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We consider concentrated vorticities for the Euler equation on a smoothdomain $\Omega \subset \mathbf{R}^2$ in the form of \[ \omega = \sum_{j=1}^N\omega_j \chi_{\Omega_j}, \quad |\Omega_j| = \pi r_j^2, \quad \int_{\Omega_j}\omega_j d\mu =\mu_j \ne 0, \] supported on well-separated vortical domains$\Omega_j$, $j=1, \ldots, N$, of small diameters $O(r_j)$. A conformal mappingframework is set up to study this free boundary problem with $\Omega_j$ beingpart of unknowns. For any given vorticities $\mu_1, \ldots, \mu_N$ and small$r_1, \ldots, r_N\in \mathbf{R}^+$, through a perturbation approach, we obtainsuch piecewise constant steady vortex patches as well as piecewise smoothLipschitz steady vorticities, both concentrated near non-degenerate criticalconfigurations of the Kirchhoff-Routh Hamiltonian function. When vortex patchevolution is considered as the boundary dynamics of $\partial \Omega_j$,through an invariant subspace decomposition, it is also proved that thespectral/linear stability of such steady vortex patches is largely determinedby that of the $2N$-dimensional linearized point vortex dynamics, while themotion is highly oscillatory in the $2N$-codim directions corresponding to thevortical domain shapes.

Concentrated steady vorticities of the Euler equation on 2-d domains and their linear stability