Tài liệu Laser điốt được phân phối thông tin phản hồi và các bộ lọc du dương quang P5 pdf

5 Threshold Analysis and Optimisation of Various DFB LDs Using the Transfer Matrix Method 5.1 INTRODUCTION In the previous chapter, the transfer matrix method (TMM) was introduced to solve the coupled wave equations in DFB laser structures. Its efficiency and flexibility in aiding the analysis of DFB semiconductor LDs has been explored theoretically. A general N-sectioned DFB laser model was built which comprised active/passive and corrugated/planar sections. In this chapter, the N-sectioned laser model will be used in the practical design of the DFB laser. The spatial hole burning effect (SHB) [1] has been known to limit the performance of DFB LDs. As the biasing current of a single quarterly-wavelength-shifted (QWS) DFB LD increases, the gain margin reduces. Therefore, the maximum single-mode output power of the QWS DFB LD is restricted to a relatively low power operation. The SHB phenomenon caused by the intense electric field leads to a local carrier depletion at the centre of the cavity. Such a change in carrier distribution alters the refractive index along the laser cavity and ultimately affects the lasing characteristics. By changing the structural parameters inside the DFB LD, an attempt will be made to reduce the effect of SHB. As a result, a larger single-mode power, and consequently a narrower spectral linewidth, may be achieved. A full structural optimisation will often involve the examination of all possible structural combinations in the above-threshold regime. On the other hand, the analysis of the structural design may be simplified, in terms of time and effort, by optimising the threshold gain margin and the field uniformity. The structural changes and their impacts on the characteristics of DFB LDs will now be presented. By introducing more phase shifts along the laser cavity, a three-phase-shift (3PS) DFB LD will be investigated in section 5.2. In particular, impacts due to the variation of both phase shifts and their positions on the lasing characteristics of the 3PS DFB LD will be discussed. To reduce the SHB effect, it is necessary to have a more uniform field distribution, whilst maintaining a large gain margin ðÁLÞ. The optimised structural design for the 3PS DFB laser based on the values of ÁL and the flatness (F) of the field distribution will be discussed in section 5.3 [2]. Distributed Feedback Laser Diodes and Optical Tunable Filters H. Ghafouri–Shiraz # 2003 John Wiley & Sons, Ltd ISBN: 0-470-85618-1 By changing the height of the corrugation and thus the coupling coefficient along a DFB laser cavity, a distributed coupling coefficient (DCC) DFB laser can be built. In section 5.4, the threshold characteristics of this structure will be shown. In particular, effects due to the variation of the coupling ratio and the position of the corrugation change will be investigated. To maintain a single-mode oscillation, a single phase shift is introduced at the centre of the cavity. By changing the value of the phase shift, the combined effect with the non-uniform coupling coefficient will be presented. Optimised structural combinations that satisfy both a high gain margin and a low value of flatness will be selected for later use in the above-threshold analysis. In section 5.5, the combined effect of both multiple phase shifts and non-uniform coupling coefficients will be investigated using a DCC þ 3PS DFB laser structure. Finally, a summary will be presented at the end of this chapter. 5.2 THRESHOLD ANALYSIS OF THE THREE-PHASE-SHIFT (3PS) DFB LASER By introducing more phase shifts along the laser cavity, it has been shown [3–5] that the spatial hole burning effect can be reduced in a 3PS DFB LD which is characterised by a more uniform internal field distribution. Experimental measurement has been carried out [5] using a fixed value of phase shift. However, independent changes in the value of phase shift have not been fully explored. Using the TMM, it was shown in Table 4.1 of Chapter 4 that four transfer matrices are necessary to determine the threshold condition of 3PS DFB lasers. In Fig. 5.1, a schematic diagram of the 3PS DFB laser structure is shown. In the figure,  2 ,  3 and  4 represent phase shifts and the length of each smaller section is labelled L j ð j ¼ 1; 2Þ. In the analysis, zero facet reflection at the laser facets is assumed. Following the formulation of the transfer matrix method, the overall transfer matrix of the 3PS DFB laser becomes: Y z 5 j z 1 ðÞ¼F ð4Þ F ð3Þ F ð2Þ F ð1Þ ¼ y 11 z 5 j z 1 ðÞy 12 z 5 j z 1 ðÞ y 21 z 5 j z 1 ðÞy 22 z 5 j z 1 ðÞ  ð5:1Þ where F ð jÞ ð j ¼ 1 to 4) corresponds to the transfer matrix of each smaller section. For a mirrorless cavity, the threshold condition can be found by solving the following equation y 22 z 5 j z 1 ðÞ¼0 ð5:2Þ Figure 5.1 Schematic diagram showing a 3PS DFB LD. 124 THRESHOLD ANALYSIS AND OPTIMISATION OF VARIOUS DFB LD S Using a numerical approach such as Newton–Raphson’s method [6] for analytical complex equations, the threshold equation above may be solved. Figure 5.2 shows the resonance modes obtained from a symmetrical 3PS DFB laser where  2 ¼  3 ¼  4 ¼ =2 and L 1 ¼ L 2 are assumed. For comparison purposes, results obtained from a mirrorless conventional DFB laser and a single =2 phase-shifted DFB laser are also included. In all three cases, the coupling coefficient and the overall laser cavity length L are fixed at 40 cm À1 and 500 mm, respectively. Oscillation modes at the Bragg wavelength are found for both the single =2 and a 3PS DFB structure. However, the Bragg resonance mode of the 3PS DFB laser does not show the smallest amplitude threshold gain. Instead, degenerate oscillation occurs since it is shown that both the À1 and þ1 modes share the same value of amplitude threshold gain. It is interesting to see how a single =2 phase shift enables SLM operation whilst multi- mode oscillation occurs in the case where there are three phase shifts, i.e. f=2;=2;=2g. The pair of braces fgused hereafter will indicate a phase combination in the 3PS structure, that is f 2 ; 3 ; 4 g. 5.2.1 Effects of Phase Shift on the Lasing Characteristics In order that stable SLM operation can be achieved in the 3PS DFB laser, one must change the value or the position of the phase shift. Figure 5.3 shows oscillation modes of various 3PS DFB laser structures. In the analysis, the values of the three phase shifts are assumed to be equal and the phase shift positions are the same as in Fig. 5.2. A shift of resonance mode can be seen when all phase shifts change from =2to2=5. The þ1 mode which demonstrates the smallest amplitude threshold gain will become the lasing mode after lasing Figure 5.2 Resonance modes of various DFBs that include: (a) a conventional DFB laser diode; (b) a single QWS DFB laser diode; (c) a three /2-phase-shifted DFB laser diode. THRESHOLD ANALYSIS OF THE THREE-PHASE-SHIFT (3PS) DFB LASER 125 threshold is reached. On the other hand, the À1 mode will become the lasing mode when the three phase shifts change from =2to3=5. With all three phase shifts displaced from the usual =2 values, SLM can be achieved in the 3PS DFB LD. 5.2.2 Effects of Phase Shift Position (PSP) on the Lasing Characteristics The 3PS DFB laser structure we have discussed so far is said to be symmetrical. For a cavity length of L, the position of phase shifts is assumed in such a way that L 1 ¼ L 2 ¼ L=4. To investigate the effect of the phase shift position (PSP) on the threshold characteristics, a position factor is introduced such that ¼ L 1 L 1 þ L 2 ¼ 2L 1 L ð5:3Þ where  3 is assumed to be located at the centre of the cavity. Using the above equation, it should be noted that both ¼ 0 and ¼ 1 correspond to a single-phase-shifted DFB laser structure. In Fig. 5.4, the variation of the amplitude threshold gain is shown with the position factor for different values of normalised coupling coefficient L. All the phase shifts are fixed at  2 ¼  3 ¼  4 ¼ =3. At a fixed value of , the figure shows a decrease in amplitude threshold gain as the L value increases. Along the curve L ¼ 1:0, discontinuities at ¼ 0:12 and ¼ 0:41 indicate possible changes in the oscillation mode. Figure 5.3 Resonance modes in various 3PS DFBs that include: (a) a f=2, =2, =2g 3PS DFB laser; (b) a f2=5; 2=5; 2=5g 3PS DFB laser; (c) a f3=5; 3=5; 3=5g laser. 126 THRESHOLD ANALYSIS AND OPTIMISATION OF VARIOUS DFB LD S Figure 5.5 The variation of detuning coefficient with respect to the phase shift position for coupling coefficient . Figure 5.4 The change of amplitude gain with respect to the phase shift position for different values of coupling coefficient . Such a change in oscillation is confirmed when the relationship between the detuning coefficient and the position factor is shown in Fig. 5.5. Along L ¼ 1:0, it can be seen that the À1 mode remains as the oscillation mode when increases from zero. When ¼ 0:12 is reached, however, a sudden change of oscillation mode is observed. Similar mode jumping occurs at ¼ 0:41. When the PSP shifts, there is a continuous change in the resonant cavity formed by the DFB laser such that the actual lasing mode may alter. At ¼ 0:77, it is interesting to see how all L values converge to the same lasing wavelength. It appears that at this particular phase shift position, the effect of the variation of L is irrelevant and the lasing characteristic depends on the presence of the =3 phase shifts. 5.3 OPTIMUM DESIGN OF A 3PS DFB LASER STRUCTURE A complete structural optimisation of MPS DFB lasers cannot be achieved without analysing the above-threshold performances. This involves solving the carrier rate equation, which is a fairly complex process and needs intensive computation. On the other hand, it is believed that the complexity of the structural design in the 3PS DFB laser can be reduced by optimising the threshold amplitude gain difference and the flatness of field distribution. Hence, we can simply concentrate on those structures satisfying these design criteria. For a high-performance DFB LD, both a stable single-mode oscillation and a uniform field distribution are important to prevent LDs from being affected by the spatial hole burning effect. In our analysis, DFB laser structures having a high gain margin ðÁLÞ are considered, whilst the spatial hole burning effect is included by analysing the corresponding effects on field uniformity. Reports by Kimura and Sugimura [3– 4] as well as Ogita et al. [5] suggested that the lasing characteristics are strongly influenced by both and . To maintain a stable SLM oscillation, and consequently improve the performance of the spectral linewidth, these structural parameters need to be optimised. 5.3.1 Structural Impacts on the Gain Margin To achieve a stable laser source that oscillates at a single longitudinal mode, it is important that there is a gain margin ÁL > 0:25½1. In the analysis, we assumed the length of the laser L to be 500 mm. For a 3PS DFB LD, Fig. 5.6 shows the relationship between the gain margin and the phase shift  in a symmetrical structure for different values of L ranging from 1 to 3. The position factor ¼ 0:5 corresponds to the case where L 1 ¼ L 2 ¼ L=4. In all cases, the degenerate oscillations occur at  ¼ 0, =2 and , and the distributions of gain margins are symmetrical with respect to  ¼ =2. It is also shown that the variation of L has little effect on the gain margin of the 3PS laser structure. Along the line L ¼ 1, it is found that a stable laser having ÁL > 0:25 can be obtained provided that 47  <<73  or 107  <<133  . In Fig. 5.7, a contour map is shown that relates the gain margin to the values of phase shifts in three-phase-shift  2 ; 3 ; 4 fg DFB LDs. In the calculations, L ¼ 2 and ¼ 0:5 are assumed. The phase shift  3 introduced at the centre of the cavity is separated from the rest so that its value can be selected independently. Other phase shifts are assumed to be equal as  2 ¼  4 ¼  side . As stated earlier, to satisfy the requirement of ÁL > 0:25,  side must either be greater than 105  or less than 80  if  3 can be varied freely between 0 and . A maximum 128 THRESHOLD ANALYSIS AND OPTIMISATION OF VARIOUS DFB LD S Figure 5.6 Variation of the gain margin versus the phase shift for different coupling coefficients. Figure 5.7 Relationship between the gain margin ÁL and phase shifts for a 3PS DFB laser diode. value of ÁL ¼ 0:73 is obtained at f0;=2; 0g and f; =2;g which corresponds to a single =2-phase-shifted DFB laser. The variation of ÁL with respect to the position factor is shown in Fig. 5.8. In this figure, the values of phase shifts are equal (i.e.  2 ¼  3 ¼  4 ¼ ) and three different sets of results are calculated with  ¼ =2, 2=5 and =3. By changing the values of the phase shifts, ÁL also changes for each particular value of . At a fixed phase shift  ¼ =2 (solid line), it is shown that a non-zero value of gain margin is observed where <0:13 and >0:725. As approaches zero, the phase shifts  2 and  4 move towards the laser facets and their contributions become less influential. Also, as approaches unity, both  2 and  4 move towards the central phase shift  3 . In this case, the 3PS laser structure is reduced to a single-phase-shifted structure and the lasing characteristic is described by an effective phase shift of  eff %  2 þ  3 þ  4 . Figure 5.9 shows the dependence of ÁL upon for different values of L. In the analysis, all phase shifts are assumed to be identical (i.e.  ¼ =3). From this figure, it is clear that L has little effect on ÁL in 3PS DFB lasers. 5.3.2 Structural Impacts on the Uniformity of the Internal Field Distribution In this section, the structural impact on the internal field distribution will be discussed. To quantify the uniformity of the field distribution, it was shown in Chapter 3 that the flatness Figure 5.8 Variation of the gain margin versus for various 3PS DFB laser diode structures. 130 THRESHOLD ANALYSIS AND OPTIMISATION OF VARIOUS DFB LD S (F) of the internal field of a general N-sectioned DFB laser cavity is defined as F ¼ 1 L Z z Nþ1 z 1 ðIðzÞÀI avg Þ 2 dz ð5:4Þ where IðzÞ is the electric field intensity along the longitudinal axis and I avg is its average value. In the above equation, a zero value of F corresponds to a completely uniform field. In order to minimise the effects of longitudinal spatial hole burning, it has been shown experimentally ½1; 7 that a DFB laser cavity with F < 0:05 is necessary for stable SLM oscillation. To optimise the structural design of 3PS DFB lasers, F < 0:05 will be used as one of the design criteria. In order to evaluate the flatness of the internal field distribution, the threshold equation of the 3PS DFB laser needs to be solved first. The normalised amplitude threshold gain  th L and the normalised detuning coefficient  th L of the lasing mode are then used to determine the field distribution. In our analysis, a 500 mm long DFB laser is subdivided into a substantial number of small sections with equal length. From the output of each transfer matrix, both the forward and the backward propagating electric fields can be determined, and the electric field intensity at an arbitrary position z 0 is found to be Iðz 0 Þ¼ E R ðz 0 Þ jj 2 þ E S ðz 0 Þ jj 2 ð5:5Þ Figure 5.9 Variation of the gain margin versus for different coupling coefficients. OPTIMUM DESIGN OF A 3PS DFB LASER STRUCTURE 131 In Fig. 5.10, the internal field distributions of three different structures are shown. These structures include a conventional mirrorless, a single =2-phase-shifted and a three-phase- shift f=3;=3;=3g DFB laser. All the electric field distributions have been normalised so that the intensity at the laser facets is unity. It can be seen that the single =2-phase-shifted DFB laser has a flatness value of F ¼ 0:301. Such a high value of F (which means that the field is highly non-uniform) induces a local carrier escalation near the centre of the cavity after the laser threshold is reached, consequently affecting the single-mode stability of the laser device. With three phase shifts incorporated into the cavity, the intensity distribution spreads out and the overall distribution becomes more uniform (see dashed line with F ¼ 0:012Þ. By optimising the values and the positions of the phase shifts with respect to the flatness, a 3PS DFB laser can maintain a uniform field distribution even at a high value of L, which is necessary to reduce the spectral linewidth of the laser. The effect of on F is shown in Fig. 5.11 for different combinations of L. When small values of L ð< 1:5Þ are used, the field intensity distribution becomes less uniform when the phase shifts  2 and  4 shift towards the laser facets (i.e. as tends to 0). As the optical feedback becomes stronger with increasing L, the field intensity distribution becomes more intense near the centre of the laser cavity where is found to be about 0.77. The contour map shown in Fig. 5.12 can be used to optimise the value of phase shifts with respect to F. In a similar way to Fig. 5.7, the central phase shift  3 is used as the x-axis and other phase shifts are represented in the y-axis. In this figure, all phase combinations with F < 0:05 form a ribbon shape stretching from the lower left-hand corner to the upper right- hand corner of the contour. The worst case, which leads to the largest value of F, can be Figure 5.10 Field distribution in various DFB laser diode structures. 132 THRESHOLD ANALYSIS AND OPTIMISATION OF VARIOUS DFB LD S [...]... laser cavity having a longitudinal variation of is achieved With a %=2 phase shift fabricated at the centre of the cavity, oscillation at the Bragg wavelength is ensured In the analysis, a constant corrugation period of à and hence a fixed Bragg wavelength !B is assumed The DCC laser structure used is different from the continuouspitch-modulated (CPM) DFB laser [10] in which à is varying along the laser. .. 500 mm length laser cavity With more phase shifts introduced along the laser cavity, a 3PS DFB LD was shown to have an improved field uniformity By changing the corrugation height along the laser cavity, the DCC þ QWS DFB LD shows an improved threshold gain and field flatness The combined effect of having 3PS and a non-uniform coupling coefficient was investigated in a novel DCC þ 3PS DFB laser structure... asymmetric three phase shift distributed feedback laser diode, Microwave and Optic Technol Lett., 7(18), 827–831, 1994 9 Kotaki, Y., Matsuda, M., Fujii, T and Ishikawa, H., MQW-DFB lasers with nonuniform-depth !=4 shifted gratings, Proc ECOC/ICOC 91, pp 137–140, 1991 10 Okai, M., Tsuchiya T., Uomi, K., Chinone, N and Harada, T., Corrugation-pitch-modulated MQWDFB laser with narrow spectral linewidth (170 kHz),... assumed When 1 increases, both thL and ÁL show a monotonic decrease in value The reduction in thL is obvious since a larger 1 implies a stronger optical feedback and consequently smaller amplitude threshold gain At À1 1 ¼ 2:0 mm , the corrugation becomes uniform and the DCC laser is reduced to the uniform QWS DFB laser Figure 5.17 Variations of both the amplitude threshold gain and the gain margin... DISTRIBUTED COUPLING COEFFICIENT DFB LD a parameter known as the averaged coupling coefficient laser structure such that avg ¼ 1 ðCPÞ þ 2 ð1 avg 139 is introduced into the DCC À CPÞ ð5:7Þ where 1 and 2 are the coupling coefficients inside the DCC laser cavity and CP is the position of the corrugation change For a 500 mm long laser cavity, avg is assumed to be 4:0 mmÀ1 so that the value avg L ¼ 2:0 can be maintained... the position and the value of phase shift in the DCC þ 3PS laser structure, the optimised design obtained from the uniform 3PS DFB laser was used From the hatched area shown in Fig 5.13, all phase shifts are assumed to be %=3 and PSP ¼ 0:5 will be used in the analysis of the DCC þ 3PS laser structure THRESHOLD ANALYSIS OF THE DCC þ 3PS DFB LASER STRUCTURE Figure 5.24 Variation of the gain margin versus... suppressed The gain margin of the 3PS DFB laser, however, is reduced as compared with the QWS DFB laser, whilst oscillation at the Bragg wavelength cannot be maintained To improve the lasing characteristics of the QWS, a novel structure having a non-uniform coupling coefficient has been proposed [9] Basically, a corrugation having non-uniform depth is fabricated along the laser cavity Since the coupling coefficient... distributed feedback semiconductor laser diodes at threshold using the transfer-matrix method (TMM), Semi Sci and Technol., 8(5), 1126–1132, 1994 3 Kimura, T and Sugimura, A., Coupled phase-shift distributed-feedback lasers for narrow linewidth operation, IEEE J Quantum Electron., QE-25(4), 678–683, 1989 4 Kimura, T and Sugimura, A., Narrow linewidth asymmetric coupled phase-shift DFB lasers, Trans IEICE.,... phase shift for a 3PS DFB laser diode 3 ¼ 20 and ¼ 0:3 are assumed Figure 5.15 Relationship between the flatness and the phase shift for a 3PS DFB laser diode 3 ¼ 20 and ¼ 0:3 are assumed 136 5.4 THRESHOLD ANALYSIS AND OPTIMISATION OF VARIOUS DFB LDS THRESHOLD ANALYSIS OF THE DISTRIBUTED COUPLING COEFFICIENT (DCC) DFB LD By incorporating more phase shifts along the DFB laser cavity, 3PS DFB LDs... introduced along the laser cavity, the 3PS structure has been shown to have an improved field uniformity In this section, the combined effect of both non-uniform and 3PS on the threshold characteristics of DFB LDs will be investigated Figure 5.23 Schematic diagram of a distributed coupling coefficient DFB LD with three phase shifts (DCC þ 3PS) A schematic diagram of such a combined DCC þ 3PS DFB laser . assumed. The DCC laser structure used is different from the continuous- pitch-modulated (CPM) DFB laser [10] in which  is varying along the laser cavity DFB laser diode; (b) a single QWS DFB laser diode; (c) a three /2-phase-shifted DFB laser diode. THRESHOLD ANALYSIS OF THE THREE-PHASE-SHIFT (3PS) DFB LASER