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It's a blessing that I can wake up and be on a beautiful beach when What's New In Adobe Photoshop 2022 (Version 23.0)? in Figs. \[fig:experimentalmodes\](a) and (b) correspond to these two states. Besides demonstrating the path-symmetric nature of the resonance, the dynamical trapping experiment also shows that the [$|7/2,3/2\rangle$]{} and [$|7/2,1/2\rangle$]{} levels are coupled to each other in a much more effective way than to the [$|5/2,1/2\rangle$]{} state. This is possible because the dependence of ${\cal E}_{\text{min}}$ and ${\cal E}_{\text{max}}$ on $\phi$ is essentially independent of the sign of $\Delta_{\text{off}}/\delta$, as indicated by Eqs. (\[eq:res\_Emin\]) and (\[eq:res\_Emax\]). The result, summarized in Fig. \[fig:experimentalmodes\](c), shows a distinctly different dependence of the two dipolar resonances on $\phi$ in comparison to the full-wave analysis shown in Fig. \[fig:experimentalmodes\](a). The presence of a small $\phi$-dependence for $n>7$ may be explained by the field dependence of the measured zero-field splitting. Using Eq. (\[eq:dE\_phi\]), the splittings can be calculated for the ZFS parameters of the sample. Since the splittings have not been directly measured, we assume that $\epsilon_\text{ZFS}$ is independent of $\phi$. This is valid if the local inhomogeneity of the [$|5/2,1/2\rangle$]{} and the [$|7/2,1/2\rangle$]{} states, which is expected to be of the order of $0.1$ meV, is small compared to the splitting of the Zeeman levels of the dots. The calculated splittings are shown as dashed lines in Fig. \[fig:experimentalmodes\](c). ![\[fig:gateset\] (Color online) Detailed diagram of the pulse sequence used in the measurements of the coherent dipole coupling System Requirements: To install and run the game, you will need the following minimum system requirements. The software is tested on the following machines but other configurations may work as well. 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