Abstract:with some Hölder continuous solution that is constant outside (−3/2, 3/2) × T 3 . We also propose a conjecture related to our main result that would imply Onsager's conjecture that there exist energy dissipating solutions to Euler whose velocity fields have Hölder exponent 1/3 − ǫ.
“…In our context, we need to develop a sharp version that works at the critical regularity. Our key tool is an explicit solution operator to the divergence equation [2,3,11] which preserves the compact support property; see Proposition 4.4.…”
Section: Theorem 12 (Small Energy Global Well-posedness In Coulomb Gmentioning
confidence: 99%
“…This solution operator was first used by Bogovskiȋ [2,3]. We remark that a similar solution operator was used in [11] in the context of the incompressible Euler equations.…”
Section: Excision and Gluing Of Initial Data Setsmentioning
confidence: 99%
“…Our construction below follows the approach of [11], in which a similar solution operator was constructed for the symmetric divergence equation ∂ j R j = U . We sharpen the estimates for V compared to [11] (where non-sharp estimates sufficed), which turns out to be necessary due to the criticality of our problem. The class of domains we work with is that of star-shaped domains, and unions thereof.…”
Section: Support-preserving Solution Operator For the Divergence Equamentioning
This paper is the first part of a trilogy [22,23] dedicated to a proof of global well-posedness and scattering of the (4 + 1)-dimensional mass-less Maxwell-KleinGordon equation (MKG) for any finite energy initial data. The main result of the present paper is a large energy local well-posedness theorem for MKG in the global Coulomb gauge, where the lifespan is bounded from below by the energy concentration scale of the data. Hence the proof of global well-posedness is reduced to establishing non-concentration of energy. To deal with non-local features of MKG we develop initial data excision and gluing techniques at critical regularity, which might be of independent interest.
“…In our context, we need to develop a sharp version that works at the critical regularity. Our key tool is an explicit solution operator to the divergence equation [2,3,11] which preserves the compact support property; see Proposition 4.4.…”
Section: Theorem 12 (Small Energy Global Well-posedness In Coulomb Gmentioning
confidence: 99%
“…This solution operator was first used by Bogovskiȋ [2,3]. We remark that a similar solution operator was used in [11] in the context of the incompressible Euler equations.…”
Section: Excision and Gluing Of Initial Data Setsmentioning
confidence: 99%
“…Our construction below follows the approach of [11], in which a similar solution operator was constructed for the symmetric divergence equation ∂ j R j = U . We sharpen the estimates for V compared to [11] (where non-sharp estimates sufficed), which turns out to be necessary due to the criticality of our problem. The class of domains we work with is that of star-shaped domains, and unions thereof.…”
Section: Support-preserving Solution Operator For the Divergence Equamentioning
This paper is the first part of a trilogy [22,23] dedicated to a proof of global well-posedness and scattering of the (4 + 1)-dimensional mass-less Maxwell-KleinGordon equation (MKG) for any finite energy initial data. The main result of the present paper is a large energy local well-posedness theorem for MKG in the global Coulomb gauge, where the lifespan is bounded from below by the energy concentration scale of the data. Hence the proof of global well-posedness is reduced to establishing non-concentration of energy. To deal with non-local features of MKG we develop initial data excision and gluing techniques at critical regularity, which might be of independent interest.
“…A key remark of Isett in [46] compared to [37,38] is that advective derivatives behave much better than simple time derivatives. For instance, since…”
Section: Lemma 71 (The Operator DIV −1 ) There Exists a Homogeneousmentioning
confidence: 99%
“…Statement (B) has been shown for X = L ∞ (0, 1; C 1/10−ε ) in [38], whereas P. Isett in his PhD thesis [46] was the first to prove statement (A) for X = L ∞ (0, 1; C 1/5−ε ), thereby reaching the current best "uniform" Hölder exponent for part (b) of Onsager's conjecture. Subsequently, T. Buckmaster, the two authors, and P. Isett proved statement (B) for X = L ∞ (0, 1; C 1/5−ε ) in [14].…”
Abstract. In this note we present "an analyst's point of view" on the NashKuiper Theorem and, in particular, highlight the very close connection to turbulence-a paradigm example of a high-dimensional phenomenon. Our aim is to explain recent applications of Nash's ideas in connection with the incompressible Euler equations and Onsager's famous conjecture on the energy dissipation in 3D turbulence.
For any " > 0 we show the existence of continuous periodic weak solutions v of the Euler equations that do not conserve the kinetic energy and belong to the space L 1 t .C
1=3 " x/; namely, x 7 ! v.x; t / is . 1 =3 "/-Hölder continuous in space at a.e. time t and the integral R OEv. ; t / 1=3 " dt is finite. A well-known open conjecture of L. Onsager claims that such solutions exist even in the class L 1 t .C1=3 " x /.
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