In this paper, we are interested in the existence and concentration of normalized solutions for the following logarithmic Schrödinger–Bopp–Podolsky type system involving the 𝑝-Laplacian in ℝ3: ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩ −𝜀𝑝⁢Δ𝑝⁢𝑢+𝑍⁡(𝑥)⁢|𝑢|𝑝−2⁢𝑢−𝜅⁢𝜙⁢𝑢=𝜆⁢|𝑢|𝑝−2⁢𝑢+|𝑢|𝑝−2⁢𝑢⁢log⁡|𝑢|𝑝 in ℝ3, −𝜀2⁢Δ⁢𝜙+𝑎2⁢𝜀4⁢Δ2⁢𝜙=4⁢𝜋⁢𝑢2 in ℝ3, ∫ℝ3|𝑢|𝑝𝑑𝑥=𝑑𝑝⁢𝜀3, where Δ𝑝 ⋅ =div⁡(|∇⋅|𝑝−2∇ ⋅) denotes the usual 𝑝-Laplacian operator, 𝑍 is a given external potential, 𝜅 >0 a constant, 𝑎 >0 is the Bopp–Podolsky constant and 𝜀 >0 is a small parameter. The unknowns are 𝑢,𝜙 :ℝ3 →ℝ and the Lagrange multiplier 𝜆 ∈ℝ. If 𝑝 ∈[2, 12 5 ), we obtain, via the variational method, that the number of positive solutions depends on the profile of 𝑍 and the solutions concentrate around the global minimum points of 𝑍 in the semiclassical limit as 𝜀 →0+.

Existence and concentration of normalized solutions for logarithmic Schrödinger–Bopp–Podolsky type system

Gaetano Siciliano
;
2025-01-01

Abstract

In this paper, we are interested in the existence and concentration of normalized solutions for the following logarithmic Schrödinger–Bopp–Podolsky type system involving the 𝑝-Laplacian in ℝ3: ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩ −𝜀𝑝⁢Δ𝑝⁢𝑢+𝑍⁡(𝑥)⁢|𝑢|𝑝−2⁢𝑢−𝜅⁢𝜙⁢𝑢=𝜆⁢|𝑢|𝑝−2⁢𝑢+|𝑢|𝑝−2⁢𝑢⁢log⁡|𝑢|𝑝 in ℝ3, −𝜀2⁢Δ⁢𝜙+𝑎2⁢𝜀4⁢Δ2⁢𝜙=4⁢𝜋⁢𝑢2 in ℝ3, ∫ℝ3|𝑢|𝑝𝑑𝑥=𝑑𝑝⁢𝜀3, where Δ𝑝 ⋅ =div⁡(|∇⋅|𝑝−2∇ ⋅) denotes the usual 𝑝-Laplacian operator, 𝑍 is a given external potential, 𝜅 >0 a constant, 𝑎 >0 is the Bopp–Podolsky constant and 𝜀 >0 is a small parameter. The unknowns are 𝑢,𝜙 :ℝ3 →ℝ and the Lagrange multiplier 𝜆 ∈ℝ. If 𝑝 ∈[2, 12 5 ), we obtain, via the variational method, that the number of positive solutions depends on the profile of 𝑍 and the solutions concentrate around the global minimum points of 𝑍 in the semiclassical limit as 𝜀 →0+.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11586/600361
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