Single-photon nonlinearities and blockade from a strongly driven photonic molecule

Davide Nigro; Marco Clementi; Marco Clementi; Camille-Sophie Brés; Marco Liscidini; Dario Gerace

doi:10.1364/OL.468546

Optics Letters
Vol. 47,
Issue 20,
pp. 5348-5351
(2022)
•https://doi.org/10.1364/OL.468546

Single-photon nonlinearities and blockade from a strongly driven photonic molecule

Davide Nigro, Marco Clementi, Camille-Sophie Brés, Marco Liscidini, and Dario Gerace

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Davide Nigro, Marco Clementi, Camille-Sophie Brés, Marco Liscidini, and Dario Gerace, "Single-photon nonlinearities and blockade from a strongly driven photonic molecule," Opt. Lett. 47, 5348-5351 (2022)

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Table of Contents Category
- Nonlinear Optics
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About this Article
History
- Original Manuscript: June 24, 2022
- Revised Manuscript: September 16, 2022
- Manuscript Accepted: September 21, 2022
- Published: October 11, 2022

Abstract

Achieving the regime of single-photon nonlinearities in photonic devices by just exploiting the intrinsic high-order susceptibilities of conventional materials would open the door to practical semiconductor-based quantum photonic technologies. Here we show that this regime can be achieved in a triply resonant integrated photonic device made of two coupled ring resonators, in a material platform displaying an intrinsic third-order nonlinearity. By strongly driving one of the three resonances of the system, a weak coherent probe at one of the others results in a strongly suppressed two-photon probability at the output, evidenced by an antibunched second-order correlation function at zero-time delay under continuous wave driving.

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Supplementary Material (1)

Name	Description
Supplement 1	Zip archive containing the supplemental file .tex and figures

Data availability

Data underlying the results presented in this paper are not publicly available at this time but may be obtained from the authors upon reasonable request.

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Material	$n$	$n_{2}$	$Q_{0}$	$R$	$γ_{n l}$	${\tilde{g}}_{n l} / Γ_{s}$
		$(m^{2} W^{- 1})$	$\times 10^{6}$	$(m)$	$(m^{- 1} W^{- 1})$	$P_{p} = 0.1 W$	$P_{p} = 1 W$	$P_{p} = 10 W$
$L i N b O_{3}$ [18]	$2.24$	$1.8 \times 10^{- 19}$	$4.4$	$80 \times 10^{- 6}$	$0.7$	$5.7 \times 10^{- 4}$	$1.8 \times 10^{- 3}$	$5.7 \times 10^{- 3}$
$S R N$ [20]	$3.1$	$2.8 \times 10^{- 17}$	$0.06$	$100 \times 10^{- 6}$	$550$	$7.3 \times 10^{- 4}$	$2.3 \times 10^{- 3}$	$7.3 \times 10^{- 3}$
$S i C$ [22]	$2.6$	$6.9 \times 10^{- 19}$	$1.1$	$50 \times 10^{- 6}$	$3.2$	$3.8 \times 10^{- 4}$	$1.2 \times 10^{- 3}$	$3.8 \times 10^{- 3}$
$G a P$ [23]	$3.3$	$1.1 \times 10^{- 17}$	$0.25$	$50 \times 10^{- 6}$	$250$	$4.1 \times 10^{- 3}$	$1.3 \times 10^{- 2}$	$4.1 \times 10^{- 2}$
$S i_{3} N_{4}$ [19]	$2.0$	$2.5 \times 10^{- 19}$	$37$	$115 \times 10^{- 6}$	$0.7$	$1.2 \times 10^{- 2}$	$3.9 \times 10^{- 2}$	$0.12$
$A l G a A s$ [24]	$3.3$	$2.6 \times 10^{- 17}$	$3.14$	$28 \times 10^{- 6}$	$390$	$0.23$	$0.73$	$2.3$

Abstract

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Optics Letters