{"title":"On a new singular and degenerate extension of the p-Laplace operator","authors":"George Baravdish , Yuanji Cheng , Olof Svensson","doi":"10.1016/j.na.2024.113553","DOIUrl":null,"url":null,"abstract":"<div><p>We study a novel degenerate and singular elliptic operator <span><math><msub><mrow><mover><mrow><mi>Δ</mi></mrow><mrow><mo>˜</mo></mrow></mover></mrow><mrow><mrow><mo>(</mo><mi>τ</mi><mo>,</mo><mi>χ</mi><mo>)</mo></mrow></mrow></msub></math></span> defined by <span><math><mrow><msub><mrow><mover><mrow><mi>Δ</mi></mrow><mrow><mo>˜</mo></mrow></mover></mrow><mrow><mrow><mo>(</mo><mi>τ</mi><mo>,</mo><mi>χ</mi><mo>)</mo></mrow></mrow></msub><mi>u</mi><mo>=</mo><mi>τ</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mi>D</mi><mi>u</mi><mo>)</mo></mrow><mrow><mo>(</mo><mrow><mo>|</mo><mi>D</mi><mi>u</mi><mo>|</mo></mrow><msub><mrow><mi>Δ</mi></mrow><mrow><mn>1</mn></mrow></msub><mi>u</mi><mo>+</mo><mi>χ</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mi>D</mi><mi>u</mi><mo>)</mo></mrow><msub><mrow><mi>Δ</mi></mrow><mrow><mi>∞</mi></mrow></msub><mi>u</mi><mo>)</mo></mrow><mo>,</mo></mrow></math></span> where the singular weights <span><math><mrow><mi>τ</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mi>s</mi><mo>)</mo></mrow><mo>></mo><mn>0</mn></mrow></math></span> and <span><math><mrow><mi>χ</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mi>s</mi><mo>)</mo></mrow><mo>≥</mo><mn>0</mn></mrow></math></span> are continuous functions on <span><math><mrow><mi>Ω</mi><mo>×</mo><msup><mrow><mi>R</mi></mrow><mrow><mi>n</mi></mrow></msup><mo>∖</mo><mrow><mo>{</mo><mn>0</mn><mo>}</mo></mrow></mrow></math></span>. The operator <span><math><msub><mrow><mover><mrow><mi>Δ</mi></mrow><mrow><mo>˜</mo></mrow></mover></mrow><mrow><mrow><mo>(</mo><mi>τ</mi><mo>,</mo><mi>χ</mi><mo>)</mo></mrow></mrow></msub></math></span> is an extension of <span><math><mrow><msub><mrow><mi>Δ</mi></mrow><mrow><mrow><mo>(</mo><mi>p</mi><mo>,</mo><mi>q</mi><mo>)</mo></mrow></mrow></msub><mi>u</mi><mo>=</mo><msup><mrow><mrow><mo>|</mo><mi>D</mi><mi>u</mi><mo>|</mo></mrow></mrow><mrow><mi>q</mi></mrow></msup><msub><mrow><mi>Δ</mi></mrow><mrow><mn>1</mn></mrow></msub><mi>u</mi><mo>+</mo><mrow><mo>(</mo><mi>p</mi><mo>−</mo><mn>1</mn><mo>)</mo></mrow><msup><mrow><mrow><mo>|</mo><mi>D</mi><mi>u</mi><mo>|</mo></mrow></mrow><mrow><mi>p</mi><mo>−</mo><mn>2</mn></mrow></msup><msub><mrow><mi>Δ</mi></mrow><mrow><mi>∞</mi></mrow></msub><mi>u</mi><mo>,</mo><mspace></mspace><mi>p</mi><mo>≥</mo><mn>1</mn><mo>,</mo><mspace></mspace><mi>q</mi><mo>≥</mo><mn>0</mn><mo>,</mo></mrow></math></span> introduced by the authors in Baravdishet al. (2020), which in turn is an extension of the <span><math><mi>p</mi></math></span>-Laplace operator <span><math><mrow><msub><mrow><mi>Δ</mi></mrow><mrow><mi>p</mi></mrow></msub><mo>.</mo></mrow></math></span> We establish the well-posedness of the Neumann boundary value problem for the parabolic equation <span><math><mrow><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><msub><mrow><mover><mrow><mi>Δ</mi></mrow><mrow><mo>˜</mo></mrow></mover></mrow><mrow><mrow><mo>(</mo><mi>τ</mi><mo>,</mo><mi>χ</mi><mo>)</mo></mrow></mrow></msub><mi>u</mi></mrow></math></span> in the framework of viscosity solutions. For the solution <span><math><mi>u</mi></math></span>, the weight <span><math><mi>χ</mi></math></span> controls the evolution along the tangential and the normal directions, respectively, on the level surface of <span><math><mi>u</mi></math></span>. The weight <span><math><mi>τ</mi></math></span> controls the total speed of the evolution of <span><math><mi>u</mi></math></span>. We also prove the consistency and the convergence of the numerical scheme for the finite differences method of the parabolic equation above. Numerical simulations show that our novel nonlinear operator <span><math><msub><mrow><mover><mrow><mi>Δ</mi></mrow><mrow><mo>˜</mo></mrow></mover></mrow><mrow><mrow><mo>(</mo><mi>τ</mi><mo>,</mo><mi>χ</mi><mo>)</mo></mrow></mrow></msub></math></span> gives better results than both the Perona–Malik (Perona and Malik, 1990) and total variation (TV) methods (Chan and Shen, 2005) when applied to image enhancement.</p></div>","PeriodicalId":1,"journal":{"name":"Accounts of Chemical Research","volume":null,"pages":null},"PeriodicalIF":16.4000,"publicationDate":"2024-04-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0362546X24000725/pdfft?md5=6ea663f7ef82d1217c13c05825c4031b&pid=1-s2.0-S0362546X24000725-main.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Accounts of Chemical Research","FirstCategoryId":"100","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0362546X24000725","RegionNum":1,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
We study a novel degenerate and singular elliptic operator defined by where the singular weights and are continuous functions on . The operator is an extension of introduced by the authors in Baravdishet al. (2020), which in turn is an extension of the -Laplace operator We establish the well-posedness of the Neumann boundary value problem for the parabolic equation in the framework of viscosity solutions. For the solution , the weight controls the evolution along the tangential and the normal directions, respectively, on the level surface of . The weight controls the total speed of the evolution of . We also prove the consistency and the convergence of the numerical scheme for the finite differences method of the parabolic equation above. Numerical simulations show that our novel nonlinear operator gives better results than both the Perona–Malik (Perona and Malik, 1990) and total variation (TV) methods (Chan and Shen, 2005) when applied to image enhancement.
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