For bistable RD fronts, the reaction integral acts as a driving force; a 1D-based reduced model yields explicit blocking thresholds for waveguide–cone geometries when w ≲ 4.
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Blocking of 2D bistable reaction-diffusion fronts by obstacles
For bistable RD fronts, the reaction integral acts as a driving force; a 1D-based reduced model yields explicit blocking thresholds for waveguide–cone geometries when w ≲ 4.