Edwin Jan Klein - Universiteit Twente

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D. H. Geuzebroek, E. J. Klein, H. Kelderman and A. Driessen, “Wavelength selective switch using thermally tunable microring resonators,” In F. Michelotti, A. Driessen, M. Bertolotti (Eds.), Proceedings 39 th Course of the International School of Quantum Electronics “Microresonators as building blocks for VLSI photonics,” pp. 413-414, Melville, New York, USA: American Institute of Physics, 2004. D. H. Geuzebroek, E.J. Klein, H. Kelderman and A. Driessen, “Compact wavelength selective switch,” In (Ed.) Proceedings of the 30 st European Conference on Optical Communications (ECOC), Stockholm, Sweden, 2004, pp. 580-581, ISBN 91- 975291-3-3. D. H. Geuzebroek, E. J. Klein, H. Kelderman and A. Driessen, “Wavelength tuning and switching of a thermo-optic micro ring resonator,” In J. Ctyroky, M. Hubalek, F. Ondrcek (Eds.), In (Ed.) Proceedings of the 11 th European Conference on Integrated Optics (ECIO) 2003, pp. 395-398, Prague, Czech Republic: Czech Technical University Prague, ISBN 80-01-02729-5. D. H. Geuzebroek, E. J. Klein, H. Kelderman, F. S. Tan, D. J. W. Klunder and A. Driessen, “Thermal tunable, Wide FSR switch based on Microring Resonators,” In (Ed.), T. D. Visser, D. Lenstra, H. F. Schouten (Eds.), Proceedings of IEEE/LEOS 2002, pp. 155-158, Amsterdam: IEEE/LEOS Benelux Chapter, c/o Vrije Universiteit van Amsterdam, ISBN 90-807519-1-x. D. H. Geuzebroek, E. J. Klein, H. Kelderman, F. S. Tan, D. J. W. Klunder and A. Driessen, “Thermal wavelength-selective switch based on micro-ring resonators,” In (Ed.), Proceedings of the 28 st European Conference on Optical Communications (ECOC), Copenhagen, Denmark, 2002. R. G. Heideman, D. H. Geuzebroek, A. Leinse, A. Melloni, F. Morichetti, C. G. H. Roeloffzen, A. Meijerink, L. Zhuang, E. van Etten, E. J. Klein and A. Driessen, “Low loss, high contrast optical waveguides based on CMOS compatible LPCVD processing,” Invited, In (Ed.), Proceedings of the 13 th European Conference on Integrated Optics (ECIO), Kopenhagen, Denmark, 2007. M. C. Larciprete, E. J. Klein, A. Belardini, D. H. Geuzebroek, A. Driessen and F. Michelotti, “Polarization conversion in vertically coupled Si3N4/SiO2 microring resonators,” In (Ed.), F. Michelotti, A. Driessen, M. Bertolotti (Eds.), Proceedings 39 th Course of the International School of Quantum Electronics “Microresonators as building blocks for VLSI photonics,” pp. 413-414, Melville, New York, USA: American Institute of Physics, 2004. R. Meijerink, D. H. Geuzebroek, E. J. Klein, H. Kelderman, R. Dekker, M. B. J. Diemeer and A. Driessen, “Optimization of driving signal fort hermal modulation of a microring resonator,” In R. M. de Ridder, G. Altena, D. H. Geuzebroek, R. Dekker (Eds.), In (Ed.) Proceedings 8th Annual Symposium IEEE/LEOS Benelux Chapter, pp 85-88, 2003, Enschede: IEEE LEOS Benelux, p/a Universiteit Twente, Integrated Optical Microsystems, ISBN 90-365-1990-X. P. J. Urban, E. G. C. Pluk, E. J. Klein, A. M. J. Koonen, G. D. Khoe and H de Waardt, “Simulation Results of Dynamically Reconfigurable Broadband Photonic Access 218
Networks (BB Photonics),” International Conference on Access Technologies, Cambridge, 2006. 219
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DENSELY INTEGRATED MICRORING- RESON
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DENSELY INTEGRATED MICRORING- RESON
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To my parents…
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esonators is limited by the spacing
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iv Samenvatting Dit proefschrift be
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schakelaar “aan” is, dan is de
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3.6.2 Overlap loss reduction.......
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Chapter 1 Introduction The devices
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1.2 Broadband to the home 3 Introdu
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1.3 Bringing Fiber to the Home 5 In
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Figure 1.5. The technological scope
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9 Introduction these basic paramete
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Chapter 2 2.1 Introduction Integrat
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Chapter 2 light Icav2 in the cavity
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Chapter 2 ∆ = ⎛ β r − β g
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Chapter 2 2.3.3 Combined model The
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Chapter 2 FC 4µ 1µ 2 ⋅ χr = 2
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Chapter 2 P Through /P In (dB) 0 -1
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Chapter 2 The figure shows that it
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Chapter 2 In − jϕr1 2 Figure 2.1
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Chapter 2 differences between the f
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Chapter 2 M = ⋅ FSR = N ⋅ FSR F
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Chapter 2 the heat will therefore f
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Chapter 2 index. Although this can
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Chapter 2 resonators for instance h
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Chapter 2 a rather complex MEMS bas
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Chapter 3 3.1 Introduction The most
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Chapter 3 3.2.1 Drop port on-resona
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Chapter 3 3.2.3 Filter bandwidth In
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Chapter 3 (resulting in a higher ba
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Chapter 3 Figure 3.11. Residual cha
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Chapter 3 3.3 Geometrical design ch
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Chapter 3 resonator and the port wa
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Chapter 3 Another important fact wh
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Chapter 3 The flowchart of the desi
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Chapter 3 While the resonator in th
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Chapter 3 3.6.1 Port waveguide and
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Chapter 3 overlap losses are only 0
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Chapter 3 3.7 Component design cons
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Chapter 3 By maximizing the power t
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Chapter 3 important, due to the fac
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Chapter 4 4.1 Introduction As was s
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Chapter 4 4.2.1 Transient response
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Chapter 4 Under the condition that
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Chapter 4 Figure 4.4. Screenshot of
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Chapter 4 The equations required to
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Chapter 4 using an approach based o
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Chapter 4 4.5.1 Architecture The Au
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Chapter 4 4.5.2 Simulation method A
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Chapter 4 Figure 4.9. A Primitive w
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Chapter 4 Listing 4.3. Pseudo code
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Chapter 4 Listing 4.4. Pseudo code
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Chapter 4 simulated output spectra
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Chapter 4 Figure 4.21. The reflecto
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Chapter 4 P Drop /P In (dB) 0 -10 -
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Chapter 4 Figure 4.27a. OADM with r
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Chapter 4 will propagate through th
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Chapter 4 As demonstrated by these
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Chapter 4 What is more interesting
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Chapter 4 method it does allow time
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Chapter 4 complex than the interact
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Chapter 5 5.1 Introduction The mate
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Chapter 5 wafer is used (step 1). T
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Chapter 5 range of 0.9 to 1.1 µm.
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Chapter 5 The process flow with the
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Chapter 5 5.3.3 Mask layout The big
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Chapter 5 5.4. Fabrication and mask
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Chapter 5 1. Definition of the vert
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Chapter 5 5.4.2 Fabrication The fab
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Chapter 5 Figure 5.21. Process flow
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Chapter 5 removed using lift-off of
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Chapter 6 6.1 Introduction About ha
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Chapter 6 In early, comparatively s
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Chapter 6 that the TEOS has a very
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Chapter 6 The most important aspect
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Chapter 6 6.2.3 Chromium heater des
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Chapter 6 Therefore, even if the si
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Chapter 6 Next, the heater was heat
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Chapter 6 6.3 Characterization of s
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Chapter 6 polarization maintaining
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Chapter 6 the resonators in this gr
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Chapter 6 Although the fitted coupl
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Chapter 6 a cladding thickness of 3
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Chapter 6 6.4 A wavelength selectiv
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Chapter 6 A possible explanation fo
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Chapter 7 Densely integrated device
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Densely integrated devices for WDM-
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Page 183 and 184: 7.2.2 Spectral measurements Densely
Page 185 and 186: Densely integrated devices for WDM-
Page 189 and 190: Power Densely integrated devices fo
Page 191 and 192: 7.3.4 Characterization Densely inte
Page 195 and 196: Figure 7.31a. Eye pattern of the re
Page 197: Densely integrated devices for WDM-
Page 200 and 201: Chapter 8 8.1 Introduction In most
Page 202 and 203: Chapter 8 amount of power will be d
Page 204 and 205: Chapter 8 Another problem that may
Page 206 and 207: Chapter 8 halves that are each comp
Page 209 and 210: Chapter 9 Discussion and Conclusion
Page 211 and 212: Appendix A. Mason’s rule Several
Page 213 and 214: Appendix B. Crosstalk Derivation Th
Page 215 and 216: List of Acronyms ADSL - Asymmetric
Page 217 and 218: List of Symbols Q - Quality Factor
Page 219 and 220: Bibliography [1] Dan Schiller, “E
Page 221 and 222: Regions,” IEEE Photonics Technolo
Page 223 and 224: [66] B. E. Little, S. T. Chu, J. V.
Page 225 and 226: [97] H. Haeiwa, T. Naganawa and Y.
Page 227 and 228: [135] A. Driessen, D. H. Geuzebroek
Page 229 and 230: [165] T. Barwicz, M. R. Watts, M. A
Page 231 and 232: Publication List Patents (pending)
Page 233: R. Dekker, L.T.H.Hilderink, M.B.J.
Page 237 and 238: Dankwoord/Acknowledgements Zo, dit
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Edwin Jan Klein - Universiteit Twente

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