抄録
The transient time of an optical pulse in multi-layered photonic crystal is discussed as a function of the length L of the crystal and the wave vector of the incident light. In a periodic photonic crystal, the transient time τ for the wave vector close to photonic band gap is proportional to L 3 while τ for the wave vector at the center of photonic band is proportional to L. In a non-periodic Fibonacci lattice, τ becomes proportional to L 3.127 and L 1.1287 for the wave vector close to photonic band gap and at the center of photonic band, respectively. The power for L β in Fibonacci (periodic) photonic crystal can (not) be changed by refraction indices of consequent layers.
本文言語 | English |
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ホスト出版物のタイトル | Conference Program - MOC'11 |
ホスト出版物のサブタイトル | 17th Microoptics Conference |
出版ステータス | Published - 2011 12月 1 |
イベント | 17th Microoptics Conference, MOC'11 - Sendai, Japan 継続期間: 2011 10月 30 → 2011 11月 2 |
Other
Other | 17th Microoptics Conference, MOC'11 |
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国/地域 | Japan |
City | Sendai |
Period | 11/10/30 → 11/11/2 |
ASJC Scopus subject areas
- 電子材料、光学材料、および磁性材料
- 原子分子物理学および光学