<i>L</i><sup>2</sup> Concentration of Blow-Up Solutions for the Nonlinear Schrödinger Equation with an Inhomogeneous Combined Non-Linearity

This article studies the Schrödinger equation with an inhomogeneous combined term <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>i</mi><msub><mo>∂</mo><mi>t</mi&...

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Main Authors: Baoli Xie, Congming Peng, Caochuan Ma
Format: Article
Language:English
Published: MDPI AG 2024-04-01
Series:Mathematics
Subjects:
Online Access:https://www.mdpi.com/2227-7390/12/7/1060
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author Baoli Xie
Congming Peng
Caochuan Ma
author_facet Baoli Xie
Congming Peng
Caochuan Ma
author_sort Baoli Xie
collection DOAJ
description This article studies the Schrödinger equation with an inhomogeneous combined term <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>i</mi><msub><mo>∂</mo><mi>t</mi></msub><mi>u</mi><mo>−</mo><msup><mrow><mo stretchy="false">(</mo><mo>−</mo><mo>Δ</mo><mo stretchy="false">)</mo></mrow><mi>s</mi></msup><mi>u</mi><mo>+</mo><msub><mi>λ</mi><mn>1</mn></msub><msup><mrow><mo stretchy="false">|</mo><mi>x</mi><mo stretchy="false">|</mo></mrow><mrow><mo>−</mo><mi>b</mi></mrow></msup><msup><mrow><mo stretchy="false">|</mo><mi>u</mi><mo stretchy="false">|</mo></mrow><mi>p</mi></msup><mi>u</mi><mo>+</mo><msub><mi>λ</mi><mn>2</mn></msub><msup><mrow><mo stretchy="false">|</mo><mi>u</mi><mo stretchy="false">|</mo></mrow><mi>q</mi></msup><mi>u</mi><mo>=</mo><mn>0</mn><mo>,</mo></mrow></semantics></math></inline-formula> where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>s</mi><mo>∈</mo><mrow><mo stretchy="false">(</mo><mfrac><mn>1</mn><mn>2</mn></mfrac><mo>,</mo><mn>1</mn><mo stretchy="false">)</mo></mrow><mo>,</mo><msub><mi>λ</mi><mn>1</mn></msub><mo>,</mo><msub><mi>λ</mi><mn>2</mn></msub><mo>=</mo><mo>±</mo><mn>1</mn><mo>,</mo><mn>0</mn><mo><</mo><mi>b</mi><mo><</mo><mrow><mo>{</mo><mn>2</mn><mi>s</mi><mo>,</mo><mi>N</mi><mo stretchy="false">}</mo></mrow></mrow></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>p</mi><mo>,</mo><mi>q</mi><mo>></mo><mn>0</mn></mrow></semantics></math></inline-formula>. We study the limit behaviour of the infinite blow-up solution at the blow-up time. When the parameters <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>p</mi><mo>,</mo><mi>q</mi><mo>,</mo><msub><mi>λ</mi><mn>1</mn></msub></mrow></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>λ</mi><mn>2</mn></msub></semantics></math></inline-formula> have different values, we obtain the nonexistence of a strong limit for the non-radial solution and the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>L</mi><mn>2</mn></msup></semantics></math></inline-formula> concentration for the radial solution. Interestingly, we find that the mass of the finite time blow-up solutions are concentrated in different ways for different parameters.
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spelling doaj.art-90ab95d2205345b3a00e9b7e89531ca12024-04-12T13:22:45ZengMDPI AGMathematics2227-73902024-04-01127106010.3390/math12071060<i>L</i><sup>2</sup> Concentration of Blow-Up Solutions for the Nonlinear Schrödinger Equation with an Inhomogeneous Combined Non-LinearityBaoli Xie0Congming Peng1Caochuan Ma2School of Mathematics and Statistics, Tianshui Normal University, Tianshui 741000, ChinaSchool of Mathematics and Statistics, Tianshui Normal University, Tianshui 741000, ChinaSchool of Mathematics and Statistics, Tianshui Normal University, Tianshui 741000, ChinaThis article studies the Schrödinger equation with an inhomogeneous combined term <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>i</mi><msub><mo>∂</mo><mi>t</mi></msub><mi>u</mi><mo>−</mo><msup><mrow><mo stretchy="false">(</mo><mo>−</mo><mo>Δ</mo><mo stretchy="false">)</mo></mrow><mi>s</mi></msup><mi>u</mi><mo>+</mo><msub><mi>λ</mi><mn>1</mn></msub><msup><mrow><mo stretchy="false">|</mo><mi>x</mi><mo stretchy="false">|</mo></mrow><mrow><mo>−</mo><mi>b</mi></mrow></msup><msup><mrow><mo stretchy="false">|</mo><mi>u</mi><mo stretchy="false">|</mo></mrow><mi>p</mi></msup><mi>u</mi><mo>+</mo><msub><mi>λ</mi><mn>2</mn></msub><msup><mrow><mo stretchy="false">|</mo><mi>u</mi><mo stretchy="false">|</mo></mrow><mi>q</mi></msup><mi>u</mi><mo>=</mo><mn>0</mn><mo>,</mo></mrow></semantics></math></inline-formula> where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>s</mi><mo>∈</mo><mrow><mo stretchy="false">(</mo><mfrac><mn>1</mn><mn>2</mn></mfrac><mo>,</mo><mn>1</mn><mo stretchy="false">)</mo></mrow><mo>,</mo><msub><mi>λ</mi><mn>1</mn></msub><mo>,</mo><msub><mi>λ</mi><mn>2</mn></msub><mo>=</mo><mo>±</mo><mn>1</mn><mo>,</mo><mn>0</mn><mo><</mo><mi>b</mi><mo><</mo><mrow><mo>{</mo><mn>2</mn><mi>s</mi><mo>,</mo><mi>N</mi><mo stretchy="false">}</mo></mrow></mrow></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>p</mi><mo>,</mo><mi>q</mi><mo>></mo><mn>0</mn></mrow></semantics></math></inline-formula>. We study the limit behaviour of the infinite blow-up solution at the blow-up time. When the parameters <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>p</mi><mo>,</mo><mi>q</mi><mo>,</mo><msub><mi>λ</mi><mn>1</mn></msub></mrow></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>λ</mi><mn>2</mn></msub></semantics></math></inline-formula> have different values, we obtain the nonexistence of a strong limit for the non-radial solution and the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>L</mi><mn>2</mn></msup></semantics></math></inline-formula> concentration for the radial solution. Interestingly, we find that the mass of the finite time blow-up solutions are concentrated in different ways for different parameters.https://www.mdpi.com/2227-7390/12/7/1060inhomogeneous Schrödinger equationL2 concentrationlimit behaviour
spellingShingle Baoli Xie
Congming Peng
Caochuan Ma
<i>L</i><sup>2</sup> Concentration of Blow-Up Solutions for the Nonlinear Schrödinger Equation with an Inhomogeneous Combined Non-Linearity
Mathematics
inhomogeneous Schrödinger equation
L2 concentration
limit behaviour
title <i>L</i><sup>2</sup> Concentration of Blow-Up Solutions for the Nonlinear Schrödinger Equation with an Inhomogeneous Combined Non-Linearity
title_full <i>L</i><sup>2</sup> Concentration of Blow-Up Solutions for the Nonlinear Schrödinger Equation with an Inhomogeneous Combined Non-Linearity
title_fullStr <i>L</i><sup>2</sup> Concentration of Blow-Up Solutions for the Nonlinear Schrödinger Equation with an Inhomogeneous Combined Non-Linearity
title_full_unstemmed <i>L</i><sup>2</sup> Concentration of Blow-Up Solutions for the Nonlinear Schrödinger Equation with an Inhomogeneous Combined Non-Linearity
title_short <i>L</i><sup>2</sup> Concentration of Blow-Up Solutions for the Nonlinear Schrödinger Equation with an Inhomogeneous Combined Non-Linearity
title_sort i l i sup 2 sup concentration of blow up solutions for the nonlinear schrodinger equation with an inhomogeneous combined non linearity
topic inhomogeneous Schrödinger equation
L2 concentration
limit behaviour
url https://www.mdpi.com/2227-7390/12/7/1060
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AT congmingpeng ilisup2supconcentrationofblowupsolutionsforthenonlinearschrodingerequationwithaninhomogeneouscombinednonlinearity
AT caochuanma ilisup2supconcentrationofblowupsolutionsforthenonlinearschrodingerequationwithaninhomogeneouscombinednonlinearity