错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

KFP operators with coefficients measurable in time and Dini continuous in space

  • S. Biagi,
  • M. Bramanti,
  • B. Stroffolini

摘要

We consider degenerate Kolmogorov–Fokker–Planck operators \(\begin{aligned} \mathcal {L}u&=\sum _{i,j=1}^{m_{0}}a_{ij}(x,t)\partial _{x_{i}x_{j}} ^{2}u+\sum _{k,j=1}^{N}b_{jk}x_{k}\partial _{x_{j}}u-\partial _{t}u\\&\equiv \sum _{i,j=1}^{m_{0}}a_{ij}(x,t)\partial _{x_{i}x_{j}}^{2}u+Yu \end{aligned}\) L u = i , j = 1 m 0 a ij ( x , t ) x i x j 2 u + k , j = 1 N b jk x k x j u - t u i , j = 1 m 0 a ij ( x , t ) x i x j 2 u + Y u (with \((x,t)\in \mathbb {R}^{N+1}\) ( x , t ) R N + 1 and \(1\le m_{0}\le N\) 1 m 0 N ) such that the corresponding model operator having constant \(a_{ij}\) a ij is hypoelliptic, translation invariant w.r.t. a Lie group operation in \(\mathbb {R} ^{N+1}\) R N + 1 and 2-homogeneous w.r.t. a family of nonisotropic dilations. The matrix \((a_{ij})_{i,j=1}^{m_{0}}\) ( a ij ) i , j = 1 m 0 is symmetric and uniformly positive on \(\mathbb {R}^{m_{0}}\) R m 0 . The coefficients \(a_{ij}\) a ij are bounded and Dini continuous in space, and only bounded measurable in time. This means that, setting \(\begin{aligned} \mathrm {(i)}&\,\,S_{T}=\mathbb {R}^{N}\times \left( -\infty ,T\right) ,\\ \mathrm {(ii)}&\,\,\omega _{f,S_{T}}(r) = \sup _{\begin{array}{c} (x,t),(y,t)\in S_{T}\\ \Vert x-y\Vert \le r \end{array}}\vert f(x,t) -f(y,t)\vert \\ \mathrm {(iii)}&\,\,\Vert f\Vert _{\mathcal {D}( S_{T}) } =\int _{0}^{1} \frac{\omega _{f,S_{T}}(r) }{r}dr+\Vert f\Vert _{L^{\infty }\left( S_{T}\right) } \end{aligned}\) ( i ) S T = R N × - , T , ( ii ) ω f , S T ( r ) = sup ( x , t ) , ( y , t ) S T x - y r | f ( x , t ) - f ( y , t ) | ( iii ) f D ( S T ) = 0 1 ω f , S T ( r ) r d r + f L S T we require the finiteness of \(\Vert a_{ij}\Vert _{\mathcal {D}(S_{T})}\) a ij D ( S T ) . We bound \(\omega _{u_{x_{i}x_{j}},S_{T}}\) ω u x i x j , S T , \(\Vert u_{x_{i}x_{j}}\Vert _{L^{\infty }( S_{T}) }\) u x i x j L ( S T ) ( \(i,j=1,2,...,m_{0}\) i , j = 1 , 2 , . . . , m 0 ), \(\omega _{Yu,S_{T}}\) ω Y u , S T , \(\Vert Yu\Vert _{L^{\infty }( S_{T}) }\) Y u L ( S T ) in terms of \(\omega _{\mathcal {L}u,S_{T}}\) ω L u , S T , \(\Vert \mathcal {L}u\Vert _{L^{\infty }( S_{T}) }\) L u L ( S T ) and \(\Vert u\Vert _{L^{\infty }\left( S_{T}\right) }\) u L S T , getting a control on the uniform continuity in space of \(u_{x_{i}x_{j}},Yu\) u x i x j , Y u if \(\mathcal {L}u\) L u is bounded and Dini-continuous in space. Under the additional assumption that both the coefficients \(a_{ij}\) a ij and \(\mathcal {L}u\) L u are log-Dini continuous, meaning the finiteness of the quantity \(\begin{aligned} \int _{0}^{1}\frac{\omega _{f,S_{T}}\left( r\right) }{r}\left| \log r\right| dr, \end{aligned}\) 0 1 ω f , S T r r log r d r , we prove that \(u_{x_{i}x_{j}}\) u x i x j and Yu are Dini continuous; moreover, in this case, the derivatives \(u_{x_{i}x_{j}}\) u x i x j are locally uniformly continuous in space and time.