Channel Drop Tunneling through Localized States
Channel Drop Tunneling through Localized States
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DOI:
10.1103/physrevlett.80.960
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发表时间:
1998-02
影响因子:
8.6
通讯作者:
S. Fan;P. R. Villeneuve;J. Joannopoulos;H. Haus
中科院分区:
文献类型:
--
作者:
S. Fan;P. R. Villeneuve;J. Joannopoulos;H. Haus
We present a general analysis of the tunneling process through localized resonant states between onedimensional continuums. We show that complete transfer can occur between the continuums by creating resonant states of different symmetry, and by forcing an accidental degeneracy between them. The degeneracy must exist in both the real and imaginary parts of the frequency. We illustrate the results of the analysis by performing computational simulations on the transport properties of electromagnetic waves in a two-dimensional photonic crystal. [S0031-9007(97)05091-6] Resonant tunneling processes can occur between states when they interact through a coupling element which supports localized resonances. Of particular interest is the complete channel drop tunneling between one-dimensional continuums, i.e., the selective transfer of a single propagating state (i.e., monoenergy electron, or single-frequency photon) from one continuum to the other, leaving all other states unaffected. Examples include the transfer of states between electron waveguides [1,2] through a quantum dot device, and the transfer of photonic states between dielectric waveguides through an optical resonator system. Such transfer processes are important for single-energy electron spectroscopy or wavelength demultiplexing in optical communication systems [3,4]. However, to our knowledge, the general conditions needed to realize optimal transfer until now have not been recognized. In this Letter, we determine the general characteristics of the coupling element required to achieve complete channel drop tunneling. We begin by presenting a qualitative analysis using symmetry and energy conservation arguments which identifies the important ingredients needed in constructing an analytical theory. Using a rigorous mathematical formalism, we then demonstrate that complete transfer can occur by creating resonant states of different symmetry, and by forcing an accidental degeneracy of both the real and imaginary parts of the frequency between the resonant states. We illustrate the results of the analysis by simulating the transport properties of electromagnetic waves in a two-dimensional photonic crystal.