Landau-de Gennes corrections to the Oseen-Frank limit: Anchoring-induced tilt modes
Abstract
An asymptotic analysis of the Landau--de Gennes framework is performed to compute higher-order corrections to the Oseen--Frank limit in a bounded three-dimensional domain under appropriately scaled surface anchoring energy. A systematic decomposition of the Q-tensor into three mutually orthogonal subspaces-the uniaxial scalar, geometric tilt vector, and transverse anisotropy tensor-reveals that the leading πͺ(Ξ΅) correction to the Oseen--Frank director field n0(x) is dominated by a non-vanishing tilt field p1(x), where Ξ΅ represents the ratio of the nematic coherence length to the characteristic domain size. This macroscopic variation constitutes a soft mode released from the boundary once the surface anchoring energy is retained at its physical scaling rather than driven to an infinite strength. We show that this tilt field is governed by the linear Jacobi equation, π₯n0(p1)=0, subject to a non-trivial, anchoring-driven Dirichlet boundary condition, where π₯n0 is the on-shell Jacobi operator of the harmonic map n0 on π2. The two fields are accompanied at πͺ(Ξ΅2) by an off-shell correction to both the uniaxial scalar and the transverse anisotropy tensor, passively induced by the elastic non-uniformity (βn0β 0) and the boundary-driven tilt (p1β 0). Through πͺ(Ξ΅2), the tilt enters the energy only through surface terms, not the bulk, providing a pathway for the system to lower its energy . Under the conventional benchmark of rigid Dirichlet conditions, this response is annihilated outright, demonstrating that corrections built upon infinite energy barriers obscure the underlying physics of anchoring-driven tilt modes.
Related
- Heterogeneity-induced chaos in globally coupled Stuart--Landau oscillators
- Photon induced corrections to Drell-Yan production in POWHEG
- Extended Landau--Lifshitz equation for nanomagnets: a path-integral derivation of surface-induced magnetization nutation
- Observational Viability of Ο2-Superpotential Inflation with GUP-Induced Corrections
- Boundary-induced corrections to the response of an Unruh-DeWitt detector outside a compact star with Robin surface conditions
BibTeX
@misc{rajamanickam2026landaude,
title = {{Landau-de Gennes corrections to the Oseen-Frank limit: Anchoring-induced tilt modes}},
author = {Prabakaran Rajamanickam},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.35127},
eprint = {2609.35127},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.35127},
}
RIS
TY - UNPB
TI - Landau-de Gennes corrections to the Oseen-Frank limit: Anchoring-induced tilt modes
AU - Prabakaran Rajamanickam
PY - 2026
DA - 2026/09/29
PB - arXiv
DO - 10.48550/arxiv.2609.35127
UR - https://arxiv.org/abs/2609.35127
AB - An asymptotic analysis of the Landau--de Gennes framework is performed to compute higher-order corrections to the Oseen--Frank limit in a bounded three-dimensional domain under appropriately scaled surface anchoring energy. A systematic decomposition of the Q-tensor into three mutually orthogonal subspaces-the uniaxial scalar, geometric tilt vector, and transverse anisotropy tensor-reveals that the leading πͺ(Ξ΅) correction to the Oseen--Frank director field n_0(x) is dominated by a non-vanishing tilt field p_1(x), where Ξ΅ represents the ratio of the nematic coherence length to the characteristic domain size. This macroscopic variation constitutes a soft mode released from the boundary once the surface anchoring energy is retained at its physical scaling rather than driven to an infinite strength. We show that this tilt field is governed by the linear Jacobi equation, π₯_n_0(p_1)=0, subject to a non-trivial, anchoring-driven Dirichlet boundary condition, where π₯_n_0 is the on-shell Jacobi operator of the harmonic map n_0 on π^2. The two fields are accompanied at πͺ(Ξ΅^2) by an off-shell correction to both the uniaxial scalar and the transverse anisotropy tensor, passively induced by the elastic non-uniformity (βn_0β 0) and the boundary-driven tilt (p_1β 0). Through πͺ(Ξ΅^2), the tilt enters the energy only through surface terms, not the bulk, providing a pathway for the system to lower its energy . Under the conventional benchmark of rigid Dirichlet conditions, this response is annihilated outright, demonstrating that corrections built upon infinite energy barriers obscure the underlying physics of anchoring-driven tilt modes.
ER -