8.6 5.2 19.19 19.23 Staff Site Universitas Negeri Yogyakarta

ISSN 2086-5953 Figure 2. The uniformity of p-metal contact on the top of the ridge and good isolation layer SiO 2 underneath. 3 EXPERIMENTAL RESULTS There are several ways to analyze a tapered waveguide in order to see the amount of loss that occurs. But, from several different techniques that have been used to analyze taper structures, a general consensus has been made that if a taper is made long enough and has gradual enough taper slope , the taper can have low loss. It has been observed that taper lengths which are on the order of hundreds of microns can achieve high output power and small threshold current, and also the circular optical beam mode [7]. Table 1 and Table 2 show two samples characteristics of the total output power and threshold current for the total laser cavity length vary from 400-700 m and 600-900 m, respectively. These results verify that for the 200 m taper length with 500 m cavity laser gives the smaller threshold current and higher output power. And for the 500 m taper length with 800 m cavity laser also gives the smaller threshold current and higher output power. Also, for the same cavity lengths 600 and 700 m with different taper lengths show the matching results with the previous above analysis. Table 3 shows the best divergence angles of those FP lasers are 19 o x 19 o for lateral and vertical directions, respectively. Table 1. Threshold current and output power characteristics for 200 m taper length. Total cavity length [ m] Threshold current [mA] Resistance [ ] Output power [mW] 400 40 22.8 2.4 500 22

16.8 8.6

600 26 23.3 2.7 700 32 20.8 6.6 Table 2. Threshold current and output power characteristics for 500 m taper length. Total cavity length [ m] Threshold current [mA] Resistance [ ] Output power [mW] 600 54 29 1.4 700 36 19.3 4.1 800 33

25.2 5.2

900 33 25.7 3.8 Table 3. Divergence Angles Measurement Results No facet coatings Cavity Length µm Taper Region µm Divergence Angle deg FWHM=2α 200 100 22.25 22.06 500 200

19.48 19.19

700 200 21.89 22.19 800 500

19.37 19.23

Theoretical model for injection-locking FP- LD which shows the dynamic characteristics with external injected narrow-band ASE light based on the rate equations for the semiconductor laser diode refers to Ref [8]. This model was solved numerically by fourth-order Runge-Kutta method. The simulation has been done and the calculated optical spectra of the wavelength-locked FP-LD has was shown below Figure 3. Figure 3. Simulated optical spectra of the wavelength-locked FP-LD [7]. By understanding the theoretical model that described above, we performed some experiments for injection-locking technique. When we do not inject the external light into the laser, the taper FP-LD shows multimode output. But, when an external narrowband optical signal is injected into the multi-longitudinal mode laser such as vertical taper FP-LD, the lasing mode can be locked to a single mode. The external optical signal from tunable laser diode acts as a seed for laser oscillation in the FP cavity; moreover, the mode that is nearest to the peak wavelength of the ISSN 2086-5953 injected optical signal will be locked to the injected light, and other modes will be suppressed Figure 4. To increase the injection efficiency, we may need the antireflection coating AR-coating on the front facet of the laser. Here, for injection-locking, we used a FP-LD chip with 500 µm of total cavity length including 200 µ m taper and 300 µm laser section with 5 of front facet reflectivity. Figure 4. Measured optical spectra of the vertical taper FP-LD w and wo injection-locking. 4 CONCLUSION The fabricated of vertical down-tapered ridge waveguide FP-LD was extremely smooth using a simple and low-cost diffusion-limited etching method. The overall device length is 500 µ m, comprising the laser section 300 µm and taper length 200 µ m produced 8.6 mW output power and 16 slope efficiency and 19 o x 19 o divergence angles for lateral and vertical which potentially can be used as a low-cost light source for WDM-PON based on injection-locking technique. More than 30 dB SMSR was achieved at 100 mA bias current. ACKNOWLEDGEMENT This project was supported by National Science Council under grant of NSC97-2219-E- 011-004. REFERENCES [1] Banerjee A, Park Y, Clarke F and Song H, Yang S, Kramer G, Kim K, and Mukherjee B 2005 Wavelength-division-multiplexed passive optical network WDM-PON technologies for broadband access: a review [Invited]. Journal of Optical Networking 4: 737-757. [2] Park S.-J, Lee C.-H, Jeong K.-T, Park H.-J, Ahn J.-G, and Song K.-H 2004 Fiber-to-the- home services based on wavelength-division- multiplexing passive optical network. Journal of Lightwave Technology 22: 2582-2591. [3] Banerjee A, Park Y, Clarke F and Song H, Yang S, Kramer G, Kim K, and Mukherjee B 2005 Wavelength-division-multiplexed passive optical network WDM-PON technologies for broadband access: a review [Invited]. Journal of Optical Networking 4: 737-757. [4] Park S.-J, Lee C.-H, Jeong K.-T, Park H.-J, Ahn J.-G, and Song K.-H 2004 Fiber-to-the- home services based on wavelength-division- multiplexing passive optical network. Journal of Lightwave Technology 22: 2582-2591. [5] An F T, Kim K S, Hsueh Y L, Rogge M, Shaw W T, and Kazovsky L G 2003 Evolution, challenges and enabling technologies for future WDM-based optical access networks. Proceeding 2nd Symposium of Photonic Network Computing, Cary, NC, September, 2003. [6] Kazovsky L.-G, Shaw W.-T, Guiterrez D, Cheng N, and Wong S.-W 2007 Next- generation optical access networks. Journal of Lightwave Technology 25: 3428-3442. [7] Jeon H, Verdiell J.-M, Ziari M, and Mathur A 1997 High power low-divergence semiconductor lasers for GaAs-based 980-nm and InP-based 1550-nm applications. Journal of Selected Topics in Quantum Electronics 3: 1344-1350. [8] Simatupang J. W, Wu W. S, and Lee S. L 2009 The Study of relative etching rate of masked InPInGaAsP in fabrication of vertical taper-waveguide by diffusion-limited etching, Proceeding of ICOMMET, Graha ITS- Surabaya, Indonesia, June 24-25, 2009, MI-26. [9] Fan R. S, and Hooker R. B 1999 Tapered polymer single-mode waveguides for mode transformation. Journal of Lightwave Technology 17: 466-474. [10] Park K.-Y, Mun S.-G, Choi K.-M, and Lee C.- H 2005 A Theoretical model of a wavelength-locked fabry-perot laser diode to the externally injected narrow-band ASE. IEEE Photonics Technology Letter 17: 1797-1799. 77 ISSN 2086-5953 MANAGEMENT DECISION MAKING FOR EXTENDED CROW METHOD TO PREDICT RELIABILITY OF SHIP OIL SYSTEM Syamsuri 1 , Tungga Bhimadi 2 1 Department of Mechanical Engineering National Taiwan University of Science and Technology 2 Department of Naval Engineering Sepuluh Nopember Institute of Technology Email: syam_sby2003yahoo.com 1 , tunggabhimadiyahoo.com 2 ABSTRACT Method and procedure selection to recalculate the component and sub system reliability growth after their failures have challenged researchers for satisfaction collaborating and regulation of operating system. Reliability level was proposed compliance with: temporary using, paralel circuit as stand by, impulsive system, real caused by routine maintenance, and Management Decision Making MDM in repairing sub system or replacement component. This paper was reliability growth approach using Reliability Growth of Extended Crow RGEC method. Management decision that proposed are: scheduling in harmony, using non standard component, handling after hazard, and using component or system resulted from innovation. Time to Failure TTF data are needed to predict reliability growth of ship oil system until its damage. The mean value of reliability was 64.3, and reliability level was 0.15 for 25 years operation until the end of life time system. Keywords: Reliability Growth of Extended Crow, Management Decision Making, Time to Failure. 1 INTRODUCTION

1.1 Motivation