Space-Time Estimates in the Besov Spaces and the Navier-Stokes Equations
Space-Time Estimates in the Besov Spaces and the Navier-Stokes Equations
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DOI:
10.4310/maa.2006.v13.n1.a6
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发表时间:
2006-03
影响因子:
0.3
通讯作者:
Qionglei Chen;Zhifei Zhang
中科院分区:
文献类型:
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作者:
Qionglei Chen;Zhifei Zhang
for vector functions u, v. For given u0 ∈ L2(R) with ∇ · u0 = 0, J. Leray and E. Hopf [17, 20](see also [21, 30]) constructed a global weak solution u(t, x) ∈ L∞(0,∞;L2(R)) ∩ L2(0,∞;H1(R)). It is well known that the weak solution is unique and regular in two spatial dimensions[11, 30]. In dimensions n ≥ 3, however, the question of regularity of weak solutions has remained open in spite of much effort of mathematicians. There are two ways to develop the regularity theory for the Navier-Stokes equations. One is to give a regularity criterion on weak solutions and the other is to study a better partial regularity of weak solutions which are known to exist. For the latter, L. Caffarelli, R. Kohn,L. Nirenberg[4] proved that the one dimensional Hausdorff measure of the singular set is zero, which is the best result at present. J. Serrin[24, 25] is the pioneer in the former research, later on, Fabes, Jones and Riviere[13], Sohr[26], Giga[16], Struwe[27] and Takahashi[28] extended and improved Serrin’s regularity criterion. In order to state their result, we first recall the definition of weak solutions to the Navier-Stokes equations. Definition 1.1. Let u0 ∈ L2(R) with ∇ · u0 = 0. The function u(t, x) will be called a weak solution of (NS) on (0, T ) if u satisfies the following properties: