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Peer-reviewedCC BYCommunications in Mathematical Physics

Linear Fluctuation of Interfaces in Glauber–Kawasaki Dynamics

Abstract

In this article, we find a scaling limit of the space-time mass fluctuation field of Glauber + Kawasaki particle dynamics around its hydrodynamic mean curvature interface limit. Here, the Glauber rates are scaled by K=KN K = K N (with KN↑ ∞ K N ↑ ∞ as N↑ ∞ N ↑ ∞ ), the Kawasaki rates by N2 N 2 and space by 1/ N . We start the process so that the continuum interface Γ t Γ t formed, between ‘high’ ρ + ρ + and ‘low’ ρ - ρ - density regions, is stationary that is, Γ t Γ t is ‘flat’. When the Glauber rates are balanced on 𝕋d T d , the interface Γ t=Γ ={v: v1=0} Γ t = Γ = { v : v 1 = 0 } is immobile and the hydrodynamic limit is given by ρ (t,v) = ρ + ρ ( t , v ) = ρ + for v1∈ (0,1/2) v 1 ∈ ( 0 , 1 / 2 ) and ρ (t,v)= ρ - ρ

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BibTeX
@article{funaki2026linear,
  title = {{Linear Fluctuation of Interfaces in Glauber–Kawasaki Dynamics}},
  author = {Tadahisa Funaki and Claudio Landim and Sunder Sethuraman},
  journal = {Communications in Mathematical Physics},
  year = {2026},
  month = sep,
  doi = {10.1007/s00220-026-05712-3},
  eprint = {2412.04015},
  archivePrefix = {arXiv},
  url = {https://hal.science/hal-05770829v1},
  note = {CC BY},
}
RIS
TY  - JOUR
TI  - Linear Fluctuation of Interfaces in Glauber–Kawasaki Dynamics
AU  - Tadahisa Funaki
AU  - Claudio Landim
AU  - Sunder Sethuraman
PY  - 2026
DA  - 2026/09/27
JO  - Communications in Mathematical Physics
DO  - 10.1007/s00220-026-05712-3
UR  - https://hal.science/hal-05770829v1
AB  - In this article, we find a scaling limit of the space-time mass fluctuation field of Glauber + Kawasaki particle dynamics around its hydrodynamic mean curvature interface limit. Here, the Glauber rates are scaled by K=K_N K = K N (with K_N↑ ∞ K N ↑ ∞ as N↑ ∞ N ↑ ∞ ), the Kawasaki rates by N^2 N 2 and space by 1/ N . We start the process so that the continuum interface Γ _t Γ t formed, between ‘high’ ρ _+ ρ + and ‘low’ ρ _- ρ - density regions, is stationary that is, Γ _t Γ t is ‘flat’. When the Glauber rates are balanced on 𝕋^d T d , the interface Γ _t=Γ ={v: v_1=0} Γ t = Γ = { v : v 1 = 0 } is immobile and the hydrodynamic limit is given by ρ (t,v) = ρ _+ ρ ( t , v ) = ρ + for v_1∈ (0,1/2) v 1 ∈ ( 0 , 1 / 2 ) and ρ (t,v)= ρ _- ρ
SN  - 0010-3616
SN  - 1432-0916
ER  -