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2104.02196

Defect-mediated dynamics of coherent structures in active nematics

Mattia Serra, Linnea Lemma, Luca Giomi, Zvonimir Dogic, L. Mahadevan

wrongmedium confidence
Category
math.DS
Journal tier
Strong Field
Processed
Sep 28, 2025, 12:56 AM

Audit review

The paper’s instantaneous Eulerian folding-rate formula (SI Eq. (2) and main-text Eq. (8)) includes a minus sign in front of the vorticity-gradient contribution, i.e., −(∇ω·n)/2. Under the stated perpendicular operator ∇⊥ = (−∂y, ∂x) and the standard 2D vorticity definition ω = ∂x v_y − ∂y v_x, the correct sign is plus. A simple check with v(x,y) = (0, (g/2)x^2) at (x,n)=(0,e1) shows the paper’s sign would predict zero curvature growth, whereas the correct plus sign gives κ̇ = g, matching the direct geometry of the advected parabola. The model’s derivation recovers κ̇(t,x,n) = [(∇D n)·n]·n⊥ + (1/2)(∇ω·n), agreeing with the sanity check. See the paper’s stated formulae in SI (Eq. (2)-(3)) and main text (Eq. (8)) for the sign used in the manuscript , and note their perpendicular operator definition ∇⊥ = (−∂y, ∂x) .

Referee report (LaTeX)

\textbf{Recommendation:} minor revisions

\textbf{Journal Tier:} strong field

\textbf{Justification:}

The paper effectively bridges Lagrangian and Eulerian views to analyze folding and coherent structures in active nematics and presents compelling computational and experimental observations. However, the central instantaneous Eulerian folding-rate identity is stated with the wrong sign for the vorticity-gradient term, given the paper’s conventions. This is a fixable issue that should be corrected; clarifying the sign conventions will prevent confusion. The qualitative conclusions and many figures (which use the modulus of the rate) are not undermined by this correction.