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作 者:万勇[1] 李长红[2] 云茂金[1] 郭月[1] 杨阳[1] 崔莹[1]
机构地区:[1]青岛大学物理科学学院,山东青岛266071 [2]青岛大学自动化工程学院,山东青岛266071
出 处:《光学学报》2013年第10期214-220,共7页Acta Optica Sinica
基 金:国家自然科学基金(11144007);山东省基金项目(BS2012CL012)
摘 要:采用渐变圆弓形散射元构建线性缺陷波导,并将其应用于光子晶体的慢光效应。在工作波长λ=1550nm时,通过圆弓形散射元单列纵向渐变,获得群折射率在31.4~95.0,低色散(△ng〈10%)带宽在3.7-11.8nm,无量纲标量积ng×(△λ)以在0.2268-0.2390,超低色散带宽(△ng〈1%)在2.2~4.8nm之间的慢光;通过三列圆弓形散射元纵向周期性渐变,获得群折射率在31.6~108.2,低色散(△ng〈10%)带宽在4.0~13.0nm,无量纲标量积ng×(△λ)/1在0.2650-0.2792,超低色散带宽(△ng〈1%)在2.6-6.8nm之间的慢光;通过圆弓形散射元横向渐变,获得群折射率在32.189.3,低色散带宽在2.9~9.3nm,无量纲标量积ng×(△λ)/λ在0.1670~0.1926,超低色散带宽在1.6~3.5nm之间的慢光。可见,采用散射元纵向渐变和横向渐变,特别是纵向渐变,可以实现慢光效应,从而为慢光结构设计和应用提供了新的方向。With operating wavelength λ= 1550 nm, two-dimensional graded eye-shaped scatterers are applied into photonic crystal waveguide (PCW) for slow light effect in three ways: 1) getting slow light with the group index ng from 31.4 to 95.0, the low-dispersion bandwidth (△ng〈10%) from 3.7 nm to 11.8 nm, the scalar product ng × (AA)/A from 0.2268 to 0. 2390, and the ultralow-dispersion bandwidth (△ng〈1%) from 2. 2 nm to 4. 8 nm by grading the single-row eye-shaped scatterers along the longitudinal direction; 2) getting slow light with the group index ng from 31.6 to 108.2, the low-dispersion bandwidth (△ng〈10%) from 4. 0 nm to 13. 0 nm, the scalar product ng×(△λ)/A from 0. 2650 to 0. 2792, and the ultralow-dispersion bandwidth (△ng〈1% ) from 2. 6 nm to 6.8 nm by grading the triple-row eye-shaped scatterers periodically along the longitudinal direction; 3) getting slow light with the group index ng from 32.1 to 89.3, the low-dispersion bandwidth from 2.9 nm to 9.3 nm, the scalar product ng× (△λ)/λ from 0. 1670 to 0. 1926, and the ultralow-dispersion bandwidth from 1.6 nm to 3.5 nm by grading the eye-shaped scatterers along the transverse direction. It means that graded structures, especially the graded eye-shaped scatterers along the longitudinal direction, can achieve slow light effect well and may provide a new way to design and apply slow light.
分 类 号:TN202[电子电信—物理电子学] TN203
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