The Study of Quantum Interference in Metallic Photonic Crystals Doped with Four-Level Quantum Dots
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- Hatef, A. & Singh, M. Nanoscale Res Lett (2010) 5: 464. doi:10.1007/s11671-009-9517-1
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In this work, the absorption coefficient of a metallic photonic crystal doped with nanoparticles has been obtained using numerical simulation techniques. The effects of quantum interference and the concentration of doped particles on the absorption coefficient of the system have been investigated. The nanoparticles have been considered as semiconductor quantum dots which behave as a four-level quantum system and are driven by a single coherent laser field. The results show that changing the position of the photonic band gap about the resonant energy of the two lower levels directly affects the decay rate, and the system can be switched between transparent and opaque states if the probe laser field is tuned to the resonance frequency. These results provide an application for metallic nanostructures in the fabrication of new optical switches and photonic devices.
KeywordsMetallic photonic crystal Quantum dot Dipole–dipole interaction Quantum interference Quantum optics
In the past few decades, there has been a growing interest in the development of artificial nano-materials. One class of material such as this is photonic crystals (PCs), which are periodic dielectric or semiconductor structures that display a photonic band gap (PBG) in their electromagnetic wave transmission characteristics [1, 2, 3, 4]. The existence of the PBG has inspired the design of various nano-optical and opto-electronic devices . Since the formation of the PBG is due to the multiple Bragg reflections within a PC, ordinary PCs are a combination of lossless materials for which the stop band has a small width, almost less than 25% of the central frequency. This is due to the fact that a significant percentage of incident radiation passes through the periodic structure cores so that the reflected radiation is weaker than the transmitted radiation. Because of this, Bragg scattering comes into play when there are periodicities along the direction of propagation. To exhibit a noticeable PBG with fewer periodicities it is much better to use impenetrable materials. Metals would be one of the best options since they are more reflective than dielectric or semiconductor materials over a broad range of frequencies, due to their imaginary dielectric component that exists in even the optical and near infrared regions, where metals are dispersive and absorptive in these frequency regions [6, 7, 8]. Recently, considerable progress has been made in constructing these periodic arrangements which are called metallic or metallodielectric photonic crystals (MPC/MDPC) in one-, two-, and three-dimensional systems. For instance, one-dimensional (1D) MDPCs with metal thicknesses on the order of hundreds of nanometres has been proved transparent to visible light while blocking ultraviolet and infrared [9, 10]. This characteristic can be used for example in laser safety glasses, UV protective films and flat panel displays. Two-dimensional (2D) MPC structures are usually made of metallic rods or nanodisks that are periodically arranged on a waveguide layer. Waveguided MPCs have exhibited unique optical properties because of the strong coupling that exists between the particle plasmon resonance and waveguide mode. Such structures have a number of potential applications in biosensors  and all-optical switching , among others. In the case of three-dimensional (3D) structures, there are also several applications such as high-efficiency light sources  and thermal photovoltaic power generation .
Besides these advantages, PCs can be used for radiation suppression and emission enhancement below the electronic band gap and near a photonic band edge, respectively, where a PC functions as a reservoir for an exited light emitter or active medium such as an atom, a molecule or a quantum dot (QD). According to Fermi’s ‘Golden Rule’, the decay rate is proportional to the local density of states (LDOS) that counts the number of electromagnetic modes available to the photons for emission into the environment. Thus, any modification in the LDOS would lead to manipulation of the decay rate. Recently, the inhibition, enhancement and quantum interference (QI) effects of spontaneous emission (SE) from the QDs doped in 3D–PCs have been widely studied, both experimentally and theoretically [15, 16, 17, 18, 19]. Controlling spontaneous emission by using quantum optics would lead to several interesting effects, such as optical gain enhancement  and photoluminescence enhancement , optical switching [22, 23], quantum information processing [24, 25] and electromagnetically induced transparency . QI in a three- or multi-level atomic system can arise from the superposition of SEs when electron transitions take place between the upper and lower levels. Under certain circumstances the initially excited atomic system may not decay to its ground level due to a cancellation of SE by QI between atomic transition levels. Due to this, dark states with zero absorption amplitude would appear causing the multi-level atomic system to act like a transparent medium, which has potential applications for optical switches and photonic devices [27, 28]. In this paper, the effects of electronic QI on the absorption coefficient of QDs have been investigated for small and large concentration of the dopants (QDs). We consider that the QDs are four–energy level systems where the two upper levels are very close, coupled to a lower one via the same and single field continuum and damped by the MPC interaction.
Metallic Photonic Crystals
Recently, theoretical and experimental studies have shown that it is possible to make 3D MPCs that contain nano-sized metallic spheres which are transparent to visible and near infrared light [7, 29, 30]. In this paper, we have used an ideal 3D isotropic MPC model made from metallic spheres of radius a with a frequency dependent refractive index n1(ω), which are arranged periodically in a background dielectric material with a constant refractive index (n2). The dispersion relation and photonic band structure of this idealized theoretical 3D model was developed by S. John in the following references [31, 32]. Although many simplifying approximations have been used in this model, it is sufficient for our purpose as it leads to qualitatively correct physics and exhibits many of the observed and computed characteristics of 3D MPC which opens a band gap in the rage of visible frequencies [7, 29, 30].
Active Medium Embedded in a MPC
System Hamiltonian and Density Matrix Equations
Here, N is the concentration of quantum dots and ε is the energy of the incident laser beam.
In order to study the linear response of the system, we have calculated the normalized absorption coefficient given in Eq. (11) (α/α0) by using a very low driving field (Ω = 0.01). We consider that the metallic spheres are made of silver with εp = 9 eV. The two upper resonant energies (εab = 2.78 eV and εac= 2.783 eV) are considered to be far away from the upper edge band gap in the first Brillouin zone where Γb ≈ Γc= 1.57γ0. The value of Γa can be set by changing the resonant energy εad. This decay rate (Γa) can be totally suppressed if the resonant energy lies within the band gap.
In conclusion, we have studied the effect the quantum interference and DDI on the absorption of a MPC doped with an ensemble of four-level QDs, for both cases where DDI was neglected or accounted for, while the system approached a steady state. A single driving laser field which induces a dipole moment in each QD was applied to measure the absorption. The density matrix method and linear-response theory have been used to calculate the absorption.
It is found that when the resonance energy of the lower levels is within the band gap, the system is in an absorbing state. However, when the resonance energy of the lower levels is outside the band gap, the system is in a nonabsorption state. Thus, the system can be switched between the absorption and nonabsorption states. We anticipate that the results described here will be useful for developing new types of optical switching devices.
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