1. Introduction

In this essay some recent results concerning Trudinger-type imbedings will be presented. These results are based mainly on paper [a] by Stephen M. Buckley and Julann O'Shea. Results from other sources will be quoted as appropriate and additionally some extensions of mine will be considered.
The Trudinger inequality is an improvement over the Sobolev inequality in the case where the exponent of the gradient's norm equals the dimension of the underlying space: The Sobolev-inequality tells us that
(1.1)
where is the closure of Ck in the Sobolev space W1,p(see e.g. [e, p. 148], [g, p. 97]) for a domain of sufficient regularity ( by assuming more regularity of the domain, we can also remove the index "0" in (1.1)). We see that the right hand side of (1.1) becomes undefined when n=p. For this p, (1.1) suggests that the Sobolev can be imbedded into Lp for any p 1, which is in fact true. However an imbedding into L is not possible; the Sobolev inequalities provide no best imbedding for this case. The situation was remedied in 1967 when Neil Trudinger found an imbedding of this Sobolev space into an Orlicz space defined by an exponential function. The assumptions on the domain as well as on the measures involved in the norm structure of the spaces have since been relaxed.
In [a] the Trudinger inequliaty is extended to cases where the Lebesgue measure is replaced by more general measures. Most previous undertakings have supposedly concentrated on weighted generalizations of Sobolev and Hölder-type imbeddings (the latter term refers to imbeddings of Sobolev spaces with p>n) and today most research in this area is concentrated on extending previous results to metric spaces. However, as will be seen, the imbedding problem is far from settled even in the Euclidian setting, to which we will restrict ourselves.
This paper is organized as follows: Chapter 2 presents the background needed to understand the classical (non-weighted) Trudinger inequality, and concludes with a problem statement. Chapter 3 describes some conditions that can be imposed on the domain and the measures involved in order that some imbedding results may be derived. Since these concepts might be unfamiliar, some examples are included; these also serve to establish some limits of what we can hope to achieve in terms of imbeddings. Chapter 4 determines some combinations of domains and measures that admit an imbedding. Conversely, chapter 5 shows some cases in which such imbeddings are not possible, i.e. attempts at proving certain sharpness results for the imbeddings. Finally chapter 6 presents a summary of what has been accomplished and strives at making some statements of what more could be done.

2. Background

It will be assumed throughout that is a bounded domain (open and connected) in Rn, and n is the dimension of the space. Further, and are real borel measures supported on and m denotes the Lebesgue measure mn. The notation will be used for the Ln+s norm when there is no danger of confusion.
The following shorthand notation will be used: u , is the weighted average of u over :
,
Similarly u ,f is the average weighted by the measure defined by d :=f dm and u is the ordinary average over . The convention indicated, writing f instead of f dm and a blank or a 1 instead of m will also be used more generally.
The unquantified (that is, lacking subscripts or explicit functional dependencies) "c" or "C" will stand for any constant, and its value may vary even in a single expression (i.e. we might say that u v if and only if cu<v<cu). The "constant" usually depends on n, the domain and possibly other parameters as well. A prime " ' " after a constant symbol denotes the conjugate exponent of the constant: p':=p/(p-1).

2.1 The Orlicz spaces
Let f be a convex homeomorphism [0, ) [0, ) (The Orlicz function of the class/space). We define the Orlicz class Lf( , ) by
,
and the Orlicz space Lf*( , ) as the linear hull of the Orlicz class (W1n denotes the Sobolev space). Equipped with the Luxemburg norm,
(2.1) ,
Lf*( , ) is a Banach space (see e.g. [d] for more information on Orlicz spaces). We note some results from that book:
Lemma 2.1 Let f,g be Orlicz functions. If for every c>0, , we write g f. We identify an Orlicz function with the equivalence class of all functions where the above ratio is finite and non-zero for every c>0. Then defines a linear order. Moreover, equivalent functions define the same Orlicz space and Lf*( , ) is properly contained in Lg*( , ) if and only if g f.
Proof: [d, p. 104].

2.2 The Trudinger inequality
We say that a triple ( , , ) supports or satisfies an s-Trudinger inequality (also written as ( , , ) s-T) if
(2.2) ,
where u , is the average of u over , fs(x):=exp(x(n+s)')-1 and s 0. Note that fs ft if and only if s<t. For this kind of Orlicz function, the Orlicz norm dominates the Lp-norm for every 1 p< and the L -norm dominates the Orlicz norm. Hence we see, in view of what was said in the introduction, that this kind of Orlicz functions define spaces that are potentially useful in the limiting case of the Sobolev inequlity as indeed it proved to be: Trudinger showed that ( , 1, 1) 0-T provided satisfies an uniform interior cone condition, and Smith and Stegenga relaxed this condition to domains satisfying a quasi-hyperbolic boundary condition (see below, 3.1.1).
Note that in order to take the average u , we must either have ( )< or resort to a limiting process. Since we allow pretty arbitrary domains and measures, it would be difficult (perhaps impossible) to devise a limiting process that would be useful for all domains and measurs so the latter alternative is not viable.

Lemma 2.2 A triple ( , , ) supports an s-Trudinger inequality if and only if the following inequality holds for every t 1:
(2.3) .
Sketch of proof: Insert the right-hand-side of the inequality as "t" in the definition of the Orlicz norm. By taking the terms in the expansion of fs as a power series one at the time, we see that (2.1) implies (2.3) for every integer, whence the lemma follows by interpolation. On the other hand inserting the estimate (2.3) into the power series expansion of fs in (2.1), we conclude the converse also.

2.3 Problem statement
Since the idea in proving (2.1) is to find an imbedding of the Sobolev space on a certain domain into an Orlicz space on the same domain, it would seem that there are at least to different interesting scenarios: a) Given and find, if possible, some (hopefully quite regular) and the greatest s, such that ( , , ) s-T; b) Given , and determine for which (if any) s ( , , ) s-T.
Buckley and O'Shea seem preoccupied with the latter task, which in a sense is a prerequisite to the former. However in pursuing the latter we may make certain assumptions not reasonable given the former objective.

3. Tools for the generalized Trudinger type inequality


Throughout this essay, if X is a geometrical entity with center x0, c0X is the concentric dilate of X scaled by a factor c0, i.e. . Some of the examples in this section are not from [a]. The reason for this deviation is that it seems that these examples are better suited to the more general case under consideration, whereas those in [a] are remnants from the Lebesgue case.

3.1 Geometrical conditions
The following lemma from [a] is presupposed:
Lemma 3.1 (Whitney decomposition) can be covered by a countable set of disjoint cubes {Qj} satisfying: a) 100 d(Qj, ( )/diam(Qj) 300; b) the 20-fold dilate of the cubes covers no point more then c(n) times.
The cubes may be chosen to be dyadic. A fixed set of cubes satisfying the above conditions for the given domain will be denoted W( ). Moreover the following notation will be used, (x):=d(x, ) and Q is the diameter of Q. Hence condition a) says that (x) Q for x Q. Every Whitney cube is of approximately the same quasi-hyperbolic diameter (see the next section).

3.1.1 Quasi-hyperbolic distance
We define the quasi-hyperbolic distance between two points x and y by:
,
where the infimum is taken over the set of rectifiable curves joining x and y completely contained in . For a domain this is actually a minimum, i.e. there exists a geodesic, x,y for which the integral attains its infimum. As (x) Q for x Q for a Whitney cube Q, we see that the geodesic passes through approximately k (x,y)+1 Whitney cubes. In the plane (n=2) the quasi-hyperbolic metric for a simply connected domain is comparable to the hyperbolic metric [c].
We say that satisfies a quasi-hyperbolic boundary condition (abbreviated: " is QHBC") if there exists a constant c>1 such that
(2.3)
for every x belongs and a fixed y belongs . We call y the QHBC-center of , and the smallest c for which (2.3) is valid the QHBC constant of with center y, c ,y. Quasi-hyperbolicity of the boundary is a property of the domain, not the center, i.e. if (2.3) is true for some center, it is true for any point as center point, although, as indicated, the QHBC constant depends on the choice of center. A simply connected planar domain is QHBC if and only if its boundary is Hölder continuous.

3.1.2 The Slice-condition
We say that has a c0-slice property with respect to center y belongs if for every x belongs there is a path 0:[0,1] with endpoints x and y and a disjoint collection of open sets {Si}ki=0 with y S0, x Sk satisfying:
(a) x and y are in different components of for every 0<i<k,
(b) for any curve through x and y we have for every 0<i<k, diam(S'i, )<c0len(S'i, inter ) for some >0, where ,
(c) for some xi Si inter , with x0=y and xk=x, Bi:=B(xi, ri/2) is contained in Si where ri:=diam(Si)/c0 and
(d) for every t [0,1] there is some i such that d( (t),Si)< <c0diam(Si).
We say that satisfies a slice condition if it has a c-slice property for some finite c.

It was proved in [f] that a domain is QHBC if it has a slice property and supports a 0-Trudinger inequality with Lebesgue measures. Hence, if has a slice property, belongsQHBC eqiv( ,1,1) s0-T. This prompts Buckley and O'Shea to claim in [a] that QHBC is the natural class of domains to associate with the Trudinger inequality.
Condition (b), which is stronger than the corresponding condition in [f], says that the slices may not be very oblong and the -condition says that this "evenness" is not achieved by having thin segments (in particular exterior cusps). Condition (d) is a formal relaxation of the corresponding condition in [f] (which requires the c0 in (d) to be equal to zero), saying that the slices cover some fixed portion of the slice-path in a uniform manner, but is actually no more general, although perhaps sometimes easier to use.
In view of condition (a) there are basically two types of slices, "annular" slices which enclose either point (but not both) and "flat" slices that stretch all the way across the domain from boundary to boundary. Although the latter are perhaps what comes to mind by only reading the definition here, the annular type is important, as it arrises naturally when a uniform domains is mapped quasi-conformally onto a domain, which then has a slice-property [a, teorem 2.4] (see also lemma 3.2, below).

3.1.3 The weak slice condition
We say that satisfies a c0-weak slice condition with center y if for every point x belongs there is a number mx 0 and a collection of disjoint open sets , that satisfies conditions (a) and (b) (with k=mx+1) above (3.1.2) and additionally
(c') 1+mx>(1 + k (x,y))/c0 and
(d') B:=B(y, (y)/c0) and B0:=B(x, (x)/c0) are disjoint from every Si.

By noting that 1+k (x,y) is dominated by the number of Whitney cubes through which a path from x to y passes, we see that (c)&(d) (from 3.1.2) imply (c') with mx=k-1. Also (c) implies (d'). Note that since we allow mx=0, any part of , in which k (x,y) is bounded, in particular every point in any satisfies the weak slice condition.

Lemma 3.2 Every QHBC domain satisfies a weak slice condition.
Proof: Let be a QHBC domain with center y and QHBC-constant c , normalized so that (y)=1. Let a point x belongs be given. By the remark after the definition of the weak slice condition, we may assume that (x)<1/8. Then let and Si:=B(x,2i (x)) \ B(x,2i-1 (x)) for 1 i mx. We immediately see that these sets satisfy condition (a), (b) and (d). Finally (c) is just a restatement of the defining property of QHBC domains (2.3) for this choice of mx.

3.2 Conditions on the measures
All measures under consideration are assumed to be positive real borel measures supported on .

3.2.1 Doubling measures
We say that a measure is locally doubling if we have:
,
We easily deduce the following properties of locally doubling measures:
Lemma 3.3 Let be locally doubling. Then
a) if (Q)=0 for some cube Q, q0 likewise for ,
b) for every cube Q, ,
c) for a compact K in with d(K, )>0, satisfies and
d) is locally doubling if and only if, for every adjacent Q1 and Q2, 1/c0 (Q1)< (Q2)<c0 (Q1), where c0 does not depend on the specific cubes.
Sketch of proof: b) is trivial if q so assume (Q)< and arrive at a contradiction by assuming ( Q)>0. Statement c) follows by a a argument similar to that following the definition of the weak slice property, above. d) follows since adjacent Whitney cubes are approximately equal in size.

Example 3.1 Let d :=fdm, where if and if . Then clearly is not locally doubling. However, even so ( , , ) s0-T if satisfies a uniform interior cone condition. This can be seen by repeating Trudinger's original proof mutatis mutandis since (Q)=m(Q) for every Whitney cube. We thus see that local doubling is not a necessary condition for a Trudinger inequality.

We say that a measure is in the strong doubling class Dt( ) for t>1/2, if for every ball B, the 1/t-fold dilate of which belongs to , satisfies (2B inter )<c (B inter ) for some fixed c. Obviously every strongly doubling measure is locally doubling.
Note that the essential difference between the two doubling conditions lies in the constraints they impose on the boundary behavior of measures, as the Whitney cubes to which the local doubling is tied do not reach the boundary in a finite number of steps.
We denote by r:={x belongs | (x)<r} the interior boundary of thickness r of . Define Li:= 2-i\ 2-i-1. We say that a measure is non-localized doubling if for any Q1, Q2 belongsW( ) both of which intersect Li (Q1) (Q2). We see that every non-localized doubling measure is locally doubling. However strong doubling and non-localized doubling are disjoint consepts. On an intuitive level, we see that whereas strong doubling constrains the behaviour of a locally doubling measure in all directions, in particular towards the boundary, non-localized doubling is a more restrictive than strong doubling along the boundary, but equivalent to local doubling in approaching the boundary. Any measure defined by d :=f( (x))dm where f is a continuous is a non-localized doubling measure. It is strongly doubling if f is uniformly continuous.

3.2.2 Some Lebesgue measure-conditions
We define the Muckenhoupt A1( ) class as consisting of those functions for which the following condition is valid: for every cube Q the double of which is contained in the inequality
(2.4)
holds. We define the Reverse Hölder class, RH , as consisting of the functions satisfying, under the same condition on Q,
(2.5) .
In both cases dm denotes the n-dimensional Lebesgue measure of . Note that in particular these conditions are then satisfied for every Whitney cube.
Every Muckenhoupt and Reverse Hölder measure is locally doubling. It is worth noting the difference between how the local doubling condition is strenghtened by additionally assuming strong doubling or either (2.4) or (2.5). The former extends the same doubling behavior to the borders of the domain, the later has about the same global behavior, but forces the measure to look locally like the Lebesgue measure.

3.3 Balance conditions
We define the quantity (X) where X is a Whitney cube or a ball in by:

where X denotes diam(X) (as already defined for cubes). It will be worth keeping in mind that the closeness of (X) to 1 in some sense measures how well resembles a Lebesgue measure in n+s dimensional space, i.e. one in which the volume of a cube scales as the n+sth power of the diameter.
We say that the pair of measures ( , ) is locally balanced provided for every Whitney cube Q. Similarly they are globally balanced if
(2.6) ,
for every Qx belongsW( ), where the sum is taken over a chain of Whitney cubes connecting Qx to a fixed central cube Q0. If and are locally doubling on , the choice of Q0 is immaterial for the satisfiability of (2.6) since the new center is only a finite number of chain cubes removed from Q0 and the value of (Q), (Q) and Q vary only by at most a bounded amount from one cube to an adjacent one. Since (2.6) is an increasing function of c, it may again be satisfied for a possibly higher choice of c. Clearly the global condition implies the local one. Since there are only a finite number of Whitney cubes in any compact subset of , we see that the balance conditions actually restrict the behavior of the measures only near the boundary.
Since we may always discount a finite amount of cubes from consideration by choosing a large enough constant, we see that unless (Q) the local doubling condition is trivially satisfied for any finite (and we will restrict ourselves to such , as already noted). Likewise (2.6) is trivially true if S (Q) is convergent for every chain of cubes converging to the boundary. The limiting case for the global balance condition is in a sense that in which (Q) 1, which is satisfied by the measure defined by d = s(x)dm. Hence these measures may be considered as canonical examples of measures satisfying the balance condition.
As will be shown in the next chapter, the local and global balance conditions are often necessary or sufficient for a domain to support a Trudinger inequality. Since we concluded that the balance condition is relevant only for small cubes (which are near the boundary), we can also consider the following intuitive notion: if the local balance condition is satisfied non-trivially for s=0, the measure "resembles" the Lebesgue measure, which is flat and hence does not take the shape of the boundary into consideration. If on the other hand for s>0 this implies that "looks like" s(x)dm, and is hence influenced by the shape of the boundary. With this intuition in mind it is easy to appreciate that the cases s=0 and s>0 will be delt with separately in several theorems.

4. The imbeddings theorems


In this chapter we will present most results from [a] that show relationships between the conditions on the measures, conditions on the domain and supportability of an s-Trudinger inequality. Throughout the chapter it will be assumed that and are locally doubling and that is a bounded domain with finite measure.

Lemma 4.1 ( , , ) supports an s-Trudinger inequality if and only if for every Whitney cube Q, .
Proof: By using the triangle inequality of the Orlicz norm, we see that the the lemma follows if we can bound ||uQ, u , || by the Ln+s norm of the gradient. However, by the following formula
,
and its counterpart with Q and interchanged, recalling that the Orlicz norm dominates the L1 norm and that is finite, we complete the proof by invoking the s-Trudinger inequality.
Spurred by the lemma we let Q0 be a fixed Whitney cube containing the point x0, called respectively the central cube and the center (of ), for the rest of this chapter.

Theorem 1 (a necessary condition) If ( , , ) supports an s-Trudinger inequality then ( , ) is locally balanced .
Proof: We may discount a finite number of cubes from our consideration by choosing a sufficiently large constant in the balance condition, so we restrict our attention to Whitney cubes Q, satisfying (2Q) interQ0. Fix some such cube, Q, and a function u: [0,1] dominating cQ supported in 2Q, with |--u|<c Q. To see that the last condition can be satisfied, recall that d( Q, (2Q)) Q by the definition of the Whitney cubes. Hence, applying the s-Trudinger inequality to u we obtain:
,
where the first approximation is best verified by inserting the logarithm into "t" in the defining equation of the Orlicz norm, (2.1), keeping in mind that ( ) is finite. The last approximtion follows from |--u|<c Q.

Proposition 1 (a necessary condition) If ( , ,w) s0-T with w sA1( ) then w(x)>cw>0 for every x s .
Proof: Since w sA1( ) it suffices to show that wQ is bounded from below by (2.4). Fix a Q with center z, different from the central cube Q0. Define u(x):=f(|z-x|), where f is continuous, decreasing and linear on each of the intervals Ai:=[2-i-1 Q,2-i Q] for every i belongs to 1, , k, for a fixed but arbitrary k, and constant elsewhere with f(x)=0 for x> Q. Further choose the slopes so that for ever i k. Then . Furthermore since w dm is locally equivalent to the Lebesgue measure, we deduce that u(x) wQ 1/nk(n 1)/n, for every x in the central constant region x<2-k-1 Q, where the proportionality constants depend only on the Muckenhoupt constant of w. Hence we have the following inequality:
(4.1) ,
where c0 is bounded by the Muckenhoupt constant of w and C is the local doubling constant of . In the second inequality (B) was approximated by the local doubling condition along the chain B:=B(z,2-k-1 Q), 2B, ..., 2k+1B. This is permissible, since 2iB is contained in Q for i k.
Suppose we require that the the left hand side of (4.1) is less than 1, which can always be achieved for a fixed u by choosing t large enough. If we could apply the Trudinger inequality to the Lipschitz function u, we could conclude that this is possible with t uniformly bounded from above (since ||--u||=1). Hence, since k can be chosen arbitrarily large, by checking the sign of k in the exponent, we derive wQ>cw>0 with the constant not depending on Q. By approximating u with a series of continuously differentiable functions, we conclude the proof.
This is the first instance of the special case of s=0 comes into play, as mentioned after the definition of the balance conditions. We also note that this proposition contrasts the behavior of (the canonical representatives) dm and s(x)dm, of which the former is bounded away from zero and the latter is not.

Theorem 2 (a necessary condition) ( , ) is globally balanced if ( , , ) supports an s-Trudinger inequality, sDC1 ( ) and satisfies has a C1-slice property.
Proof: Fix a Whitney cube Q containing the point x. As above, we may neglect a finite number of cubes and hence assume that the slice path cover consists of more than two sets (i.e. k>1 in the definition). Using the notation from the definition of the slices (see 3.1.2), we remind that Bi is a ball that is contained in the slice Si and centered on the slice path.
We will first prove the following inequality:
(4.2) ,
which is the global balance condition with the balls taking the place of the Whitney cubes. For this purpose we define the functions
,
where the infimum is taken over all rectifiable paths containing y and x0 and the ai are constants that will be specified later. By the the triangle inequality in Euclidian space, we conclude that every ui is Lipschitz with constant ai (Bi)-1/(n+s), which is hence also a bound for the absolute value of the gradient.
Recall that Si is contained in 2C1Bi, where C1 is the slice constant of the domain. Hence by the strong doubling of we conclude that (Si) (Bi) and consequently that the Ln+s( , ) norm of --ui is bounded by cai. Moreover, using property (b) of the slice condition to bound the infimum, we derive ui(y) ai (Bi)-1/(n+s)ri=ai 1/(n+s)'(Bi) for every y sQ, since ri Bi. Set u:=S1k-1ui and , with the constant "a" chosen so that the sum of the ain+s is normalized to 1:
.
Hence the Ln+s( , ) norm of --u is bounded and u(y) a(S (Bi))=a-(n+s-1) for every y sQ. Also u(y)=0 for every y sB0 by condition (a) and (c) of the slice property so that uB0, =0. Therefore we have
(4.3) .
We see that the global balance condition for the balls would follow if we could apply the s-Trudinger inequality to the Lipschitz function u. However, it is fairly simple to produce a series of approximating functions owing to the strenghtened condition (b) of the slice condition: we simply apply a smoothening integral transform, the kernel of which is supported on an -sized ball and of total weight one ("a mollifier", see [e, p. 140]), to the function u(x)- for points of S'i, (defined in 3.1.2). Letting approach zero, we see that the C1 approximating function will have both value and gradient approximating that of u. Thus we have proved the global balance condition for balls.
But this implies the global balance condition (for the Whitney cubes). Because, as is a doubling measure, (Bi) (Qi) where Qi is any Whitney cube, the intersection with Bi of which is non-empty and ri Qi since both are defined in terms of ratios of the distance of the set to the boundary of . The balls cover only some portion of the slice path, but this is unimportant: for a cube Q on between Bi and Bi+1, (Q) is comparable to (Bi), and furthermore there are only a bounded amount of such Q for every ball in the chain, hence the global balance condition.

Lemma 4.2 (a) If p>n and u sL1,p(Q), for a cube Q, then
(4.4) .
Hence we have:
(4.5)
(b) If u sC1(Q), we have for n p< and q< with C=C(n, p, q):
(4.6) .
(c) If q=jn', C(n, p, q) j!(a(n, p))j in (4.6).
Proof: (a) The classical (local) Hölder imbeding result (4.4) leads to (4.5) if we use the estimate |x-y| Q, integrate over d (y) and divide by (Q), raise both sides to the power of j(n+s)' and integrate over x. (b) The classical Poincaré inequality [e, p. 157, (7.44)], with the gradient's exponent changed by means of the Hölder inequality. (c) Follows directly from lemma 2.2, since (Q,m,m) certainly satisfies a (zero-)Trudinger inequality. Inserting t=q=jn' the claim follows by Hölder's inequality since we may estimate the Ln mean-"norm" by the Lp mean-"norm" as n p and m(Q) is finite.
Note that both (4.4) and (4.6) are local inequalities. Consequently, if is locally equivalent to the Lebesgue measure, in particular A1 or RH , we can replace the mean on either side by the my-weighted mean.

Theorem 3 (a sufficient condition) Let d =w dm with w sA1( ) be globally balanced and let shrink so fast that
(4.7) ,
for some positive . If s>0 then ( , , ) supports a s-Trudinger inequality. If s=0, the same conclusion follows if the following additional conditions are true: w(x)>cw>0 and d =v dm where sRH ( ),
Proof: By scaling , and u s) respectively, we may assume that diam(Q0)=1, ( )=1/2 and ||--u||Ln+s( , )=1. We must thus show that fs(|u|/t) is bounded by a constant for some t>0 uniformly bounded from above. Let where . By lemma 2.1 fs' and fs define the same Orlicz space. By the triangle inequality and the convexity of fs' we have the pointwise estimate fs'(|u(x)-uQ0, |/t)<fs'(|u(x)-uQ, |/t)+fs'(|uQ0, uQ, |/t), where x belongs to Q. We call the first type of term "good" and the second kind "bad" and denote by G and B, respectively, their total integrals.
Expanding fs' as a power series we have conclude that
(4.8) .
Assuming s=0 we may use the estimate from lemma 4.2(c) with p=n in (4.8) by the remark following that lemma. Noting that Qn/ (Q) m(Q)/ (Q) 1/cw, and that ||--u|| 1, we arrive at the inequality:
,
so any G is bounded for any t>a1/n'.
If s>0, we instead apply the estimate (4.5) from Lemma 4.2(a) (again invoking the local equivalence of and the Lebesgue measure):
.
Inserting this into (4.8) noting that ||--u||n+s=1 and interchanging the order of summation (positive summands), we see that
,
where the local balance condition was used for the last inequality. Hence the good terms are bounded by assumption (4.7) in the case s>0 case also.
We still have to estimate the bad terms, i.e.
(4.9) .
Using the triangle inequality, we estimate
(4.10),
where {Qi} is the chain of Whitney cubes from the global balance condition (we implicitly assume, without loss of generality, that k-1 is even). Now we derive the estimate:
.
The second inequlity follows from the fact that 9Qi+1 contains Qi and the local doubling condition, the third from estimate (4.6) with q=1 and p=n+s. Note that the quantity before the gradient's norm is 1/(n+s)'(9Qi+1).
Inserting this estimate in (4.10) and applying the Hölder inequality for sums with the exponent n+s followed by the global balance condition deduce:
,
Inserting this into (4.9) we get
,
where the last inequality follows by assumption (4.7) and the second to last is valid when t>(C0/ )1/(n+s)'. Hence also the bad terms have been controlled for t bounded by max{2a1/n', 2(C0/ )1/(n+s)') where "a"(from lemma 4.2(c) depends only on n and C0 (from (4.6) through some intermediate steps) only on n and s. Hence the Orlicz norm has a finite bound, which is what we needed to show since we assumed ||--u||=1.
Note that in the proof of this theorem we separated the estimation of "good" and "bad" terms by means of the triangle inequality. It is far from clear that nothing is lost in this approximation. Of course the whole proof revolves around this estimate, in that we basically assume our measures to be locally equivalent to the Lebesgue measure, use the old results for this case and bound the non-local difference by means of a chain. The sharpness properties of this method of proof is wanting of further investiagtion.

Recall that r:={x s< | (x)<r}, the interior boundary of thickness r of .
Lemma 4.3 Let be QHBC(with constant c ) and sDC1( ). If C1>C(c ,n) then there exist C2, >0 such that
.
Proof: [h].

Lemma 4.4 If is QHBC then any finite (i.e. ( )< ) sDC1( ) satisfies the sub-summability condition (4.7) of theorem 3.
Proof: Assume, without loss of generality, that diam( )=1 and ( )=1 and define Li:= 2-i+1\ 2-i. By definition, Q 2i if Q has center zQ in Li and moreover the Q is contained in 2-i+2. The number of such Whitney cubes is bounded by 2in since ( )=1 and hence by the Hölder inequality for sums with exponent (1 ) we have
(4.11) ,
where we have used Lemma 4.3 to bound the second term for the second inequality. Hence, for any satisfying 0< < /( + ), we derive the sub-summability condition by summing (4.11) over i.

Corollary 1 Let satisfy the QHBC and C0-slice condition. Further let w sA1( ) interDC0( ) and v sRH ( ) interDC1( ) for C1>c(C ). Then ( ,w,v) ss-T if and only if (v,w) is globally balanced and w is bounded away from zero when s=0.
Proof: Follows from Theorems 2 and 3, proposition 1 and Lemma 4.4.

5. Sharpness results


We no longer implicitly assume the measures to be locally doubling, however, still denotes a bounded domain in Euclidian n-space.
In trying to prove sharpness results of the imbeddings established in chapter 4, it important to realize that some of those results are not sharp at all! The easiest way to see this is to consider why we started investigating Trudinger type inequlities in the first place, viz. because of the gap between L and Lp for a finite p. However in chapter 4 no precausions are taken to ensure that the L norm is infinite, and in fact for some measures it might not be.
Owing to theorem 1, we may conclude that if is locally doubling and is not too complicated (in particular it might be QHBC) then the Trudinger inequality implies the local balance condition which implies that for every >0, Qn+s+ / (Q) lim0 as Q approaches the boundary. Therefore some growth assumtion on the mearsures seems appropriate, although the assumptions contained in what follows are quite a bit more specific than those of the positive results of the previous section. Another obvious difference to the previous theorems is that in proving sharpness resluts, we can restrict our attention to a neighbourhood of one arbitrary boundary point, since if an inequality is not valid there it can impossibly be valid for the whole domain.

Proposition 2 (sharpness) Let R>0, z be a fixed boundary point and {xi} be an sequence in satisfying:
(a) | xi-z| <2 (xi)=:4ri,
(b) (2jBi) (2jri)n+s, for all j 0, where Bi:=B(xi,ri) and
(c) (Bi)>riR.
Then s in the Trudinger inequality is sharp, i.e. (2.1) becomes false if we replace s by any satisfying s .
Note: Condition (b) is equivalent to (2iB) 1 for every i 0. Note that (b) constrains the boundary behavior of at z, whereas (c) is more like a local condition, never actually reaching the boundary.
Proof: Assume x0 is in the center cube Q0 and (x0)=1. Further assume ri<1/6. Fix m>0 and denote r:=rm, B:=Bm and x:=xm. Let M be the smallest integer such that 2M+2 includes x0. From this definition and (a) it follows that
.
Hence as (x) lim0, so we may assume that this ratio is between 1/2 and 2.
Set Ai:=(2iB)\(2i-1B) for every i M. Define a radial function u(y):=f(|x-y|), linear on each Ai, zero outside 2MB, constant on B and continuous. Moreover fix the slopes so that f(2i-1)-f(2i)=M-1/(n+s). Hence |--u|=21-i r-1 M-1/(n+s) for points in Ai and

because Ai is contained in 2iB by assumption (b). Summing over i we conclude that ||--u||n+s is bounded by one.
B0 lies completely outside 2MB, because if they intersected, 2M+1 would contain B0 contrary to definition. Hence u(x)=0 on B0 and u(x)=M1 1/(n+s)= M1/(n+s)' on B. Thus
,
where Q0 is contained in B0. Fixing t>0 greater than the psi-Luxemburg-norm of u-uQ0, , we derive, assuming a psi-Trudinger inequality can be applied (which it of course can, after the usual smoothening argument) :
(5.1) ,
provided C0>t(2R+1)ln(2). The constant C0 is the reciprocal of the c in the definition of , above (lemma 2.1), and may hence be chosen arbitrarily. For points xi converging to z, M and r lim0, contradicting (5.1) and thus showing that fs is sharp (if it's applicable, in the first place).

Theorem 4 (a necessary condition) Let satisfy a c0-weak slice property with center x0. Suppose that (B(x,t)) tn+s and (Q) QR for every x and Q sW( ) and R>0, t 0. If ( , , ) satisfies an s-Trudinger inequality then is QHBC.
Note: The condition on can again be succinctly stated using : for every t>0 and every ball B, (tB)>1.
Proof: As usual, we need only consider the QHBC condition for points far from x0 in the quasi-hyperbolic metric, so we assume that mx 2. We will denote the fixed mx by m and further assume that c0>2. Akin to the proof of theorem 2, we define
,
where the infimum is taken over all rectifiable curves through x0 and y. Using the same intermediate steps as in the proof of theorem 2 we have, by the condition on :
(5.2) ,
Condition (d) of the definition of the weak slice property implies ui(x)=0 for every x in B0 and condition (b) implies ui(x) m 1/(n+s) for x in B (B0 and B are defined in section 3.1.3, above). Define u:=Sui. It follows from (5.2) that and u(x) m(n+s 1)/(n+s) for x belongsB. Hence, using the s-Trudinger inequality (after the usual smoothening argument) we conclude:
,
for some bounded t. Solving for t, we derive
,
and so, by condition (c) of the weak-slice property,
(5.3) .
Recalling that B is defined in terms of its centers distance to the boundary of (it is a Whitney type object), we conclude by that (B) R(x), where x is a point in B, by the assumption on . Then (5.3) clearly implies the QHBC condition.

Corollary 2 is QHBC iff it has a weak slice property and ( , t , s) ss-T.
Proof: If is QHBC, lemma 3.2 implies that it has a weak slice property. From the inequality, where we first estimate (Q) 1 and then use the definition of QHBC, formula (2.6):
(5.6)
we deduce that ( t, s) is globally balanced since the constant c1 depends on the arbitrary constant in the balance condition and can hence be made smaller than t, so that the right hand side of (5.6) dominates n+t(x). Also t satisfies the sub-summability condition (4.7) by lemma 4.4. Hence the corollary follows by theorems 3 and 4.

Let us define measures , absolutely continuous with respect to the Lebesgue measure satisfying
(5.5a) (Q) g( Q) Qn+s and
(5.5b) (Q) f( Q)
on the unit sphere at the vicinity of some boundary point. The sense of (5.5) is of course to be able to control the behavior of the balance condition directly, since (Q) g( Q)-1/(n+s-1). To see that the conditions (5.5) can be satisfied consider
(5.6) ,
where z is a boundary-point and f and g are functions belonging to D(0, ):
(5.7) .
Then if {Qi} is a chain of Whitney cubes converging to z, all but a finite number have the desired property. With the help of these functions we derive the following

Proposition 3 (sharpness) Let be the unit sphere and z a boundary point. For the measures in (5.6) define ai:=f(2-i) and bi:=g(2-i). Assume: (i) , (ii) and (iii) where c0>1 and
.
Then ( , , ) does not support an s-Trudinger inequality .
Note: Because of (5.5b) i is the sum in the global balance condition for the chain consisting of the i first cubes on a path from the center to the boundary point z. Assumption (i) tells us that does not satisfy the sub-summability condition (4.7) even for this chain. Hence (ii) is like the global balance condition for this chain, except that the inequality is reversed. Since (i) and (ii) imply that i with i, condition (iii) is merely a technical assumption concerning the speed of divergence.
Proof: Fix an integer M>1 and define and
.
For i M, define , where , as usual, the infimum is over all rectifiable curves in passing through y and the origin (=center of ). Continuing in the usual fashion we define u:=Sui and deduce ||--ui||n+s ci and ||--u||n+s 1. Hence by considering only regions Sj for 1 j i we deduce, since the width of Sj is at least 2-j,
(5.8)
for every y belongsTi. By condition (iii) for i-1>M/2 i-1>c M with c<1. Hence (5.8) implies u(y)>c 1-1/(n+s)(i-1)=c 1/(n+s)'(i-1) with c>1. Hence
,
where the last inequality follows from assumption (ii). As {ai} if l1 but not l p for any p, 0<p<1, we conclude that the left hand side is not bounded, an so, after the usual smoothening argument, we conclude that ( , , ) does not support a s-Trudinger inequality.

Example 5.1  There exists , satisfying the conditions of proposition 2 and further all the conditions of theorem 3 except the sub-summablility condition (4.7):



(5.9) .
Proof: Clearly (5.7) implies that and are both strongly doubling and Muckenhoupt and Reverse Hölder respectively. As (Q) is not sub-summable even over the single chain of cubes converging to z. As Q 2-i if Q intersects Si, (Q) g( Q)-1/(n+s-1)=log(3 Q-1) i for this Q. Moreover each Si contains only a bounded number of cubes intersecting this chain, so we have the following inequality:
(5.10) ,
where r is the distance of the final cube from the boundary; r 2-i for cubes in Si (see the picture on the following page). The second inequality follows from Euler's formula (the one defining 0.58...). From (5.9) we see that (Q) i-1log-2(i) for a cube intersecting Si. Hence by choosing c0<1/c1 (c0 is the constant in the definition of the balance condition, and may hence be chosen freely) in (5.10), we arrive at the global balance condition for cubes along the chain.
If s>0 the function g(t)tn+s has one minimum in the range [0,2], at 0. Thus we see that (Q1)>c(s) (Q2) when Q1 is the cube on the chain and Q2 is any other cube with Q1 Q2 and similarly (Q1)>c(s) (Q2). Hence the inequlity anlong the chain implies the global balance condition in the case s>0 for any chain.
If s=0, we fix an arbitrary point on the boundary, z'. We divide a chain of Whitney cubes converging to z' into two parts, one (which might be empty) in which |x-z| (x) and another in which |x-z|< (x). By the argument above the first part of the chain satisfies the global balance condition. However on the second part |x-z| |z'-z|, hence bounded from below, and so the global balance condition is trivially satisfied.

6. Conclusions


After a couple of theorems that were kept as general as possible, chapter 4 culminated in corollary 1, which states the tells us that the s-Trudinger inequlity is equivalent to the measures being globally balanced. To derive this reslut, however, the single, relatively weak, conditions from the preceeding theorems and lemmas were superimposed so that corrollary 1 in fact makes use of all the restrictions introduced in chapter 3.
One way to avoid this accumulation of constraints would be to use a more similar set throughout the chapter. In particular the approch taken here needs to assume that the measures are doubling in order to necessity of the geometrical conditions, whereas the A1 and RH classes are required for the sufficiency. Note that the slice-condition (or something similar) has to be assumed even with the Lebesgue measure to have the geometrical condition imply the inequlity [f].
Also, as already noted, the proof of theorem 3 involves an approximating technique that is not intrinsically sharp. It might advantageously be investigated on which domains this estimate is sharp, even for simple measures.
In chapter 5 it was shown that if the measures are sufficiently regular near a single boudary point, the the Trudinger inequlity is sharp (if it is satisfied). Furthermore, under similar conditions on the measures, it was shown that for a domain satisfying a weak slice property the inequlity implies a QHBC condition. Hence we derived corollary 2, which is an improvement of previous results [f] even when the measures involved are Lebesgue measures. Finally it was shown by example that the sub-summability condition (4.6) in theorem 3 is not superfluous.
It should be noted that the sharpness resluts of chapter 5 are more restrictive by far than the positive resluts of chapter 4; in chapter 5 it is necessary to assume that the measures approximate the "canonical" measures discussed in section 3.3. Hence also corollary 2 is a theorem only for the one dimensional subspace d = s(x)dm of the measure space.
Thus it is seen that there is a large discrepency between what can be proven and what is known to be sharp. As was mentioned in the introduction to chapter 5, it is vital to consider where Hölder(and other) type imbedings take over. This phase of the considerations where not indulged in at all, although they were sure performed implicitly.
As was promised in the introduction, it has now been indicated that there are still questions to settle also in the Euclidean setting. In particular it would be interesting to derive more necessary conditions for a Trudinger type inequlity, so far only the local balance condition was derived. On the other hand, the local balance condition suffice in a single proof.