Table of Contents
Fetching ...

Propagation processing of short pulses in Rydberg exciton medium under blockade conditions

Sylwia Zielińska-Raczyńska, David Ziemkiewicz

Abstract

Propagation of short pulses through Cu$_2$O crystal containing Rydberg excitons is studied with the use of density matrix formalism and FDTD method. Saturation effects related to the so-called Rydberg blockade are studied extensively, exploring not only reduction of absorption (bleaching) but also power-dependent changes of the dispersive properties of the medium. The role of exciton lifetime and coherent population oscillations in the dynamics of the system is investigated. A pump-probe setup with two pulses is also studied, showing good agreement with recent experimental studies.

Propagation processing of short pulses in Rydberg exciton medium under blockade conditions

Abstract

Propagation of short pulses through CuO crystal containing Rydberg excitons is studied with the use of density matrix formalism and FDTD method. Saturation effects related to the so-called Rydberg blockade are studied extensively, exploring not only reduction of absorption (bleaching) but also power-dependent changes of the dispersive properties of the medium. The role of exciton lifetime and coherent population oscillations in the dynamics of the system is investigated. A pump-probe setup with two pulses is also studied, showing good agreement with recent experimental studies.
Paper Structure (12 sections, 19 equations, 13 figures)

This paper contains 12 sections, 19 equations, 13 figures.

Figures (13)

  • Figure 1: Energy level schematic of the considered system
  • Figure 2: Geometry of the considered system
  • Figure 3: a) absorption coefficient of Cu$_2$O crystal, exhibiting multiple excitonic peaks. Dashed line represents a Gaussian laser pulse. b) zoom on a single exciton resonance ($n$=3); numerically calculated frequency spectra of incident and transmitted field, as well as medium susceptibility are shown.
  • Figure 4: The transmission spectrum of the crystal in a frequency range of a single excitonic resonance, as a function of crystal thickness.
  • Figure 5: Spatio-temporal distribution of the field illustrating the propagation of a single pulse through $L=10$$\mu$m crystal (marked by white, dashed lines).
  • ...and 8 more figures