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CHAPTER 5 ELECTRICALLY-DRIVEN INTEGRATED PHOTONIC

6.2 Suggestion for Future Work

An ideal optical buffer device in the optical communication network should possess the properties of low loss, zero dispersion, large delay time, and broad bandwidth for launched light waves. In this dissertation, photonic crystal waveguides were shown to

have great ability to slow down the light waves. Also, a small propagation loss of (2~3dB/mm) was reported. However, these are not good enough for the application to industry because of large dispersion and loss of the band-edge guided modes.

Therefore, for industrial purposes, how to manage pulse dispersion and diminish propagation loss should be the main issues.

Photonic crystal coupled waveguide is one of the solutions, as it makes possible for light waves to propagate at very slow speed and small velocity dispersion due to the unique S-shaped band structure. But the constant of formulated delay-bandwidth product leads to another trade-off problem: the larger the delay time, the smaller the bandwidth. As can be seen in Chapter 5, the observed inflection-point slow light modes correspond to a narrow bandwidth of only 2nm. This would limit the practicability in the development of photonic integrated circuits. One of the most suggested approaches is to employ the chirped refractive index on the photonic crystal waveguides [52, 61]. But this is merely theoretical proposal and may not be easy to carry out by the existing fabrication technology. So, more efforts still have to be made to achieve small group velocity and broad bandwidth for propagation waves in the photonic couple waveguides.

As for the electrically-driven integrated photonic crystal nanocavity lasers, quantum dots as an active medium should be recommended for the enhancement of the coupling probability between cavity modes and lasing modes because of its broadening emission spectrum. To achieve very high Q value (i.e. Q>10,000), the structure of the fabricated slab and the pattern of the nanocavities should be optimized.

The design rules can be referred to the published results on nanocavities, which have demonstrated Q value exceeding hundred thousands under optical pumping or coupling operation [18-19, 64]. Furthermore, the integrated nanocavites can be replaced by (or combined with) photonic crystal waveguides to become

multi-function photonic integrated circuits. These circuits would no longer need a passive waveguide and an external light source. Instead, the integrated electrical pumping edge-emitting laser diode directly provides essential optical waves. Once the laser is driven by injection current, each component of the photonic circuit would start to work accordingly. This image would be very similar to an electronic chip, and can be named “photonic chips”. To realize this, experiments on the integrated W1 type photonic crystal waveguides should be expected.

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Vita

Name:Shih-Chieh Huang (黃世傑) Date of birth:June 27, 1978

Place of birth: Changhua, Taiwan, R.O.C.

Sex: Male Education:

National Chiao Tung University Ph. D. September, 2002 — June, 2007 Institute of Electronics Engineering

National Chiao Tung University M. S. September, 2000 — June, 2002 Institute of Electronics Engineering

National Chiao Tung University B. S. September, 1996 — June, 2000 Department of Electronics Engineering

Internship:

Nippon Telegraph and Telephone Corporation

Basic Research Laboratories February, 2005 — September, 2006 (Group Leader: Dr. Masaya Notomi)

Title of Ph. D. Dissertation:

Study on Slow Light in Photonic Crystal Waveguides and Integrated Photonic Crystal Nanocavity Coupled Surface Emitting Lasers

Publication List

[1] S. C. Huang, T. H. Yang, C. P. Lee, and S. D. Lin, “Electrically driven integrated photonic crystal nanocavity coupled surface emitter laser,” Appl. Phys. Lett. 90, 151121 (2007).

[2] S. C. Huang, M. Kato, E. Kuramochi, C. P. Lee, and M. Notomi, “Time-domain and spectral-domain investigation of inflection-point slow light modes in photonic crystal coupled waveguides,” Opt. Express 15, 3543 (2007).

[3] S. C. Huang, T. H, Yang, C. P. Lee, and S. D. Lin, “Single mode operation of integrated photonic crystal nanocavity coupled surface emitting lasers,” JMB6, CLEO/QELS’07, Baltimore, U. S. A. (2007).

[4] S. C. Huang, M. Kato, E. Kuramochi, C. P. Lee, and M. Notomi, “Experimental observation of inflection-point slow light modes in photonic crystal coupled waveguides,” CMV6, CLEO/QELS’07, Baltimore, U. S. A. (2007).

[5] Y. H. Zhang, T. Tawara, N. Cade, D. Ding, T. Tanabe, E. Kuramochi, S. R.

Johnson, S. C. Huang, and M. Notomi, “GaAs based InAs Quantum Dot Photonic Crystal Lasers,” SPIE Photonics West, San Jose CA , U. S. A.(2007).

[6] M. Kato, S. C. Huang, E. Kuramochi, and M. Notomi, “Time-domain measurement of slow light in photonic crystal coupled waveguide,” JSAP Spring Meeting, Japan (2007).

[7] K. W. Sun, S. C. Huang, A. Kechiantz, and C. P. Lee, “Subwavelength gratings fabricated on semiconductor substrates via E-beam lithography and lift-off method,”

Optical and Quantum Electronics 37, 425 (2005).

[8] S. C. Huang, E. Kuramochi, T. Watanabe, C. P. Lee, and M. Notomi, “Group delay analysis of low-loss Si photonic crystal waveguides,” JSAP Autumn Meeting, Japan (2005).

[9] H. M. Lee, E. Y. Chang, S. Chen, and S. C. Huang, “50-nm-T-gate fabricated by thermally reflowed resist technique”, SPIE Microlithography, Santa Clara, California U. S. A. (2003).

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