TY - JOUR
T1 - A Characterization of Harmonic Lr -Vector Fields in Three Dimensional Exterior Domains
AU - Hieber, Matthias
AU - Kozono, Hideo
AU - Seyfert, Anton
AU - Shimizu, Senjo
AU - Yanagisawa, Taku
N1 - Funding Information:
The authors would like to express their hearty thanks to the referee for his/her variable comments. They declare that there is no conflict of interest. The research of the project was partially supported by JSPS Fostering Joint Research Program (B)-18KK0072. The research of H. Kozono was partially supported by JSPS Grant-in-Aid for Scientific Research (S)-16H06339 and Research (A)-21H04433. The research of S. Shimizu was partially supported by JSPS Grant-in-Aid for Scientific Research (B)-16H03945 and (B)-21H00992.
Publisher Copyright:
© 2022, Mathematica Josephina, Inc.
PY - 2022/7
Y1 - 2022/7
N2 - Consider the space of harmonic vector fields u in Lr(Ω ) for 1 < r< ∞ for three dimensional exterior domains Ω with smooth boundaries ∂Ω subject to the boundary conditions u· ν= 0 or u× ν= 0 , where ν denotes the unit outward normal on ∂Ω. Denoting these spaces by Xharr(Ω) and Vharr(Ω), it is shown that, in spite of the lack of compactness of Ω , both of these spaces are finite dimensional and that dimVharr(Ω) equals L for 3 / 2 < r< ∞ and L- 1 for 1 < r≤ 3 / 2. Here L is a number representing topologically invariant quantities of ∂Ω and which in the case of bounded domains coincides with the first Betti number. In contrast to the situation of bounded domains, the dimension of Vharr(Ω) in exterior domains is depending on the Lebesgue exponent r. The critical value of this exponent for exterior domains is determined to be 3/2.
AB - Consider the space of harmonic vector fields u in Lr(Ω ) for 1 < r< ∞ for three dimensional exterior domains Ω with smooth boundaries ∂Ω subject to the boundary conditions u· ν= 0 or u× ν= 0 , where ν denotes the unit outward normal on ∂Ω. Denoting these spaces by Xharr(Ω) and Vharr(Ω), it is shown that, in spite of the lack of compactness of Ω , both of these spaces are finite dimensional and that dimVharr(Ω) equals L for 3 / 2 < r< ∞ and L- 1 for 1 < r≤ 3 / 2. Here L is a number representing topologically invariant quantities of ∂Ω and which in the case of bounded domains coincides with the first Betti number. In contrast to the situation of bounded domains, the dimension of Vharr(Ω) in exterior domains is depending on the Lebesgue exponent r. The critical value of this exponent for exterior domains is determined to be 3/2.
KW - Betti numbers
KW - Exterior domains
KW - Harmonic vector fields
KW - Helmholtz–Weyl decomposition
KW - Jump condition
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U2 - 10.1007/s12220-022-00938-8
DO - 10.1007/s12220-022-00938-8
M3 - Article
AN - SCOPUS:85130249879
SN - 1050-6926
VL - 32
JO - Journal of Geometric Analysis
JF - Journal of Geometric Analysis
IS - 7
M1 - 206
ER -