Laboratoire de Dynamic et Optique des Matériaux, Département de Physique, Faculté des Sciences, Université Mohamed Premier, 60000 Oujda, Morocco.
J Phys Condens Matter. 2014 Dec 17;26(50):505901. doi: 10.1088/0953-8984/26/50/505901. Epub 2014 Nov 19.
We give an analytical and experimental demonstration of a classical analogue of the electromagnetic induced absorption (EIA) in a simple photonic device consisting of two stubs of lengths d1 and d2 grafted at the same site along a waveguide. By detuning the lengths of the two stubs (i.e. δ = d(2) - d(1)) we show that: (i) the amplitudes of the electromagnetic waves in the two stubs can be written following the two resonators model where each stub plays the role of a radiative resonator with low Q factor. The destructive interference between the waves in the two stubs may give rise to a sharp resonance peak with high Q factor in the transmission as well as in the absorption. (ii) The transmission coefficient around the resonance induced by the stubs can be written following a Fano-like form. In particular, we give an explicit expression of the position, width and Fano parameter of the resonances as a function of δ. (iii) By taking into account the loss in the waveguides, we show that at the transmission resonance, the transmission (reflection) increases (decreases) as a function of δ. Whereas the absorption goes through a maximum around 0.5 for a threshold value δth which depends on the attenuation in the system and then falls to zero. (iv) We give a comparison between the phase of the determinant of the scattering matrix, the so-called Friedel phase and the phase of the transmission amplitude. (v) The effect of the boundary conditions at the end of the resonators on the EIA resonance is also discussed. The analytical results are obtained by means of the Green's function method, whereas the experiments are carried out using coaxial cables in the radio-frequency regime. These results should have important consequences for designing integrated devices such as narrow-frequency optical or microwave filters and high-speed switches.
我们在一个由两个长度为 d1 和 d2 的短截线在同一位置沿波导接枝而成的简单光子器件中,对经典电磁感应吸收(EIA)的模拟进行了分析和实验演示。通过调谐两个短截线的长度(即 δ=d2-d1),我们表明:(i)两个短截线中的电磁波振幅可以按照两个谐振器模型来写,其中每个短截线扮演辐射谐振器的角色,具有低 Q 因子。两个短截线中的波的相消干涉可能导致在传输和吸收中具有高 Q 因子的尖锐共振峰。(ii)由短截线引起的共振的透射系数可以按照类似于 Fano 的形式来写。特别是,我们给出了共振的位置、宽度和 Fano 参数作为 δ 的函数的显式表达式。(iii)考虑到波导中的损耗,我们表明在传输共振处,透射(反射)随着 δ 的变化而增加(减少)。而吸收则在阈值 δth 左右随 δ 的变化出现最大值,该阈值取决于系统的衰减,然后降至零。(iv)我们比较了散射矩阵行列式的相位,即所谓的 Friedel 相位,与透射幅度的相位。(v)还讨论了谐振器末端边界条件对 EIA 共振的影响。通过格林函数方法获得了分析结果,而实验则在射频范围内使用同轴线进行。这些结果对于设计集成器件,如窄频带光学或微波滤波器和高速开关,具有重要意义。