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Importance of Second Order Resetting. Comparison of |λ max | for the case in which f 2 (φ) is neglected (without f 2 (φ), open circles) and the case in which it is considered (with f 2 (φ), filled diamonds) plotted against the synaptic conductance strength. For both cases, |λ max | is less than one up to .07 mS/cm 2 , predicting stability for the two cluster solution. In this range, the eigenvalue with the largest absolute value is |λ 1 |, which does not include a contribution from f 2 (φ). Beyond .07 mS/cm 2 when f 2 (φ) is considered (filled diamonds), the eigenvalue with the the largest absolute value is λ 2 , which correctly predicts that the cluster mode loses stability for conductances greater than .08 mS/cm 2 . This diverges from the case where f 2 (φ) is ignored (open circles); neglecting f 2 (φ) incorrectly predicts stability up to .18 mS/cm 2 (circles).  

Importance of Second Order Resetting. Comparison of |λ max | for the case in which f 2 (φ) is neglected (without f 2 (φ), open circles) and the case in which it is considered (with f 2 (φ), filled diamonds) plotted against the synaptic conductance strength. For both cases, |λ max | is less than one up to .07 mS/cm 2 , predicting stability for the two cluster solution. In this range, the eigenvalue with the largest absolute value is |λ 1 |, which does not include a contribution from f 2 (φ). Beyond .07 mS/cm 2 when f 2 (φ) is considered (filled diamonds), the eigenvalue with the the largest absolute value is λ 2 , which correctly predicts that the cluster mode loses stability for conductances greater than .08 mS/cm 2 . This diverges from the case where f 2 (φ) is ignored (open circles); neglecting f 2 (φ) incorrectly predicts stability up to .18 mS/cm 2 (circles).  

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... can enforce synchrony within each cluster, even if neither cluster is capable of 379 synchronizing in isolation [32]. The key is the multiplicative nature of the factors that scale 380 the perturbation in separate intervals. ...
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