“…The assertion 1 of this theorem is already established in Proposition 3.1; [21]. The assertions 2 and 3 are proved in section 3 by virtue of Theorem 1.2.…”
Section: Definition 14mentioning
confidence: 64%
“…These estimates are simple variants of the assertions 4 and 5 of Theorem 2.2 in [21]. For reader's convenience, we give a simple proof of the assertion 1 in Section 2 as Proposition 2.2 (see also Proposition 3.2; [21]).…”
Section: Proposition 11mentioning
confidence: 99%
“…As was mentioned before, when γ > 0 holds, the CKN-type inequalities were introduced in [4] as a part of multiplicative interpolation inequalities, and later in [21] the CKN-type inequalities were further investigated for all γ ∈ R. In the present paper, we shall give a simple proof of the CKN-type inequalities (1.2) with p = 1 and the best constant S 1,q ;γ defined below, using equivalence between the CKN-type inequalities with p = 1 and isoperimetric inequalities with weights. We note that in [18] a class of weighted Sobolev inequalities were already studied by using isoperimetric inequalities with general weight functions.…”
Section: Introductionmentioning
confidence: 99%
“…[10,12,13,14,15] and see also [3,20] for p > 1). Recently in [21] the second author of the present paper systematically investigated the CKN-type inequalities involving critical and supercritical weights. More precisely, validity of inequalities, existence of extremal functions, continuity of best constants, symmetry of extremal functions and symmetry breaking of the best constants were established.…”
Section: Introductionmentioning
confidence: 99%
“…More precisely, validity of inequalities, existence of extremal functions, continuity of best constants, symmetry of extremal functions and symmetry breaking of the best constants were established. For this purpose the condition p > 1 was assumed in [21] in most cases, but some results on symmetry were studied including the case where p = 1 as well. On a basis of these observation, we study in the present paper symmetry property of the best constant and its breaking phenomena for the CKN-type inequalities when p = 1.…”
The main purpose of this article is to study the Caffarelli-Kohn-Nirenberg type inequalities (1.2) with p = 1. We show that symmetry breaking of the best constants occurs provided that a parameter |γ| is large enough. In the argument we effectively employ equivalence between the Caffarelli-Kohn-Nirenberg type inequalities with p = 1 and isoperimetric inequalities with weights.
“…The assertion 1 of this theorem is already established in Proposition 3.1; [21]. The assertions 2 and 3 are proved in section 3 by virtue of Theorem 1.2.…”
Section: Definition 14mentioning
confidence: 64%
“…These estimates are simple variants of the assertions 4 and 5 of Theorem 2.2 in [21]. For reader's convenience, we give a simple proof of the assertion 1 in Section 2 as Proposition 2.2 (see also Proposition 3.2; [21]).…”
Section: Proposition 11mentioning
confidence: 99%
“…As was mentioned before, when γ > 0 holds, the CKN-type inequalities were introduced in [4] as a part of multiplicative interpolation inequalities, and later in [21] the CKN-type inequalities were further investigated for all γ ∈ R. In the present paper, we shall give a simple proof of the CKN-type inequalities (1.2) with p = 1 and the best constant S 1,q ;γ defined below, using equivalence between the CKN-type inequalities with p = 1 and isoperimetric inequalities with weights. We note that in [18] a class of weighted Sobolev inequalities were already studied by using isoperimetric inequalities with general weight functions.…”
Section: Introductionmentioning
confidence: 99%
“…[10,12,13,14,15] and see also [3,20] for p > 1). Recently in [21] the second author of the present paper systematically investigated the CKN-type inequalities involving critical and supercritical weights. More precisely, validity of inequalities, existence of extremal functions, continuity of best constants, symmetry of extremal functions and symmetry breaking of the best constants were established.…”
Section: Introductionmentioning
confidence: 99%
“…More precisely, validity of inequalities, existence of extremal functions, continuity of best constants, symmetry of extremal functions and symmetry breaking of the best constants were established. For this purpose the condition p > 1 was assumed in [21] in most cases, but some results on symmetry were studied including the case where p = 1 as well. On a basis of these observation, we study in the present paper symmetry property of the best constant and its breaking phenomena for the CKN-type inequalities when p = 1.…”
The main purpose of this article is to study the Caffarelli-Kohn-Nirenberg type inequalities (1.2) with p = 1. We show that symmetry breaking of the best constants occurs provided that a parameter |γ| is large enough. In the argument we effectively employ equivalence between the Caffarelli-Kohn-Nirenberg type inequalities with p = 1 and isoperimetric inequalities with weights.
Let Ω be a domain in R d with boundary Γ and let d Γ denote the Euclidean distance to Γ. Further let H = − div(C∇) where C = ( c kl ) > 0 with c kl = c lk are real, bounded, Lipschitz continuous functions and D(H) = C ∞ c (Ω). Assume also that there is a δ ≥ 0 suchto be bounded on Γ r . Then we prove that if Ω is a C 2 -domain, or if Ω = R d \S where S is a countable set of positively separated points, or if Ω = R d \Π with Π a convex set whose boundary has Hausdorff dimension d H ∈ {1, . . . , d − 1} then the condition δ > 2 − (d − d H )/2 is sufficient for H to be essentially self-adjoint as an operator on L 2 (Ω). In particular δ > 3/2 suffices for C 2 -domains. Finally we prove that δ ≥ 3/2 is necessary in the C 2 -case.
The best constant of the Sobolev inequality in the whole space is attained by the Aubin-Talenti function; however, this does not happen in bounded domains because the break in dilation invariance. In this paper, we investigate a new scale invariant form of the Sobolev inequality in a ball and show that its best constant is attained by functions of the Aubin-Talenti type. Generalization to the Caffarelli-Kohn-Nirenberg inequality in a ball is also discussed.
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