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        <datestamp>2026-10-02T12:04:09Z</datestamp>
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          <dc:title>Supplementary Movie 2 (br.mp4): Traveling Wave Evolution in the Beeler-Reuter (BR) Model</dc:title>
          <dc:creator>Vincent Lovero (24727126)</dc:creator>
          <dc:creator>Stephanie Dodson (1933168)</dc:creator>
          <dc:creator>Timothy Lewis (21281402)</dc:creator>
          <dc:subject>Biological sciences</dc:subject>
          <dc:subject>Mathematical sciences</dc:subject>
          <dc:subject>cardiac dynamics</dc:subject>
          <dc:subject>action potentials</dc:subject>
          <dc:subject>dispersion curves</dc:subject>
          <dc:subject>fast waves</dc:subject>
          <dc:subject>slow waves</dc:subject>
          <dc:description>This animation illustrates the parameter-dependent evolution of the traveling wave voltage profile (bottom left) and its corresponding linear stability spectrum (right) mapped to the BR dispersion relation (top left). The vertical and horizontal scales for the traveling wave (bottom left) have been normalized. The current state is indicated by a blue marker on the dispersion curve. The pink square denotes a saddle-node bifurcations and green dots denote Hopf bifurcations. As the parameter varies, the fast wave, which  initially features a sharp initial upstroke followed by a brief repolarization and a prolonged plateau, shortens in duration and ultimately transitions into a narrow ``sodium spike' along the slow wave branch. Simultaneously, the  spectrum panel visualizes the linear stability dynamics, showing the fast wave losing stability through a cascade of Hopf bifurcations, visible as multiple eigenvalues crossing into the right half-plane. After passing through the saddle-node bifurcation, a singe real unstable eigenvalue remains and is out of view with $\lambda &gt;0.3.$</dc:description>
          <dc:date>2026-10-02T12:04:09Z</dc:date>
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          <dc:identifier>10.60893/figshare.cha.33472042.v1</dc:identifier>
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          <dc:rights>CC BY 4.0</dc:rights>
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