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Orbital stability and instability of standing waves for an inhomogeneous logarithmic Schrödinger equation
Abstract
We study the inhomogeneous logarithmic Schrödinger equation i∂tu+Δu+|x|−1ulog|u|2=0, (t,x)∈R×RN, N≥2. For every initial datum in H1(RN), we establish global existence of weak solutions. We also construct explicit positive stationary solutions and solve the associated Nehari minimization problem. For ω≥0, the minimizer is unique up to {a constant} phase and is given by e(N−1)/2(1+√(1+ω)) e−(1+√(1+ω))|x|, whereas for ω<0 the infimum is zero and is not attained. Finally, we prove that the standing waves associated with these profiles are orbitally stable for ω>0 by a variational argument, and orbitally unstable for −1<ω<−1+(N−1)−2 by combining spectral analysis, localized energy and mass estimates, and phase modulation.
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BibTeX
@misc{ardila2026orbital,
title = {{Orbital stability and instability of standing waves for an inhomogeneous logarithmic Schrödinger equation}},
author = {Alex H. Ardila},
howpublished = {arXiv},
year = {2026},
month = nov,
doi = {10.48550/arxiv.2611.07167},
eprint = {2611.07167},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2611.07167},
}
RIS
TY - UNPB
TI - Orbital stability and instability of standing waves for an inhomogeneous logarithmic Schrödinger equation
AU - Alex H. Ardila
PY - 2026
DA - 2026/11/04
PB - arXiv
DO - 10.48550/arxiv.2611.07167
UR - https://arxiv.org/abs/2611.07167
AB - We study the inhomogeneous logarithmic Schrödinger equation i∂_tu+Δu+|x|^−1ulog|u|^2=0, (t,x)∈R×R^N, N≥2. For every initial datum in H^1(R^N), we establish global existence of weak solutions. We also construct explicit positive stationary solutions and solve the associated Nehari minimization problem. For ω≥0, the minimizer is unique up to {a constant} phase and is given by e^(N−1)/2(1+√(1+ω)) e^−(1+√(1+ω))|x|, whereas for ω<0 the infimum is zero and is not attained. Finally, we prove that the standing waves associated with these profiles are orbitally stable for ω>0 by a variational argument, and orbitally unstable for −1<ω<−1+(N−1)^−2 by combining spectral analysis, localized energy and mass estimates, and phase modulation.
ER -