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.