Abstract

A coherently prepared Er3+-doped yttrium aluminum garnet (YAG) crystal with a four-level ionic configuration is exploited for realizing one-dimensional (1D) and two-dimensional (2D) electromagnetically induced gratings (EIGs). Owing to the probe gain induced by the incoherent pump, the diffraction efficiency of the crystal grating, especially the first-order diffraction, can be significantly improved via increasing the incoherent pumping rate or decreasing the probe detuning. The enhancement of the grating diffraction efficiency originates from the interference between the gain and phase gratings. It is also demonstrated that the diffraction of the crystal grating can be dynamically controlled via tuning the intensity and detuning of the standing-wave driving field or the concentration of Er3+ ion. More importantly, the probe energy of the diffraction side lobes around the central principle maximum is comparable to that of the first-order diffraction field for small driving intensity or large driving detuning. Our scheme may provide a possibility for the active all-optical control of optical switching, routing and storage in fiber communication wavelengths.

Highlights

  • A coherently prepared Er3+-doped yttrium aluminum garnet (YAG) crystal with a four-level ionic configuration is exploited for realizing one-dimensional (1D) and two-dimensional (2D) electromagnetically induced gratings (EIGs)

  • It should be worth pointing out that Er3+-doped YAG crystal, where some of the Y3+ ions are replaced by Er3+ ions, is an efficient active medium for solid-state lasers operating in the eye-safe wavelengths31, which have been applied to the fields of optical communication and biomedicine

  • We investigate the Fraunhofer diffraction characteristics of one-dimensional (1D) and two-dimensional (2D) diffraction gratings realized in an Er3+-doped YAG crystal with four-level ionic configuration

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Summary

Introduction

A coherently prepared Er3+-doped yttrium aluminum garnet (YAG) crystal with a four-level ionic configuration is exploited for realizing one-dimensional (1D) and two-dimensional (2D) electromagnetically induced gratings (EIGs). By increasing the incoherent pumping rate and decreasing the probe detuning, we can significantly enhance the interference between the gain and phase gratings, and thereby improving the diffraction efficiency of the crystal grating.

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