Abstract

The control of Fano resonances is of critical importance to opto-electronic and all-optical switching devices, light delay and storage, high sensitivity sensors, and quantum information processors. In this paper, we experimentally and theoretically demonstrate that controllable electromagnetically induced transparency (EIT)-like and Fano resonances can be achieved in a single quasi-cylindrical microresonator (QCMR). Robust and selective excitation of localized axial modes in a high quality QCMR is firstly demonstrated. Based on this stable platform, EIT-like lineshapes can be tuned and converted into Fano resonances by vertically moving the resonator. Moreover, by horizontally scanning the resonator, the transmission spectrum exhibits periodically changed Fano-like lineshapes. It is reported for the first time that the above two kinds of Fano resonances originated from different mechanisms can work on the same mode simultaneously. Our approach, demonstrated in this work, provides a robust photonic platform for accessing, controlling, and engineering the Fano resonances.

Highlights

  • Sometimes manifesting as electromagnetically induced transparency (EIT), comes from quantum interference of a discrete excited state of an atom and a continuum, which was firstly discovered by Ugo Fano [1]

  • Fano resonances have been demonstrated in coupled whispering gallery mode (WGM) microcavities [6,7,8], a multimode tapered fiber coupled a microsphere [9], or in a single WGMR [10,11,12,13,14]

  • We study dynamic controlled Fano resonances in a quasicylindrical microresonator (QCMR)

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Summary

Introduction

Sometimes manifesting as electromagnetically induced transparency (EIT), comes from quantum interference of a discrete excited state of an atom and a continuum, which was firstly discovered by Ugo Fano [1]. A small perturbation in the system results in very large change in magnitude and phase This property holds great potential in fruitful applications, including but not limited to opto-electronic devices, high-sensitivity sensors [2], optical storage [3,4], slow light [5], narrowband filtering, and nonlinearity enhancement. This originates from destructive interference between a high Q and a low Q mode. By horizontally moving the QCMR, another kind of periodically changed Fano resonances are exhibited and engineered, which can be attributed to multimode coupling and modal dispersion in the fiber.

Coupling platform construction and mode selective excitation
Stable controlled Fano resonances in a QCMR platform
Theoretical model
Experimental results and discussion
Conclusion
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