2018
DOI: 10.1016/j.na.2018.01.004
|View full text |Cite
|
Sign up to set email alerts
|

On restrictions of Besov functions

Abstract: In this paper, we study the smoothness of restrictions of Besov functions. It is known that for any f ∈ B s p,q (R N ) with q p we have f (·, y) ∈ B s p,q (R d ) for a.e. y ∈ R N −d . We prove that this is no longer true when p < q. Namely, we construct a functionWe show that, in fact, f (·, y) belong to B (s,Ψ) p,q (R d ) for a.e. y ∈ R N −d , a Besov space of generalized smoothness, and, when q = ∞, we find the optimal condition on the function Ψ for this to hold. The natural generalization of these results … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

0
5
0

Year Published

2019
2019
2020
2020

Publication Types

Select...
2

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(5 citation statements)
references
References 39 publications
0
5
0
Order By: Relevance
“…On the contrary, assuming that the Lorentz-force contribution dominates the free-streaming contribution, this implies ε α−1 δ 2 − δ − ε α+β ≪ 0, which leads also to a contradiction as first δ → 0 and next ε → 0. In conclusion, if αβ + β + 3α − 1 > 0, then the right-hand side of (71) vanishes as (ε, δ) → 0, and we obtain the renormalized Vlasov equation (26). We continue with the local-in-space entropy conservation law (28).…”
Section: Remarkmentioning
confidence: 72%
See 2 more Smart Citations
“…On the contrary, assuming that the Lorentz-force contribution dominates the free-streaming contribution, this implies ε α−1 δ 2 − δ − ε α+β ≪ 0, which leads also to a contradiction as first δ → 0 and next ε → 0. In conclusion, if αβ + β + 3α − 1 > 0, then the right-hand side of (71) vanishes as (ε, δ) → 0, and we obtain the renormalized Vlasov equation (26). We continue with the local-in-space entropy conservation law (28).…”
Section: Remarkmentioning
confidence: 72%
“…for all Φ ∈ D((0, T ) × R 6 ). We now establish the renormalized Vlasov equation (26). Using regularity assumptions ( 23)-( 25), (67), Lemma 1 and 2, we obtain from (68),…”
Section: Remarkmentioning
confidence: 95%
See 1 more Smart Citation
“…Following a suggestion of the first author, Brasseur investigated the non restriction property established in Proposition 6.11. In [10] (which is independent of the present work), Brasseur extends Proposition 6.11 to the full range 0 < p < q ≤ ∞; the construction is somewhat similar to ours (based on the size of the coefficients µ j in the decomposition (6.8)), but relying on a different decomposition (subatomic instead of wavelets). [10] also contains an interesting positive result: it exhibits function spaces X intermediate between B s p,q (R) and ε>0 B s−ε p,q (R) such that, if f ∈ B s p,q (R 2 ), then for a.e.…”
Section: Remarkmentioning
confidence: 79%
“…More generally, B 0 p,q (Ω; S 1 ) has the lifting property when L ∞ → B 0 p,q . 10 The remaining cases are open.…”
Section: Open Casesmentioning
confidence: 99%