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Fig. 2.

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Illustrative numerical global MTI eigenmode with m = 50 and n = 20. Top: varying radial wavenumber, k r = E V ftd $ k_r = \sqrt{E - V_{\mathrm{ftd}}} $, as a function of the radius, r. Bottom: a high-order global MTI mode. The turning point, rc, of the mode is indicated by black dashed vertical lines. It can be found as the single solution to the equation kr(r) = 0, indicated by the grey dashed horizontal line on the top panel.

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