting a polarity, a time constant, etc., in accordance with types of optical modulators used in an optical transmission and a transmission velocity of information.

Claims: A method of optical transmission, comprising the steps of: applying a laser input signal to a semiconductor laser (1) to emit a laser light having a predetermined wavelength; and supplying a modulating signal to an optical modulator (2) to modulate said laser light, thereby generating a modulated output light signal having a first wavelength change relative to said predetermined wavelength, characterized in that said method comprises the steps of: differentiating said modulating signal to generate a differentiated signal; and combining said differentiated signal to said laser input signal to generate a compensating laser input signal; wherein in the step of applying said laser input signal said compensating laser input signal is applied to said semiconductor laser (1) to emit said laser light having a second wavelength change relative to said predetermined wavelength, said second wavelength change cancelling said first wavelength change. A method of optical transmission, according to claim 1, wherein: said laser light is modulated dependent on an optical absorption coefficient which is changed by applying an electric field in accordance with said modulating signal. A method of optical transmission, according to claim 1, wherein: said laser light is modulated dependent on an optical length of optical waveguides which is changed by applying an electric field in accordance with said modulating signal. A method of optical transmission, according to any of claims 1 to 3, further comprising a step of: generating a delayed signal of said modulating signal; wherein said modulating of said laser light is carried out in accordance with said delayed signal, so that a wavelength change of said laser light coincides with a wavelength change which occurs during said modulating step. An optical transmitter, comprising: a semiconductor laser (1) for emitting a laser light having a predetermined wavelength by receiving a laser input signal; and an optical modulator (2) for modulating said laser light in accordance with a modulating signal to generate a modulated output light signal having a first wavelength change relative to said predetermined wavelength; characterized in that said optical transmitter comprises: a differentiating circuit (3) for differentiating said modulating signal to generate a differentiated signal; and means (6) for combining said differentiated signal to said laser input signal to generate a compensating laser input signal; wherein said semiconductor laser (1) is applied with said compensating laser input signal instead of said laser input signal to emit said laser light having a second wavelength change relative to said predetermined wavelength, said second wavelength change cancelling said first wavelength change. An optical transmitter, according to claim 5, wherein: said optical modulator (2) is an optical modulator selected from an electroabsorption type optical modulator and a Mach-Zehnder type optical modulator. An optical transmitter, according to claim 5 or 6, further comprising: means (5) for generating a delayed signal of said modulating signal for supplying to said optical modulator (2); wherein said optical modulator (2) modulates said laser light in accordance with said delayed modulating signal, so that a wavelength change of said laser light coincides with the wavelength change which occurs during intensity modulation. A method of optical transmission, comprising the steps of: applying a laser input signal to a semiconductor laser (1) to emit a laser light having a predetermined wavelength; and supplying a modulating signal to an optical modulator (2) to modulate said laser light, thereby generating a modulated output light signal having a first wavelength change relative to said predetermined wavelength, characterized in that said method comprises the steps of: differentiating a clock signal to generate a differentiated signal; and combining said differentiated signal to said laser input signal to generate a compensating laser input signal; wherein in the step of applying said laser input signal said compensating laser input signal is applied to said semiconductor laser (1) to emit said laser light having a second wavelength change relative to said predetermined wavelength, said second wavelength change cancelling said first wavelength change. A method of optical transmission, according to any of claim 8, wherein: said modulating signal is a RZ code signal. An optical transmitter, comprising: a semiconductor laser (1) for emitting a laser light having a predetermined wavelength by receiving a laser input signal; and an optical modulator (2) for modulating said laser light in accordance with a modulating signal to generate a modulated output light signal having a first wavelength change relative to said predetermined wavelength; characterized in that said optical transmitter comprises: a differentiating circuit (3) for differentiating a clock signal to generate a differentiated signal; and means (6) for combining said differentiated signal to said laser input signal to generate a compensating laser input signal; wherein said semiconductor laser (1) is applied with said compensating laser input signal instead of said laser input signal to emit said laser light having a second wavelength change relative to said predetermined wavelength, said second wavelength change cancelling said first wavelength change.

Inventors: HENMI NAOYA, SUZAKI TETSUYUKI, HENMI, NAOYA,, SUZAKI, TETSUYUKI,, HENMI, NAOYA, C/O NEC CORPORATION, SUZAKI, TETSUYUKI, C/O NEC CORPORATION
Applicants: NIPPON ELECTRIC CO, NEC CORPORATION
Application year: 1990
Main classification: H04B10
IPC codes: H04B10, H01S5