Turing patterns on non-fluctuating lattices under mechanical stress modeled by Finsler geometry respond to external forces similarly to those on fluctuating membranes.
10(c), we have H1 → ∑ △ 1 χG i1 χG i2 (χ G i1)2ℓ2 i1 + (χG i2)2ℓ2 i2 = ∑ △ χG i1 χG i2 ℓ2 i1 + χG i2 χG i1 ℓ2 i2 , (A11) which is the same as that in Eq
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Turing patterns on non-fluctuating surfaces under mechanical stresses
Turing patterns on non-fluctuating lattices under mechanical stress modeled by Finsler geometry respond to external forces similarly to those on fluctuating membranes.