Fig. 3: Analysis of spin-mechanical coupling profiles and the defect cell parameters that affect this coupling.
From: Spin-optomechanical cavity interfaces by deep subwavelength phonon-photon confinement

(a) and (b) shows the 2D and 1D spin-mechanical coupling gsm profile of the spin-optomechanical crystal breathing mode, with expected position of the Group IV spin overlayed. The parameters b, ad, \({h}_{{x}_{d}}\), and \({h}_{{y}_{d}}\) impact the spin-mechanical coupling strength among other variables. The one-dimensional profile in the center of the bridge shows that strain is maximized at the bridge edge but retained in the center away from sidewalls. The crystal axis orientation in the device affects gsm (c) and gom (d, red) by changing the strain elements the spin sees and the photoelastic effect for gpe (d, yellow), which sums with a constant gmb (d, gray). e Sweeping b, ad, \({h}_{{x}_{d}}\), and \({h}_{{y}_{d}}\) about a naive parameter set shows that the parameters governing device performance, namely var ∈ {Qopt, gom, gsm}, are maximized about different variables, motivating protocol-based numerical optimization of the exact design parameters. Qmech was routinely near 106 or greater in the sweeps and not depicted. These sweeps are centered around the following parameters \(\{{h}_{{y}_{d}},{h}_{{x}_{d}},{a}_{d}\}=\{220.5,341.25,456.75\}\) nm, α = 135°; the rest of the parameters are the same as in Table 1.