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首页> 外文期刊>Optics and Spectroscopy >Fluorescence of a two-level atom in a two-dimensional photonic crystal in the vicinity of the saddle point of the photonic band spectrum
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Fluorescence of a two-level atom in a two-dimensional photonic crystal in the vicinity of the saddle point of the photonic band spectrum

机译:二维光子晶体中光子带谱鞍点附近的二级原子的荧光

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摘要

The fluorescence of a two-level atom embedded into a two-dimensional photonic crystal is considered under the assumption that the electronic transition frequency ω(10) is close to the photonic mode frequency ω(0) in the saddle critical point of the photonic spectrum. In this case, the density of photonic states has a logarithmic peak, which manifests itself in a considerable rearrangement of the fluorescence spectrum. The Green's function of the electron-photon system, which contains the description of the dynamics of spectroscopic transitions and the shape of fluorescence spectra, is obtained in the rotating field approximation. Using the Green's function, the frequency-dependent Lamb shift and the broadening of the atomic transition are calculated. The shape of the fluorescence spectra is studied. At a large oscillator strength of the atomic transition, the fluorescence line splits into two components in the vicinity of the singularity caused by the saddle critical point. This splitting is associated with a specific Fano-type resonance between the discrete spectrum (the atomic states) and the continuum (the dispersion of photons with a saddle critical point). At small detunings δ = ω(10)-ω(0), the components of the fluorescence line have considerably different intensities. As δ increases, the spectral positions of the strong and weak components tend to the frequencies of the atomic transition and the saddle point, respectively. The results obtained show that two-level atoms (or quantum dots) can be used as specific probes of the band spectra of photonic crystals. (C) 2005 Pleiades Publishing, Inc.
机译:在电子跃迁频率ω(10)在光子谱的鞍形临界点接近于光子模频率ω(0)的假设下,考虑了嵌入二维光子晶体中的二级原子的荧光。在这种情况下,光子态的密度具有对数峰,这在荧光光谱的显着重排中表现出来。电子-光子系统的格林函数,包含对光谱跃迁动力学和荧光光谱形状的描述,可以通过旋转场近似获得。使用格林函数,可以计算出随频率变化的兰姆位移和原子跃迁的展宽。研究了荧光光谱的形状。在原子跃迁的大振荡器强度下,荧光线在由鞍形临界点引起的奇点附近分裂为两个分量。这种分裂与离散光谱(原子态)和连续体(具有鞍形临界点的光子的色散)之间特定的Fano型共振有关。在小的失谐点δ=ω(10)-ω(0)时,荧光线的成分具有明显不同的强度。随着δ的增加,强和弱组分的光谱位置分别趋向于原子跃迁和鞍点的频率。获得的结果表明,两能级原子(或量子点)可以用作光子晶体带谱的特定探针。 (C)2005年Pleiades Publishing,Inc.

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