Abstract

We utilized the all-copropagating scheme, which maintains the phase-match condition, in the spontaneous four-wave mixing (SFWM) process to generate biphotons from a hot atomic vapor. The linewidth and spectral brightness of our biphotons surpass those of the biphotons produced with the hot-atom SFWM in the previous works. Moreover, the generation rate of the sub-MHz biphoton source in this work can also compete with those of the sub-MHz biphoton sources of the cold-atom SFWM or cavity-assisted spontaneous parametric down conversion. Here, the biphoton linewidth is tunable for an order of magnitude. As we tuned the linewidth to 610 kHz, the generation rate per linewidth is 1,500 pairs/(s·MHz) and the maximum two-photon correlation function, gs,as(2), of the biphotons is 42. This gs,as(2) violates the Cauchy-Schwarz inequality for classical light by 440 folds, and demonstrates that the biphotons have a high purity. By increasing the pump power by 16 folds, we further enhanced the generation rate per linewidth to 2.3×104 pairs/(s·MHz), while the maximum gs,as(2) became 6.7. In addition, we are able to tune the linewidth down to 290±20 kHz. This is the narrowest linewidth to date among all single-mode biphoton sources of room-temperature and hot media.

Highlights

  • Photons are superior carriers of information and can keep the carried information intact during the transmission, as they never collide with each other and hardly interact with the environment

  • The measured electromagnetically induced transparency (EIT) spectrum can reveal the experimental condition of optical depth, coupling Rabi frequency (Ωc), and decoherence rate (γ) for the theoretical calculation to predict the biphoton wave packet

  • We measured the spectra with an input probe field under the presence of the coupling, hyperfine optical pumping (HOP), and pump fields

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Summary

Introduction

Photons are superior carriers of information and can keep the carried information intact during the transmission, as they never collide with each other and hardly interact with the environment. Since the decoherence rate (or coherence time) is typically low (or long) in the cold-atom system, one can utilize cold atoms in the SFWM process to produce narrow-linewidth biphotons [10, 40,41,42,43,44,45,46,47,48,49,50,51]. The SFWM has two types of transition schemes: a double-Λ and a ladder schemes. The former is able to produce biphotons with a linewidth of less than 1 MHz [45, 46, 48]. We only focus on the SFWM of the double-Λ transition scheme in this study

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