J. of Inequal. & Appl., 1997, Vol. pp. 25-46 Reprints available directly from the publisher Photocopying permitted by license only (C) 1997 OPA (Overseas Publishers Association) Amsterdam B.V. Published in The Netherlands under license by Gordon and Breach Science Publishers Printed in Malaysia On Some Fractional Order Hardy Inequalities HANS P. HEINIG a, ALOIS KUFNER and LARS-ERIK PERSSON c Department of Mathematics & Statistics, McMaster University, Hamilton, Ontario, L8S 4K1, Canada b Mathematical Institute, Czech Academy of Sciences, itn 25, 115 67 Praha 1, Czech Repubfic Department of Mathematics, Lule& University, S-971 87 Lule&, Sweden (Received 6 May 1996) Weighted inequalities for fractional derivatives (= fractional order Hardy-type inequalities) have recently been proved in [4] and 1]. In this paper, new inequalities of this type are proved and applied. In particular, the general mixed norm case and a general twodimensional weight are considered. Moreover, an Orlicz norm version and a multidimensional fractional order Hardy inequality are proved. The connections to related results are pointed out. Keywords: Hardy inequality; weight function; fractional order derivative. AMS Subject Classification: 26D 15, 46E30 1 INTRODUCTION Using the notation Ilflls,o for the norm in the weighted Lebesgue space L (0, cx; w) L (w), llfll,,,o (fo0 If(t)lSw(t)dt )l/s with 1 < s < cx and w w(t) a weight function on (0, x), the Hardy inequality can be expressed in the form Ilullq,o0 <_ Cllu’llp,, 25 (1.1) H.E HEINIG et al. 26 with a constant C > 0 independent of u, i.e., under certain conditions, the weighted Lq-norrn of the function u can be estimated by a suitable weighted L P-norm of its (first order) derivative u I. The natural question arises whether it is possible to extend inequality (1.1) to "fractional order derivatives" u (z) with 0 < ) < 1, i.e., under what conditions we can derive inequalities of the type (1.2) and/or IluXllq,0 Cllu’llp,w. (1.3) The first problem which arises is how to understand the expression Let us mention that for the "non-weighted" case (i.e., for w(t) =_ 1) the following definition of IluZlls,1 Ilu<Zlls is commonly used: Ilu(Z)llq,w. [[u(X) lls= (fo fo lU(x) u(y)lS Ix yll+Zs dxdy ) a/s ,1 < s < cxz, O < ) < 1. (1.4) For this special case, the following inequality holds: lu(x)lPx-XPdx lit < Cp Ix y[l+Zp dxdy (1.5) which is inequality (1.2) for the special case p q, wx(x) =-- 1, wo(x) x -xp. Inequality (1.5) was derived by Grisvard [2] provided 1 1 < p < cxz, ,#--, P u6C(O,o). In fact, he rediscovered an earlier result of Jakovlev [3] who has shown that fo c - lu(x) u(O)IPx-)Pdx < C p . fofo [u(x)-u(y)[p Ix y]l+p dxdy. (1.6) Notice that the additional term u (0) at the left hand side of (1.6) is essential since the integral on the left hand side of (1.5) diverges if u is continuous at zero, u(0) 0 and L > FRACTIONAL ORDER HARDY INEQUALITIES 27 The inequality (1.5) was extended in the seventies by Kufner and Triebel [5]: Roughly speaking, they derived instead of (1.2) the inequality Ilullp,m0 C([lu(Zllp,o -t-Ilullp,’) where now lip Ilu(X>llp’ yl I+)p Ix w(x)dxdy (1.7) N is a certain additional weight and wo(x) w (x) x -zp. The double integral in (1.7) offers one possibility of characterizing the still undetermined expression for [lu(X) IIp,w But in spite of the symmetry of the "non-weighted" expression for lu(Zlls in (1.4), we would prefer a certain symmetry in x and y also in the weighted case, i.e., we are looking for a general inequality of the form . fo lu(x)lPw(x)dx <- CP fofo lu(x)-u(y)lp W(x, y)dxdy, (1.9) possibly (but not necessarily) with W (x, y) W (y, x). In Section 4 of this paper we will prove some new inequalities of the type (1.9). Our investigations were motivated by results of Kufner and Persson [4] and Burenkov and Evans [1]. In [4] e.g. the case when W(x, y) w(x) or W(x, y) w(y) is handled, and in [1], the case when W(x, y) w(Ix Yl)lx yl I+zp is treated. For the reader’s convenience and for later purposes, some of these results are briefly discussed and compared Ix yll+Lp in Section 2. Up to now, we dealt with the case p=q and all inequalities mentioned above can be derived more or less directly. Another approach using the theory of interpolation of Banach spaces was used in [4] and led to an inequality of the type H.P. HEINIG et al. 28 (fo cx t (fo(fo 1/q lu(x)lqwo(x)dx < C lu(x)-u(Y)IP Ix yl I+zp w(x)dx) q/p dy )l/q (1.10) i.e., to an expression with a mixed norm on the right hand side for p 5 q. Moreover, it was supposed that 1 < p < q < cxz [while the case q < p is still open] and the authors have not been able to remove the mixed norm for p 5 q. In Section 3, we will prove a new inequality of the type (1.10), moreover, with a measure v(y)dy instead of dy, but again only for p < q. Some of the results obtained in this paper can be extended in various directions. Here we only present and prove an Orlicz norm version of the inequality (1.5) [and of its extension to the power weight case see, e.g., (2.6) with/3 1 + Zp and give an example of a multidimensional fractional order Hardy inequality; see Sections 5 and 6, respectively. We close this introductory ection by noting that in all cases we have considered here we have found that the "fractional" weights w0 in the left integral are always of the type (1.8) for some suitable weight w. Maybe this is supported by the following inequality which is an easy consequence of (1.5) and of the fact that u belongs to the weighted space LP (w) if and only if uw 1/p belongs to the (non-weighted) space LP. lu(x)lPw(x)x-ZPdx <C fo lu(x)w 1/p (x) Ix u(y)w 1/p (y)l p dxdy. yl I+xp (1.11) Also the fight hand side in (1.11) could serve as a definition of the expression Ilu()llp,w, 2 SOME PRELIMINARY RESULTS AND DISCUSSIONS For the special case when the weight function W (x, y) in the fight hand side of (1.9) depends on Ix Y I, Burenkov and Evans [1] recently proved the following interesting result: FRACTIONAL ORDER HARDY INEQUALITIES 29 THEOREM 2.1 Let 0 < p < o, let w be a weight function on (0, o) and define v(x) w(t)dt. Suppose that v satisfies the A2-condition, i.e., there exists a constant c > 0 such that v(2t) _< cv(t) for all t > 0. LP (O, cx; v) Then for all u lu(x)lPv(x)dx <_ C p lu(x) u(y)lPw(lx yl)dxdy. For later purposes we also state the following slight improvement of the recent result by Kufner and Persson mentioned in the introduction: THEOREM 2.2 Let 1 < p < o and ) >_ -1/p. Furthermore, assume that the function u satisfies lim 1 x-- cx X fo x O. u(t)dt Let wo and wl be weight functions on (0, e) satisfying B" sup x>0 with p’ fo P__e_ p_l (fo x wo(t)dt Then, for every > O, [u(x)lPwo(x)dx < C p fofo w (t)dt t xlu(x)-u(y)lp Ix yl < cx W(x)dydx (2.1) (2.2) where W(x) and C p x-l wo(x) + x-l-Ptol (X) 2 p-1 max(l, Cp) with Cp <_ B pP (p 1) 1-p. The proof of Theorem 2.1 is similar to that of Proposition 1 in [4] but for the reader’s convenience we present here the details. H.P. HEINIG et al. 30 First we use an idea by Grisvard [2] (cf. also p. 261 in Triebel [9]) and define Proof u(x) g(x) u’(y)- - [u(x) x u(y)]dy. (2.3) u(z) and Obviously, g() u’(y) u(y)dy x u(y) y + and we conclude that 1 u(y) for u(x)dx + g(y) g(Y) y dx x g(y)- g(x) dx. x Therefore by using the inequality la + bl p <_ 2p-I(IaIP -q-IblP), the assumption (2.1) and Hardy’s inequality (see, e.g., [7]) we obtain that o ]u(x)lPwo(x)dx < 2 p-1 < 2 p-1 2P-1 (fo (fo [g(x)lPwo(x)dx + fo [g(x)lPwo(x)dx -I- Cp wo(x) o fg(x_) g(Y) dy Y 11)1(x) x Pdx ) Pdx Ig(x)lPWo(x)dx where Wo(x) wo(x) + CpX-Pll)I (x). Therefore, by denoting W1 (x) -p x wo(x) + Wl (x) and using (2.3) we find that [u(x)lPwo(x)dx <C fo(fo <C [g(x)lPWl(x)dx x lu(x) u(y)ldy ) Wl (x)dx. (2.4) Furthermore, by H61der’s inequality and the assumption/3 > 0, we find that FRACTIONAL ORDER HARDY INEQUALITIES ( f0 x 31 x lu(x) <__ x-PxP-1 u(y)ldy < u(y)[Pdy lU(X) x -1 f,x [u(x) -xU(Y)IP dy X/-1 lu(x) fx Jo Ix u(y)l p y[ dy. The estimate (2.2) follows by combining (2.4) and (2.5). COROLLARY 2.3 Let 1 < p < x, 13 >_ O, limx-c 2 u (t)dt O, then >_ --1/p and t > )p 1. If f fo [u(x)[Pxa-Pdx < C p foCfoX]U(X)-u(Y)[Px#-l-ZP+adydx.(2.6) Proof Apply Theorem 2.2 with wo(x) x a-zp and tO1 (X) a-zp-1 Let us note that applying Theorem 2.1 with w(t) X t-’kp+p. we find that for a < )p we have fo c [u(x)IPxa-ZPdx < C p Ix foCfoClu(x)-u(Y)lP ix yl+X p yldxdy. (2.7) Moreover, Theorem 2.1 cannot be used for any ot >_ p (since then v(x) =_ o). But using Corollary 2.3 we see that (2.7) holds also if .p _< c < )p / 1 This fact follows from (2.6) putting there/3 0 and noting that x--XP+ _< Ix y[-1-LP+a for all y, 0 < y _< x and -1 -)p + ot <0. More generally, using Theorem 2.2 with/3 decreasing we obtain an inequality of the type [u(x)lPwo(x)dx <_ C p lu(x) 0 and with W(x) strictly u(y)lPW(lx yl)dxdy, (2.8) and this inequality cannot be obtained in general using Theorem 2.1 e.g. in the case that the integral w(t)dt is divergent. Another inequality of the type (2.8) can be obtained by using our Theorem 4.1 with w(x, y) w(lx y[) (see Remark 4.5). fx H.P. HEINIG et al. 32 3 THE GENERAL (MIXED NORM) CASEp q Let to and v denote weight functions on (0, o). Moreover, define y V(y) v(x)dx, fo dx (Au)z(x, y): In(x) v(x)dx v(y), u(y)l yl x Ix The main result of this section reads as follows: THEOREM 3.1 Let 1 < p < q < o, ) > and Cp,q sup r>0 Then for u c l/p, ) wz (x) frOO (fo [wx (x)v -q (x)]l-q’dx (x)dx -zq 1/q wL (x) V -q O)p,q (X)X )l/q’ < cx. (3.1) L q (0, x; tox) lu(x)lq tox(x)dx) 1/q (3.2) I(Auz,)(x, y)l p to(x)dx] q/p v(y)dy)1/q provided K-- Cp,qq (q- 1)l/q’ Remark 3.2 Note that for the case v(y) inequality (1.10) with - 1-p’(t)dt) 1 we obtain the mixed norm x WO(X to,(X) X (-’k+l/p’)q (3.3) < 1. to -q/p’ FRACTIONAL ORDER HARDY INEQUALITIES Proof (f0 33 HSlder’s inequality yields y lu(x)l- u(y)lv(x)dx (foy < [u(x) )q u(y)[Pw(x)dx )q/P (JoY (uP(x)) e- q/p’ \ w(x) Therefore > 0 cx y_q/p_)q vp (X) Y dx) \ w(x) -q/P’ y lu(y) v(x)dx y jo u(x)v(x)dx] q v(y)dy foy u(x)v(x)dxlqdy" 1 V(y) wx(y)lu(y) Using this estimate together with the Minkowski and Hardy inequalities [the latter one can be used due to (3.1)] we find that (oC ]u(y)lqwz(y)dy ) 1/q <_ (jo wx(y)lu(y) -Jr- (fOOC wz(y)V-q (y) i V(y) (for jo u(x)v(x)dxlqv(y)dy),q y lu(x)lv(x)dx )q )l/q dy H.P. HEINIG et al. 34 w(x)dx Ix Yl +K v(y)dy w)(y)lu(y)lqdy Inequality (3.2) follows by subtracting and using (3.3). Considering the case p q in Theorem 3.1 we obtain Colot,al, 3.3 Cp If l <p< , -l/p, wx(x) Op,p(X)X -xp and wz (x) V -p (x)dx sup r>0 (zr (wz (x)v-P (x))-P’dx )alp’ < , then c fo lu(x)lPwx(x)dx) lip < 1 1-K p (fofolU(X)-u(y). w(x)v(y)dxdy) Ix-yl I+zp liP (3.4) provided K= Cpp (p- 1)l/p’ < 1. Consequently, (3.4) may be regarded as a fractional order Hardy inequality of the type (1.9) with the weight W(x, y) w(x)v(y) on the right hand side. Remark 3.4 Applying Corollary 3.3 with w(x) 1 and with 1, v(y) u (x) replaced by u (x) u (0) we find that if 1 < p < cx, ) > 1/p, then (f0 lu(x)-u(O)lPx-ZPdx) 1/p < )p_t_ p l )p 1 (fo fo lU(x) Ix u(y)l p dxdy yl I+xp )lip (3.5) FRACTIONAL ORDER HARDY INEQUALITIES 35 cf. formula (1.6). Moreover, it is not difficult to see that (3.5) holds with 0 < ) < 1 and with the constant 1/2) / (1 )) for p 1. Remark 3.5 Theorem 3.1 requires a certain integrability of v and (vPw-1)1--r- on (0, y) for y > 0. This requirement can be replaced by an integrability condition on (y, cx), if one modifies the proof of Theorem 3.1 as follows: Let fy v(x)x-1/P-’-3dx V(y) with some real parameter 3, and wx (y) v(y) w(x) ,I vq (y)" x-e’dx Now, we use the estimate l(Au)z(x,Y)l p foC (fo ifr l fo (fy w(x) )q/P lU(x)-u(Y)’ p > v(y)dy w(x)dx )q/P v(y)dy and denote the last double integral by J. Since H61der’s inequality yields (fy (fy < lu(x) u(y)l x1/p+.+6 v(x)dx lu(X)-u(y)Ip we obtain that x+@ w(x)dx )q/P(fyCX:(l)P(x)) \ w(x) @f- x-’P’dx ) q/p’ H.P. HEINIG et al. 36 Then we proceed as in the proof of Theorem 3.1, using the Minkowski inequality and the Hardy inequality the last one assuming that Cp,q < c where (fo t .(fr(L(x)v-q(x)xq/P+,q+3q)l-q’dx) r Cp,q sup r>0 x (xl -q (x)dx Finally, we obtain again inequality (3.2) provided with Cp,qq K 1/q (q- 1)l/p’ 1/q’ wz (x) replaced by z (x) < 1. 4 A GENERAL WEIGHT IN TWO VARIABLES FOR p = q In this section, we will prove the following assertion: THEOREM 4.1 Letto(x, y) be a non-negative measurablefunction on (0, o) (0, o), locally integrable in both variables separately. Let 1 < p < o and ) >_ -lip. (i) Denote x (xl_. f0 col-p’(x, W(x) and Wx (x) Cp" t)dt W (x)x -zp. If sup r>0 wl-p’(x)x)P’dx x pO+l--------ydx < (4.1) and K= then foru Cpp (p- 1)l/p’ <1, LP(O, o; Wz) (f0 Wx(x)lu(x)lPdx) 1/p (4.2) p y)dxdy) 1-K (foOfolU(X)-u(y)l 1 Ix-yl l+xp co(x, liP FRACTIONAL ORDER HARDY INEQUALITIES 37 (ii) Denote (f0y col-p’(t, W(y) and y)dt "(x)x -zp. If (x) (fo W (y)yXP’dy)lip’ r Cp" =sup yp(Z+l) r>0 dy 1-p’ (4.3) and Cpp (p- 1)l-p’ then (4.2) holds with Proof < 1, Wz and K replaced by Wz and K, respectively. Obviously lu(x) fo Ix u(y)l p co(x, y)dxdy yl l+xp _fofoXlU(X)-u(y)l Ix p oo(x, y)dydx yl +xp fx + fo > + x u(y)l p lu(x) ...ix...2. yl./.p.., w(x, y)dydx u(y)l p lu(x) xl+.p fx co(x, y)dydx lU(X) --..u(Y)l p co(x, y)dydx yl+Xp I1 + I2. H61der’s inequality yields x X(u(x) u(y))dy < (fo (fo col-P’(x,t)d lu(x) u(y)IPco(x, y)dy x t ) H.P. HEINIG et al. 38 and consequently I1 >_ foX W(x)xI-p xl+,p W(X) lu(x) xp u(y))dyl p (U(X) x u(y)dyl p IXU(X) xl+,p fo fox l x fo x u(y)dyl p Hence, by the Minkowski and Hardy inequalities, we have and since K < 1, (4.2) follows at once. Part (ii) can be proved completely analogously, estimating now from below the integral 12, which can be rewritten by Fubini’s theorem as I2 f0 y Itt(X) u(y)l p yl+,p og(x, y)dxdy. But it follows also directly from part (i) using the following symmetry argument: Since for h(x, y) lu(x) u(y)lPlx yl --xp we have h(x, y) h(y, x), the fight hand side in (4.2) satisfies h(x, y)w(x, y)dxdy h(x, y)w(y, x)dxdy. If we denote for tOl (X, y) w(y, x) by Wl(x) the function, which corresponds to tO1 as W corresponds to tO, we have that Wl(x) W(x), the of of instead W. and now we proceed as in proof part (i) with W1 FRACTIONAL ORDER HARDY INEQUALITIES 39 Remark 4.2 The proof of Theorem 4.1 shows that in fact we can derive a better inequality provided (4.1) and (4.3) hold simultaneously: (1 K) (foOO + (1 < Wx(x)lu(x)lPdx Wx(x)lu(x)lPdx K) (fo fo lU(x)_u(y)l p x COROLLARY 4.3 Let 1 < p < o, yll+Xp o)(x, y)dxdy >_ -1/p and )l/p < )p- 1. Then u(O)IPxa-XPdx lu(x) < )lip Zp + p -ot ;p ot l 1 (fo fo . (4.4) lU(X) Ix u(y)lP xadxdy y I+zp Proof Apply Theorem 4.1 (i) with u(x) replaced by u(x) u(O) and x Then W(x) x a and (4.1) holds with Cp (p 1) 1/p’/(zp + p ot 1) provided ct p) p < -1 and -tpt/p + ,kp’ + 1 > 0, i.e., if ot + 1 < p(. + 1). But this is the case if ot + 1 < )p. Moreover, K p/(Zp + p- t 1) < 1 if ot + 1 < )p. with o(x, y) w(x) Remark 4.4 For the case ct 0, the statement in Corollary 4.3 follows also at once from our Corollary 3.3 (see Remark 3.4). Moreover, according to Corollary 1 in [4] (cf. our Theorem 2.2), the following complement also holds: If 1 < p < c, Z > -1/p and ct > )p 1, then (fo lu(x)[Px-XPdx )l/p (foC fo <_ C lu(x)_u(y)lp Ix yll+Xp xadxdy )lip (4.5) where C + p/(ot ;p + 1)). For ct 0, the inequalities (4.4) and (4.5) coincide with the inequalities (1.6) and (1.5) mentioned in Section 1. 2 p-1 (1 Remark 4.5 By applying Theorem 4.1 with og(x, y) w(Ix Yl)lx y1-1-xp we obtain another inequality of the Burenkov-Evans type (see Theorem 2.1). In particular by using this result with w(x) x we rediscover the inequality (2.7). H.P. HEINIG et al. 40 Remark 4.6 In Theorem 4.1, we in fact used the integrability of col-p’ (x, y) either with respect to x or with respect to y on intervals (0, z), z > 0. If this condition is not fulfilled, we can proceed in a similar way as in Remark 3.5: We estimate the integral Ie from the proof of Theorem 4.1, fofxlU(x)-u(y)l yl+Zp 12 p co(x, y)dydx, from below using the following H61der inequality: c u(x) u(y) yl/p+)+ < P CO(X, y)dy (fxlU(X)__u(y)lp yl+.p CO(X y)dy )(fx y-P’CO(x y)dy )p-1 with a suitable parameter 6. Here, the role of the function W (x) is played by (fxCXZ y-P’CO(x, W* (x) y)dy i.e., we need the integrability of CO(x, y)y-aP’ with some 6 in the neighbourhood of infinity. The remaining steps are similar as in the proof of Theorem 4.1 (i) and are left to the reader (see also Remark 3.5). Let us mention that condition (4.1) is then replaced by r C" sup r>O (fo (fo W*(x)dx )lip c W *I-p’(x) xl/p’-P’+’+’dx) the function Wz (x) W(x)x -zp in (4.2) is replaced by W*(x). X 1-1/p-L-3 and the parameter 6 has to satisfy 6 > 1 1/p A similar result can be obtained using the integrability of x-aP’CO(x, y) (as a function of x !) in the neighbourhood of infinity if we proceed analogously with I1 rewritten (by Fubini’s theorem) as c i1 f0c fy pxl+.p lu(x)-u(y)l CO(x, y)dxdy. FRACTIONAL ORDER HARDY INEQUALITIES 41 5 A GENERALIZATION TO THE ORLICZ NORM , In this section we will modify inequalities (1.5) and (2.6), i.e., the case with power weights x using the norm in a suitable Orlicz space. For this purpose, let P be a Young function satisfying the A2-condition. Then it is well-known that there exists a/ > 0 such that for all K > 1, P(ct) <_ tc P(t). (5.1) If H is the Hardy (averaging) operator defined by lf0X (Hu)(x) x u(t)dt and both P and its complementary function P satisfy the A2-condition, then Palmieri [8] (cf. also [6, Corollary 4]) proved that lltuullp IltVHulle 1 (5.2) v where the norm in (5.2) is the Orlicz norm. [If v < 0 then the condition that P A2 can be omitted.] It is well known that the Orlicz norm I1" II P and the Luxemburg norm I1" 117o defined by Ilgll," inf [tk > 0" ( ) e !g(x)l k dx satisfy Ilgll, Let 0 < ) < IlgllP 211gll,. 1 and denote vz(x)= v(x) xX (Au)z(x, y) u(y) Ix- yl z u(x) further, let I1" IIe(z) denote the twodimensional Orlicz norm on (0, o) x dxdy (0, cx) with respect to the measure d/x Ix-yl The main result of this section reads as follows. H.P. HEINIG et al. 42 If P and P satisfy (5.1) with the constant THEOREM 5.1 l+X,8 > O, then for < 1, (5.4) CIl(Au)xlle( Iluxlle where 2(1 + 1 +/3()- 1) Moreover, if ) > 0 the condition that P satisfies (5.1) may be omitted. Proof The convexity of P yields fofo >- fo fo ( fofo (,u(x)-u(y),)dxdy Ix Ix P P(l(Au)zl)dlz x P x >_ P u(y)l lu(x) xz e yl z yl ) dY x x ( fo x u(y)l lu(x) xx ) dy dx P (luz(x) (Hu)z(x)l)dx The Minkowski inequality, the estimates (5.3) and the (Hardy) inequality (5.2) with v -) yield IluxllP Ilux (Hu)) + (Hu)xll, Iluz (Hu)zllP + II(Hu)zlle _< 211ux (nu)zllo + IIt-znulle _< , t 211(zXu)zllp(u / 1 +/3) IluzllP <_ 211(Au)zllP( 41 +/, Iluxlle and (5.4) follows immediately. Of course (5.3) shows that (5.4) holds also with Orlicz norms replaced by the Luxemburg norms. FRACTIONAL ORDER HARDY INEQUALITIES 43 6 AN N-DIMENSIONAL FRACTIONAL ORDER HARDY INEQUALITY We are also able to prove some N-dimensional versions of the inequalities N N, B(Ixl) will denote the ball mentioned. First some notation: For x {y NN; lyl _< Ixl} and IB(Ixl)l its volume. It is IB(Ixl)l IxlNISN-11/N where S u-1 is the unit sphere in N u and IsN-I its area. THEOREM 6.1 Let 1 < p < cxz, N > 1 and p > 1. Then ixlXP------ dx 2N(l+Xp/PN1/p [p(l /,k)_ l] ,p 1 IsN-111/P (f f v lu(x)_u(y)l p v Ix ylN(+Xp) )liP dydx/(6.1) Proof Obviously J" = N lu(x)-u(Y)lP fr Ix-yl N(l+xp) (Ixl) l 2N(I+Xp) > IX yl N(I+xp) dydx IX flII-N(I+Z’P) fB N since for y B(Ixl), it is inequality yields (u(x) -u(y))dy (Ixl) dydx Ix Yl u(y)lPdydx lU(X) (Ixl) < 21xl, and 1 + Lp > 0. But H61der’s <-(fB lU(X)-u(y)lPdy) IB(Ixl)l p-1 (Ixl) and consequently J > 2N(I+Lp) l 2N(+Xp) 1 2 N(I+Lp) (u(x) ixlNO+Xp f fe ’B(IxI)II-p ixlN(+Zp) B(Ixl) Ixl N<I/zp u(y))dylPdx (Ixl) u(y)dylPdx lu(x)lB(lx[)l(Ixl) lu(x) In(Ixl)l (Ixl) u(y)dylPdx. (6.2) H.P. HEINIG et al. 44 Therefore, by Minkowski’s inequality (f lu(x)l p N ----ff-dx ]xlXP )alp u(y)dy ixlzpNlU(x)--In(Ixl)l l (lxl> }alp u(y)dylPdx lip ixlXpN u lu(x)- IB(lxl)l-Pf ixlXPN u(y)dylPdx In(Ix])l (Ixl) u(y)dyl pdx (Ixl) }/P --=11+12. (6.3) It follows from (6.2) that 2N(I+)p)/PN1/P I1 < ]sN-111/p j1/p (6.4) and the Hardy inequality with power weights yields 12 <_ Cp (P_P1)l/p, (flIIu(x)IP) [x[PN lip dx provided Cp.--sup(fl r>0 ’B(IxI)I-P dx Ix [ZpN x l> sup r>0 N-1 Yr )l/P(f x <r NP dtdcr) ISN-1IP N-I-LpN-Np (fsu_l for tN-X+XP’Ndtdcr) IxI-LpN(1-P’)dx) 1/p’ 1/p 1/p’ r(N-Np-)pN)/p + ,) N) 1/p N[sN-11-1 [sN-1 [1/p+a/p’ sup (Np(1 r>0 r ()p’N+N)/p’ (,p’N + N)I/P Hence 12 < P" (p- 1)I/P p(1 + )) 1 1/p (fRo [u(x)lPdx) IxlXP and inequality (6.1) follows by the last estimate with (6.2)-(6.3) and subtracting. combining p(l+Z)-I FRACTIONAL ORDER HARDY INEQUALITIES 45 Remark 6.1 Inequality (6.1) is an N-dimensional counterpart of inequality (1.5), i.e., with weight 1 on the right hand side. Of course, also more general cases can be considered. Let us mention at least the following more dimensional extension ofTheorem 4.1; we omit the proof since the arguments are quite similar to the onedimensional case. THEOREM 6.2 Let co(x, y) be a non-negative measurable function on N x N, locally integrable in both variables separately. Let 1 < p < cx and -lip and denote W(x) (IB( i)1 fa(Ixl) col-p’ (X, t)dt) 1-p If Ix Cp" sup r>0 and K { fx < i>r P Cp (p_l)l/p, W(x) N W(x) ixlXP, wl_P,(x)dx Ix [.pN N 1/p iSN_l 1/p’ < 1, then IxlXp g lu(x)lPdx 1 1- K N1/P2N(I+Xp)/P(f ]sN-1] lip ] e ]u(x)--u(y)l p u Ix- y]U(l+kp) co(x, y)dydx) X/p Acknowledgements The work of the second author was partially supported by the Grant Agency of Czech Republic, Grant No. 201/94/1066. References [1] V. Burenkov and W.D. Evans, Weighted Hardy’s inequalities for differences and the .extension problem for spaces with generalized smoothness (to appear). [2] P. Grisvard, Espaces interm6diaires entre espaces de Sobolev avec poids,Ann. Scuola. Norm. Sup. Pisa., 23 (1969), 373-386. [3] G.N. Jakovlev, Boundary properties of functions from the space Wpt) on domains with angular points (Russian), Dokl. Akad. Nauk SSSR, 140 (1961), 73-76. [4] A. Kufner and L.E, Persson, Hardy inequalities of fractional order via interpolation, WSSIAA (1994), 417-430. [5] A. Kufner and H. Triebel, Generalizations of Hardy’s inequality, Conf Sem. Mat. Univ. Bari, 156 (1978), 21 pp. 46 H.P. HEINIG et al. [6] L. Maligranda, Generalized Hardy inequalities in rearrangement invariant spaces, J. Math. pures et appl., 59 (1980), 405-415. [7] B. Opic and A. Kufner, Hardy-type inequalities, Longman Scientific & Technical, Harlow (1990). [8] G. Palmieri, Un approcio alia teoria degli spazi di traccia relativi agli spazi di Orlicz-Sobolev, Bol. U.M.L, (5), lli-B (1979), 100-109. [9] H. Triebel, Interpolation Theory, Function Spaces, Differential Operators. 2na edition, Johann Ambrosius Barth Verlag, Heidelberg-Leipzig, 1995.