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On semiclassical states for Dirac equations
Zeitschrift für angewandte Mathematik und Physik ( IF 2 ) Pub Date : 2021-05-02 , DOI: 10.1007/s00033-021-01541-7
Abderrazek Benhassine

This paper aims to study the existence and concentration of solutions for the stationary Dirac equation in \(\mathbb {R}^3\) with critical nonlinearities:

$$\begin{aligned} i\varepsilon \sum \limits _{k=1}^3\alpha _k\partial _k u-a\beta u+V(x)u=P(x)f(|u|)u+Q(x)g(|u|)u, \end{aligned}$$

where \(\varepsilon >0\) is a small parameter and \(a>0\) is a constant. We also show the semiclassical solutions \(\omega _\varepsilon \) with maximum points \(x_\varepsilon \) concentrating at a special set \({\mathcal {H}}_{P}\) characterized by V(x), P(x) and Q(x), and for any sequence, \(x_\varepsilon \rightarrow x_0\in {\mathcal {H}}_{P}, v_\varepsilon (x):=\omega _\varepsilon (\varepsilon x+x_\varepsilon )\) converges in \(H^1(\mathbb {R}^3,\mathbb {C}^4)\) to a least energy solution u of

$$\begin{aligned} i\sum \limits _{k=1}^3\alpha _k\partial _k u-a\beta u+V(x_0)u=P(x_0)f(|u|)u+Q(x_0)g(|u|)u. \end{aligned}$$


中文翻译:

关于Dirac方程的半经典状态

本文旨在研究具有临界非线性的\(\ mathbb {R} ^ 3 \)中平稳Dirac方程解的存在性和集中性:

$$ \ begin {aligned} i \ varepsilon \ sum \ limits _ {k = 1} ^ 3 \ alpha _k \ partial _k ua \ beta u + V(x)u = P(x)f(| u |)u + Q(x)g(| u |)u,\ end {aligned} $$

其中\(\ varepsilon> 0 \)是一个小参数,而\(a> 0 \)是一个常数。我们还示出了半经典的解决方案\(\欧米加_ \ varepsilon \)与最大值点\(X_ \ varepsilon \)浓缩在一组特殊的\({\ mathcal {H}} _ {P} \),其特征在于VX),  Px)和Qx),以及任意序列\ {x_ \ varepsilon \ rightarrow x_0 \ in {\ mathcal {H}} _ {P},v_ \ varepsilon(x):= \ omega _ \ varepsilon(\ varepsilon x + x_ \ varepsilon)\)收敛于\(H ^ 1(\ mathbb {R} ^ 3,\ mathbb {C} ^ 4)\)至最小能量解

$$ \ begin {aligned} i \ sum \ limits _ {k = 1} ^ 3 \ alpha _k \ partial _k ua \ beta u + V(x_0)u = P(x_0)f(| u |)u + Q (x_0)g(| u |)u。\ end {aligned} $$
更新日期:2021-05-03
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