Abstract

The production of correlated Stokes (S) and anti-Stokes (aS) photons (SaS process) mediated by real or virtual phonon exchange has been reported in many transparent materials. In this work, we investigate the polarization and time correlations of SaS photon pairs produced in a diamond sample. We demonstrate that both S and aS photons have mainly the same polarization of the excitation laser. We also perform a pump-and-probe experiment to measure the decay rate of the SaS pair production, evidencing the fundamental diference between the real and virtual (phonon exchange) processes. In real processes, the rate of SaS pair production is governed by the phonon lifetime of $(2.8 \pm 0.3)$ ps, while virtual processes only take place within the time width of the pump laser pulses of approximately 0.2 ps. We explain the diference between real and virtual SaS processes by a phenomenological model, based on probabilities of phonon creation and decay.

Highlights

  • In correlated Raman scattering, the same phonon participates in both Stokes (S) and anti-Stokes frequency conversions, characterizing the SaS process [1,2]

  • The photon pair produced by a virtual process is analogous to the electronic Cooper pair in superconductivity [15], and this analogy has been explored in diamond samples [16,17]

  • We study the production rate of photonic Cooper pairs as a function of the time delay between the S and aS scattering in the SaS process to elucidate this fundamental difference between the real and virtual phonon exchange processes

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Summary

INTRODUCTION

In correlated Raman scattering, the same phonon participates in both Stokes (S) and anti-Stokes (aS) frequency conversions, characterizing the SaS process [1,2]. We study the production rate of photonic Cooper pairs as a function of the time delay between the S and aS scattering in the SaS process to elucidate this fundamental difference between the real and virtual phonon exchange processes. As it will be discussed, photon polarization has to be studied to enable performing the lifetime measurements

TECHNICAL DETAILS
Polarization
Lifetime
CONCLUSION
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