2020
DOI: 10.3390/nano10101952
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Integrated Source of Path-Entangled Photon Pairs with Efficient Pump Self-Rejection

Abstract: We present a theoretical proposal for an integrated four-wave mixing source of narrow-band path-entangled photon pairs with efficient spatial pump self-rejection. The scheme is based on correlated loss in a system of waveguides in Kerr nonlinear media. We calculate that this setup gives the possibility for upwards of 100 dB pump rejection, without additional filtering. The effect is reached by driving the symmetric collective mode that is strongly attenuated by an engineered dissipation, while photon pairs are… Show more

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Cited by 4 publications
(4 citation statements)
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“…To demonstrate the way of experimental realization of reciprocity breaking purely by designed nonlinear loss, here we consider a recently suggested scheme with self-Kerr nonlinear waveguides that implements the dissipative coupling scheme depicted in Fig. 1(a) [24,25,45]. This scheme allows to produce two-photon loss or NCL of the kind given by Eq.…”
Section: Toward Practical Non-reciprocity With Nonlinear Dissipationmentioning
confidence: 99%
See 1 more Smart Citation
“…To demonstrate the way of experimental realization of reciprocity breaking purely by designed nonlinear loss, here we consider a recently suggested scheme with self-Kerr nonlinear waveguides that implements the dissipative coupling scheme depicted in Fig. 1(a) [24,25,45]. This scheme allows to produce two-photon loss or NCL of the kind given by Eq.…”
Section: Toward Practical Non-reciprocity With Nonlinear Dissipationmentioning
confidence: 99%
“…Figure 3(b) shows that reciprocity is broken for such a system also for a finite time even in the regime when the system's state is far from the stationary state. For the simulation, we have taken that the system is also subject to common single-photon loss, and that two-photon loss is present also in the second part of the device (which corresponds to the realistic threewaveguide scheme [25,45]). So, for the first part, we have taken γ 0 = γ 1 = γ , γ 2 = 0; for the second part, we have taken γ j = γ , ∀ j .…”
Section: Toward Practical Non-reciprocity With Nonlinear Dissipationmentioning
confidence: 99%
“…To demonstrate the way of experimental realization of reciprocity breaking purely by designed nonlinear loss, here we consider a recently suggested scheme with self-Kerr nonlinear waveguides that implements the dissipative coupling scheme depicted in Fig. 1(a) [24,25,45]. This scheme allows to produce two-photon loss or nonlinear coherent loss of the kind given by Eq.…”
Section: Toward Practical Non-reciprocity With Nonlinear Dissipationmentioning
confidence: 99%
“…3(b) shows that reciprocity is broken for such a system also for a finite time even in the regime when the systems' state is far from the stationary state. For the simulation we have taken that the system is also subject to the common single-photon loss, and that the two-photon loss is present also in the second part of the device (which corresponds to the realistic three-waveguide scheme [25,45]). So, for the first part we have taken γ 0 = γ 1 = γ, γ 2 = 0; for the second part we have taken γ j = γ, ∀j.…”
Section: Toward Practical Non-reciprocity With Nonlinear Dissipationmentioning
confidence: 99%