The new concept of single-mode resonator for single-frequency distributed feedback (DFB) lasers is presented. This concept is based on embedded nonharmonic distributed Bragg structure with sinusoidally modulated coupling coefficient, which is a combination of two superimposed sinusoidal Bragg gratings of equal heights and slightly different periods. Resonant frequencies and corresponding threshold gains of such distributed resonator are calculated theoretically by using the coupled-mode theory. The designed resonator provides stable single-frequency oscillation and has lasing characteristics (frequencies and thresholds) very similar to those of well-known distributed resonator with quarter-wavelength shift. The developed concept of resonator with sinusoidally modulated coupling coefficient can be applied both to semiconductor laser diodes with incorporated Bragg relief grating and to DFB fiber lasers with refractive index grating. The important advantage of designed new single-mode Bragg structure, as compared to quarter-wavelength-shifted structure, is that it can be fabricated very easily on semiconductor surfaces and in photosensitive fibers by direct three-beam holographic writing.
. INTRODUCTIONDistributed feedback (DFB) semiconductor and fiber lasers with incorporated submicron Bragg relief or refractive index grating are widely used in optoelectronics and integrated optics as reliable sources of narrow-band coherent radiation for 1 .3 -1 . 5 um wavelength region. They possess very high degree of spectral selectivity due to very narrow frequency bandwidth of Bragg resonance. For example, DFB fiber laser with embedded sinusoidal index grating provides two-mode oscillation with resonant frequencies w1 and w1 slightly above and below the Bragg frequency WBr, the frequency interval &o = w1 -(Oi between these modes being Aw/WB. A/Ln, where i% is lasing wavelength, L is resonator length, n is effective mode index.4'6The progress of integrated optics and long-haul fiber communication networks imposes new hard requirements on lasing characteristics of DFB laser sources and among them the requirement of stable single-frequency oscillation is of great importance. It is well known2'3'5'6 that DFB lasers with incorporated harmonic Bragg grating (of sinusoidal, triangular, trapezoidal form, etc) can not provide single-frequency oscillation, since in this case two modes of different frequencies in the vicinity of WBr have equal thresholds. Various methods were developed to achieve the stable singlefrequency oscillation of DFB lasers. One of these methods, which is widely used now, is the utilization of distributed resonator with quarter-wavelength shift.2'7 Such distributed resonator consists of two sections with embedded harmonic Bragg gratings of equal periods d and depths h, having phase shift r at the centre of laser cavity, which results in stepped modulation of coupling coefficient along the resonator. In this case the mode with w = WBr has the lowest threshold. It provides the stable single-mode oscillation at Bra...