Strong Multi-partite Entanglement for Quantum Networks Is Unlocked by Extreme Nanophotonic Cavities

Multi-partite Entanglement for Quantum Networks

In order to attain previously unheard-of levels of light-matter interactions, a new design for nanobeam photonic crystal cavities has been presented. It combines sub-wavelength field confinement with extreme quality factors (∼107). Because these devices are designed to function at 780 nm, they are perfect for generating entanglement and coupling with ultracold 87Rb atoms, which are essential parts of quantum networks because of their hyperfine structure.

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Performance and Technology

The study focuses on nanobeam cavities made of silicon nitride, or Si3​N4​, a material selected for its minimal material losses and comparatively high refractive index. The majority of optical cavities are frequently restricted to the edge of the strong coupling regime due to the extreme difficulty of both achieving low losses (high quality factor, Q) and a tiny mode volume (V, which represents sub-wavelength field confinement.

With a diffraction-limited mode volume and an ultra-high quality factor of Q=1.3×107, the first design, D1, immediately achieves strong coupling. Two new designs (D2 and D3) were created using bow-tie tips at a high-index dielectric-air interface in order to force the systems deeper into the strong coupling domain for faster interactions. These tips achieve extreme sub-wavelength localization at optical frequencies by using evanescent fields.

Schematic of nanobeam photonic crystal cavity designs. (a) Si3N4 nanobeam with lattice constant a = 262 nm, height h = 300 nm, spatially tapered width b(x), and air hole radius R = 53 nm. The dielectric tips are parameterized by their size θ = 30°, tip–tip spacing δ = 20 nm, and rescaled hole radius rtip = 59.6 nm. (b) Field enhancement Ey/W in units of 
 along a line passing through the center of the air hole in designs D1 and D2 along the x axis, where W is the total energy of the mode. (c) Photonic mode profiles of all designs D1 → D3 operating at λ = 780. D1 contains no tips, while D2 and D3 contain one and two tips, respectively. (d) Profile of the resonant modes electric field (not to scale) for D1 with tapered region NT and mirror region NM showing confinement in the center.
Image credit to APL Quantum

These improved designs reduce the mode volume to sub-wavelength levels, namely V=0.66(λ/n)3, while maintaining ultra-high quality factors (Q=1.2×107 for D2 and 1.1×107 for D3). They operate deep within the strong coupling domain for visible wavelengths with this special combination, which results in unprecedented and high cooperativity values, reaching $C=1.3×106 for D2 and C=1.2×106 for D3, respectively. In contrast, coherent oscillations are maintained for a long lifespan of about 10 ns because the coupling strength g in D1 (9 GHz) is roughly three orders of magnitude more than the cavity loss κ (29 MHz).

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Sturdy Entanglement Creation

The realization of robust local multi-partite entanglement between two 87Rb atoms optically trapped within the device’s central unit cell is demonstrated using the nanobeam cavities. A strong quadratic trap is created by linearly combining blue-detuned modes to trap atoms.

When both atoms have the same coupling strength to the photonic mode, the entanglement between them is at its highest. It is demonstrated that the design is extremely resistant to atomic displacements that may otherwise result in changes in coupling strength.

  • The coupling strength fluctuation in nanobeam cavity D1 is negligible because of displacement, resulting in incredibly stable entanglement that only drops by roughly 0.2%, even in the most extreme scenario where one atom is moved to the dielectric interface.
  • Why The durable optical trap limits the atom inside a restricted region, limiting the decrease in entanglement to no more than 2.7%, even though design D3 has a more localised field at the dielectric tips, resulting in a greater potential fluctuation in coupling strength along the unit cell.

The scalability of the architecture and the robust, consistent, and coherent entanglement produced in these devices make them a perfect platform for creating quantum networks for distributed quantum computing and upcoming light-based quantum technologies. Quantum networks use quantum channels to disperse entanglement (flying qubits like photons) and local nodes (stationary qubits like cold atoms) to manipulate and store information. The crucial link between these flying and stationary qubits is strengthened by these nanobeam cavities.

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Analogously, consider these nanophotonic cavities as ultra-long storage tanks (the high quality factor, Q) coupled with ultra-efficient funnels (the small mode volume, V). The light and the atoms are forced to interact strongly and for an extended period of time by making the funnel incredibly narrow and making sure the storage tank doesn’t leak. This allows them to continuously exchange energy and maintain a highly tangled quantum state, even if the atoms wobble slightly inside the funnel.

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