A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE
C HRISTIAN B ERG
Moment problems and polynomial approximation
Annales de la faculté des sciences de Toulouse 6
esérie, tome S5 (1996), p. 9-32
<http://www.numdam.org/item?id=AFST_1996_6_S5__9_0>
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- 9-
Moment problems
and polynomial approximation
CHRISTIAN
BERG(1)
Annales de la Faculté des Sciences de Toulouse n° spécial Stieltjes, 1996
1. Historical introduction
In
Stieltjes
famous 1894-memoir[38,
n°24]
he writes:Nous
appellerons problème
des moments leproblème
suivant :trouver une distribution de masse
positive
sur une droite(0,oo),
lesmoments d’ordre k
(k
= 0.1, ...)
étant donnés.If
{ck}
denote thesenumbers,
theproblem
consists infinding
apositive
measure p on
[0, ~[
such thatand for
Stieltjes,
apositive
measure isgiven by
anincreasing function, (cf. [38,
n°37]):
Le
problème
des moments que nous avonsposé
au n° 24 nousconduira à considérer une distribution de masse
quelconque
sur unedroite Ox. Une telle distribution sera
parfaitement
déterminée si l’on sait calculer la masse totalerépandue
sur lesegment
Ox. Ce sera évidemment une fonction croissante de x, etreciproquement,
étantdonnée une fonction croissante de x, on pourra
toujours imaginer qu’elle représente,
de la manièreindiquée,
une distribution de masse.(1) Matematisk Institut, Universitetsparken 5, DIi-2100 Copenhagen
(Denmark)
Then he defines the
integral
of a continuous function withrespect
to anincreasing
function2013theStieltjes integral.
In
present day terminology Stieltjes
gave thefollowing characterization
of moment sequences.THEOREM 1.1.2013 A real sequence
{ck}
has theform
for
apositive
measure p withinfinite support if
andonly if
He came to the
problem
via astudy
of continued fractions of the form(1.1) below,
as we can see in the letter 325 of theHermite-Stieltjes correspondence,
cf.[3] :
325.-STIELTJES A HERMITE
Toulouse, 30 janvier
1892.CHER
WONSIEL1R,
Je suis
[...].
Maisjustement,
cesjours-ci, j’ai
fait sur cettethéorie des fractions continues une remarque extrêmement
simple
et
dont j’ose
vous entretenir. Soitune fraction continue où
sont des nombres réels et
positifs
- 11 -
Si x est réel et
positif,
il est clair que les réduites d’ordrepair
tendent,
pour n = oo, vers une limite déterminéeF(x).
De même les réduites d’ordreimpair
tendent,
pour n = ~, vers une limite déterminéeF1(x)
et[Du reste, d’après
un théorème deStern,
on aF1(x) - F(x)
> 0lorsque
la sérieest
convergente ; mais,
si cette série estdivergente,
on aLe théorème
général
est celui-ci :Supposons
que x ait une valeur réelle ouimaginaire quelconque,
en
exceptant
seulement les valeurs réelles etnégatives,
en sorte que lapartie négative
de l’axe des x est considérée comme une coupure.Alors on aura
toujours
et
F(x), F1(x)
sont desfonctions analytiques, uniformes
et sanspoints singuliers
dans le domaine considéré.Je
possède depuis longtemps
la démonstration de cethéorème,
maiselle est très
difficile ; [...]
In the same letter he realizes that a moment
problem
can have severasolutions
(if
F andF,
above aredifferent).
He says:L’existence de ces fonctions
~(u) qui,
sans êtrenulles,
sont tellesque
me
paraît
trèsremarquable.
Nine months
later,
in the letters 349 and 351separated by
fivedays,
hegives
more details about the convergence of the continued fraction in the two cases: The indeterminate or determinate casedepending
on whether§£ an
isconvergent
ordivergent:
351.-STIELTJES A HERMITE
Toulouse,
25 octobre 1892.CHER
MONSIEUR,
[...]
Je me suisproposé
d’élucidercomplètement
la nature decette fraction continue
(1.1)
dans le cas où les ai sont des nombres réelspositifs.
Deux cas sont à
distinguer,
selon que la série£ an
est conver-gente
oudivergente.
Lepremier
cas est debeaucoup
leplus
facileà traiter
et,
dans ma lettre[(349)], j’ai
donnédéjà
le résultat es-sentiel ;
il y a deux limitesoù les p, q, pi, q1 sont des fonctions
holomorphes
Dans le second cas, où la série
03A3
an estdivergente,
le résultat est aussisimple, mais,
pour l’énoncer dans toute sasimplicité,
il faut d’abordquelques préliminaires,
il est nécessaired’élargir
un peu la notion del’intégrale
définie. En me réservantd’y
revenir dans une autrelettre, je
me contenterai de dire que la fraction continue est
convergente (il n’y
-13-
a pas lieu de
distinguer
les réduites d’ordrepair
etimpair)
dans tout leplan, excepté
lapartie négative
de l’axe réel. C’estlà,
engénéral,
uneligne singulière,
et il estimpossible
de continuer la fonctionanalytique
en franchissant cette
ligne.
Mais cequi
est surtoutremarquable
c’estla forme
analytique
sous formed’intégrale
définiequ’on peut
donner à cette fonction et dontje parlerai plus
loin.[...]
ive see here the birth of the
Stieltjes integral.
Threedays
earlier Hermite had answered the letter 349 full of admiration:350.-HERMITE A STIELTJES
Paris,
22 octobre 1892.MON CHER
AMI,
Vous êtes un merveilleux
géomètre,
les recherches nouvellessur les fractions continues
algébriques
que vous mecommuniquez
sont un modèle d’invention et
d’élégance;
ni Gauss, ni Jacobine m’ont
jamais
causéplus
deplaisir,
etje
vous envoie mesvives
félicitations,
en vous demandant sije
doispublier,
dans lesComptes rendus,
lapartie mathématique
de votre lettre.[...]
All these results were
fully developped
in the final memoir[38],
whereStieltjes
gave severalexamples
of indeterminate measuresincluding
thefollowing:
Since
all densities
d03BB(t) on [0 , ~ [ given by
have the same moments
Once the moment
problem for 0 , ~[
was formulated and solvedby
Stieltjes,
it was natural to look for ageneralization
to the whole real line.The
breakthrough
came in along
paper[24]
from 1920-21by Hamburger,
who
proved:
THEOREM 1.2. - Given
{ck},
then there exists apositive
measure J-l on R withinfinite support
such thatif
andonly if
In
[33],
M. Rieszproved
the same resultusing
atechnique
whicheventually
was called Hahn-Banach’s Theorem. Hepoints
out that(1.2) implies
that the functionalon the
polynomials
ispositive
in thefollowing
sense:Riesz makes an extension of L to a
positive
linear functional L defined on aspace
containing
the indicator functions forhalf-lines ]-~, 03BE],
and in this way he constructs the distribution function of the measure p to be found.Riesz says in a footnote to
[33]:
J’ai
indiqué
cette démonstration dans une conférence faite à la SociétéMathématique
de Stockholm en avril 1918.The method of Riesz
concerning
extensions ofpositive
linear functionalson the space of
polynomials
was taken upby Choquet [22]
in an abstractsetting
calledadapted
spaces. The method wassuccesfully applied
to thek-dimensional moment
problem
in work of Cassier[19]
andSchmüdgen [36].
R. Nevanlinna
[31]
gave in 1922 anotherproof
of Theorem 1.2using
function
theory.
For further details about the historical
development
of the momentproblem
seeKjeldsen [28].
- 15-
2. The Nevanlinna
parametrization
Let
M*(R)
denote the set ofpositive
measures on R with momentsof any
order and infinite
support. For p
eM*(R)
let(Pn)
be thecorresponding
orthonormal
polynomials
determinedby
In
[24] Hamburger proved:
(a) If p
isdeterminate, meaning that y
is theonly
measure inM*(R’
with the same moments as M, then
03A3~n=0|Pn(z)|2 =
oofor al.
z ~ C B
R and all z e Rexcept
the at mostcountably
manypoints z
where
03BC({z})
> 0, in the case of which(b) If 03BC
isindeterminate, meaning
that there are several measures inM*(R)
with the same moments as Il, then03A3~n=0|Pn(z)|2
~ forall z E CC.
If 03BC
is indeterminate we let V= V03BC
denote the set of all v EM*(R)
suchthat
Clearly
V is a convex set, and it can beproved
to becompact
in the weakIo p ology,
characterizedby
J-ln -+ J1weakly
if andonly if f d03BCn ~ f dJ-l
for all functions
f
EC0(R),
the continuous functions,f :
R - Cvanishing
at
infinity.
The set V was
parametrized by
Nevanlinna in[31].
Theparameter
spaceis the
one-point compactification P
U{~}
of the set P of Pickfunctions,
i.e. the set of
holomorphic functions : CC B
R - Csatisfying
Using
thepolynomials (Qn)
of the second kindit is known in the indeterminate case that the series
03A3|Pn(z)|2
and03A3|Qn(z)|2
convergeuniformly
oncompact
subsets of C. Therefore the sériesdétermine entire
functions,
andthey satisfy
The JvT evanlinna
parametrization
is thehomeomorphism ~ ~
Vc.p ofP ~ {~}
onto Vgiven by
The
special
solutionsvt, t
eR~{00} corresponding to ~ ~ P~(~) being
a real constant
(or oo)
are called Nevanlinna extremal(short: N-extrerrtal).
The N-extremal solutions form a closed curve in 1,’. Since the
right-hand
side of
(2.1)
ismeromorphic
in this case,they
are discrete measures of theform
(withAoo
=Iz e C 1 B(z) = 0}).
- 17 -
The N-extremal solutions were characterized
by
M. Riesz in 1923.THEOREM 2.1
([34]).
- Let J-l EM*(R).
(a) If
J-l is indeterminate and v EV03BC,
thenC[t]
is dense inL2(v) if
andonly if
v is N-extremal.(b) If
J-l isdeterminate,
thenC[t]
is dense inL2(03BC).
If )0
E P U{~}
is a rationalfunction of degree
n, then 03BD~ is called canonicalof
order n or n-canonical.If ~
=p/q,
where p, q arepolynomials
without common zeros, then
is
again meromorphic, showing
that 1/r.p is discrete withmasspoints
at thezeros of
Bp - Dq,
the massesbeing given by
thecorresponding
residues.The 0-canonical solutions
together
with 03BD~ are the same as the N-extremal solutions.It is well-known that 1/ E V is n-canonical if and
only
if the measure(1 + x2)-n d03BD(x)
isN-extremal,
cf.[1,
p.121].
Another characterization of n-canonical measures isgiven
in thefollowing
result ofCassier,
whichgeneralizes
the Theorem of Riesz.THEOREM 2.2
([18], [17]).
A solution 1/ E V to an indeterminate momentproblem is
n-canonicalif
andonly if
the closurtC[t] of
thepolynomials in L2(03BD) is of
co-dimension n.Theorem 2.1 is the earliest result in the class
of problems
we shall discuss:Let 03BC E
M*(R)
and1 ~ 03B1
~. Characterizethe 03BC
and 03B1for
whichC[t] is
dense inL03B1(03BC).
This can
equally
well be studied inRk.
3.
Polynomial approximation
In
Rk
we consider the setM*(Rk)
ofpositive
measures 03BC onRk
for whichwhere
C[x] = C[x1, ..., zk denotes
the set ofpolynomials
in k variables.Let y
EM*(Rk)
and 1~
a oo begiven.
Our main concern is ifC[x]
isdense in
L03B1(03BC).
By
HBlder’sinequality
so there exists a critical
exponent
p =03C1(03BC) ~ [1, ~]
such thatAs in section 2 we consider the set
11tL
of measures v EM*(Rk)
such thatWe say that J-l is determinate if
V03BC
=tpl,
otherwise J-l isindeterminate,
inthe case of which
Vtt
is aweakly compact
convex set of measures.We recall the
following
result of Naimark from 1947:THEOREM 3.1
([30])
(i) If
J-l isdeterminate,
thenC[x]
is dense inL1(03BC).
(ii) If
J-l is indeterminate and v EV03BC,
thenC[x]
is dense inL1 (v) if
andonly if
v is an extremepoint of 1/tt.
Proof . (Gelfand) If C[x]
is not dense inL1(03BC)
there existsf
EL~(03BC)
such that
f 1:-
0 andvVe may assume
,f
real-valuedand -1 ~ f ~ 1.
Thenwith
03BC+ ~
p-. This shows that p is not an extremepoint of V03BC.
Conversely, if p = (1/2) (J-l1
+p2)
with03BC1, 03BC2 ~ V03BC being different,
thensince
03BCj ~ 2p
we have03BCj
=2fj(x) dp(x)
with0 fj ~ 1,
and henceThis shows that
C[x]
is not dense inLI (p).
0- 19-
THEOREM
3.2.- If
J-l EM*(Rk)
isindeterminate,
then the criticalexponent 03C1(03BC) ~
2.Theorem 3.2 was
proved
in[8]
for k = 1using
thereproducing
kernel03A3Pn(x)Pn(y)
for an indeterminate momentproblem.
Theproof
in[23]
isfor
any k
and uses thetheory
ofoperators
in Hilbert space.THEOREM 3.3. For
J-l E M*(Rk)
letIf 03A3 1/ 2B1 À2n =
oo, thenp(J1)
= oo.For k = 1 the infinite series condition is the Carleman condition which is sufficient for
determinacy.
For aproof
in this case see[9].
Theorem 3.3 can be deduced from the case k = 1
using
resultsrelating
moment
problems
in one and several dimensions.Let 7rj : :
mk -
R denote theprojection 03C0j(x1,
...,xk)
= Xj, and for03BC ~ M*(Rk)
let03C0j(03BC)
denote thej’th marginal
distributionof p given by
xj(p)(B) = 03BC(03C0-1j(B))
for Borel sets B~ R.
THEOREM 3.4
([32]).2013 Let 03BC
EM*(Rk).
(i) If C[t] is
dense inL03B1(03C0j(03BC)), j
=1, ..., k for
som e cx > 1, th enC[x]
is dense inL03B2(03BC) for
103B2
a.(ii) If 03C01(03BC),
...,03C0k(03BC)
are determinate. then J-l is determinate.Remarks
(a)
It is easy to establish(ii)
once(i)
has beenproved.
The idea is to prove that any v~ V03BC
is an extremepoint
ofl- .
If this is so thennecessarily V03BC
={03BC}.
For vE Vt1
it is clear that7r j (J-l)
andxj(v)
have the samemoments so
by
theassumption
in(ii)
we havexj(p)
=03C0j(v). By
theTheorem 2.1 of Riesz
C[t]
is dense inL2(03C0j(v)) for j
=1, ..., k
and hence03C1(v) ~ 2 by (i). By
Theorem 3.1 weget
that v is an extremepoint of V03BC.
(b)
There exist determinaten1easures J-l E M*(Rk)
for which03C01(03BC),
...,xk( p)
areindeterminate,
cf.[32].
One can even obtain this for rotation invariant measures y, cf.[7].
If p
EM*(R)
is determinate we have03C1(03BC) ~
2by
the Theorem 2.1 of Riesz.THEOREM 3.5.2013 There exist determinate measures as well as indeter- minate measures 03BC E
M*(R)
with03C1(03BC)
= 2.For the
proof
of this result we needLEMMA
3.6. 2013 Let 03BC
EM*(R)
and xi ... zn, 03B11 >0,
..., an > 0 begiven
anddefine
Then
p(u)
=p(p).
Proof.
- Since 03C3 ~ J1 we have03C1(03BC)
>p(u).
Suppose
next thatC(x)
is non-dense inL’(o-)
for some a > 1. ’iVe shov thatC[x]
is non-dense inL03B1’(03BC)
for all03B1’
> a and therefore03C1(03BC) ~ p( u).
If
1/03B1 + 1/03B2 = 1
there existsf
EL03B2(03C3) B {0}
such thatLet
po(x)
=03A0ni=1 (x - Xi)
andput g(x)
=f (x)po (x).
For any 103B2’ ,C
we
have 9 E L(3’ (p) by
Hbldersinequality
because1’ urthermore
showing
thatC[x]
is non-dense inLÙ’(J-l),
where1/03B1’
+1/03B2’
= 1, i. e. forany 03B1’ > 03B1. ~
-21-
Let us start with an indeterminate and lV-extremal measure p and let us
remove k ~
1point
massesfrom p
toget
where A
C supp(p)
has kpoints.
Then T is determinate(and
of index ofdeterminacy k - 1,
cf. sect.5).
If we instead add k new masses to ii, weget
where al, ..., ak are different
points of RBsupp(03BC).
Then o- is indeterminate andk-canonical,
cf.[18], [17].
By
the Lemma 3.6since
03C1() ~
2by
Theorem 2.1 and03C1(03C3) ~
2by
Theorem 3.2.The denseness of
C[t]
inL"(p)
isgoverned by
a functionAI,
introduced in connection with the Bernsteinproblem
ofweighted approximation,
cf.[29].
This function is called theHall-Mergelyan majorant.
LEMMA 3.7. - Let p E
À4*(ùÉ)
and1 ~
a oo anddefine
Then
te[t]
is dense inL03B1(03BC) if
andonly if
there exists zo~ C B supp(p)
such that
M03B1(z0)
= oc. In theaffirmative
caseM,,,(z)
= ocfor
allz
~ C B supp(p).
Proof.
- Assume first thatM03B1(z0)
oc for some zo~ C B supp (p) -
Ifwe define the new measure
and let
Il
.Il.
denote the norm inL03B1(03BC03B1),
we havIso
by
the Hahn-Banach Theorem thereexists g
EL03B2(03BC03B1),
where a andfi
are dual
exponents,
such thatIf this is
applied
topolynomials vanishing
at zo, we find for p eC[t]
and since
g(t)(t - z0)/(1
+|t|)03B1 ~ L03B2(03BC),
we see thatC[t]
is not dense inL03B1(03BC).
Assume next that
C[t]
is not dense inL03B1(03BC). Again by
the Hahn-Banach Theorem thereexists g ~ L03B2(03BC) B {0}
such thatlue Gauchy transtorm
is
holomorphic
inC B
supp(03BC)
and notidentically
zero. For zo EC B
supp(03BC)
and p e
C[t]
weget by (3.1)
so if
~(z0) ~
0 we findi.e.
with
Note that E is continuous
in {z
EC B supp(p) |~(z) ~ 0}.
- 23 -
If
cp(zo) =
0 we choose 0 rdist (z0, supp(p»
so that)O(z) =1
0 for|z - zol | = r,
andby
the maximumprinciple
weget
with 7B =
max|z-z0|=r I«z).
Theequations (3.2), (3.3)
show thatM03B1(z0) ~. ~
Using
the Lemma 3.7 Sodin[37] proved
thefollowing
THEOREM 3.8. - Let s > 1 and
define
Then
03C1(03BC)
= s.Remark. 2013
By
the above result any number A E] 1 , ~ [ is
the criticalexponent
of some nieasure p eM*(R). If p
is indeterminate and notan extreme
point
ofV,,
thenp(p)
=1,
and if the Carleman condition is fulfilled thenp(p)
= oo. Thusany À ~ [1, oo is
the criticalexponent
ofsome p e
M*(R).
This result was established in[9] for 03BB ~
2 and left open for À> 2,
cf.[4].
4. Rotation invariant measures
The natural
question
whether Theorem 2.1 of Riesz extends to dimension k > 1 was open for a number of years, cf.[23], [25,
p.529],
until it wasanswered in the
negative by Berg
and Thill in[13].
In[25]
theproblem
isascribed to the
physicist
J. Challifour(1978).
THEOREM 4.1
([13]).-
For k > 1 there exist determinate measures03BC ~ M*(Rk) for
whichC[x]
is not dense inL 2 (p).
In his survey paper
[23]
about the multidimensional momentproblem Fuglede
introduced two new notions ofdeterminacy.
The two notions wereformulated as certain conditions of
self-adjointness
of themultiplication operators Xjp
=x.,p(x)
with domainC[X1, xkl
in the Hilbert space Hequal
to the closure ofC[x]
inL2(03BC).
Fuglede
characterized these notions in terms ofapproximation properties:
(i)
p is ultradeterminate if andonly
ifC[x]
is dense inL2 ((1 + Ilx112) d03BC(x)).
(ii)
p isstrongly
determinate if andonly
ifC[x]
is dense inL2((1
+x2j)d03BC) for j
=1,
..., k.(iii) If p
isstrongly determinate,
then p is determinate andC[x]
is densein
L2(03BC).
The condition of
ultradeterminacy clearly implies strong determinacy.
Schmüdgen [35]
found anexample
of astrongly
determinate measure which is not ultradeterminate and anexample
of a determinate measure which is notstrongly
determinate.The latter also follows from Theorem
4.1,
which is based on astudy
ofrotation invariant measures in
Rk.
There is a
bijection
between rotation invariant measures M onRk
andmeasures o-
on 0 , oo [ established
as u =u5(p),
theimage
measure of punder e Rk ~ [0, oo[
definedby e(x)
=~x~2,
i.e.If j : [0, ~ [
xSk-1 ~ ntk
isgiven by j(t, 03BE) = t03BE, then
J-l =j(03C3 ~ 03C9),
where w is normalized surface measure on the unit
sphere Sk-1.
ThE momentsof y
determine the moments of o- and vice versa:which is zero unless all
n j
are even.For cr E
M*([0, ~[) (i.e. o-
EM*(R)
issupported by [0, ~[)
thereare two notions of
determinacy
to bedistinguished: Determinacy
in thesense of
Stieltjes (det(S)) meaning
that there isonly
one measure on[0, oo[
with the same moments as 03C3, and
(ordinary) determinacy (or determinacy
in the sense of
Hamburger, det(H)), meaning
that there isonly
one measureon R with the same moments as u.
It should be
emphasized
that there exist measures a eM*([0, ~[)
which are
det(S)
butindet(H),
i.e. in the infinite convex setV03C3
the measure- 25 -
u is the
only
onesupported by 0 , 00 [.
This measure o- isnecessarily
03C3 = v0, the N-extremal measure
corresponding
to theparameter
~ 0 in the Nevanlinnaparametrization,
cf.[14], [21].
The paper
[13]
contains twokey
resultsrelating p
EM*rot(Rk)
and thecorresponding 03C3 ~ M*([0, ~[)
such that(4.1)
holds.THEOREM 4.2.
Given p ~ M*rot(Rk), k ~
1.Th e n is
determinateif and only if u is det(S).
THEOREM 4.3.2013 Given J.l
~ M*rot(Rk), k
> 1. ThenC[x1, Xkl
isdense in
L2(03BC) if
andonly if c[t]
is dense inL2(tp d03C3(t)) for
p= 0, 1,
...Remarks
(i)
Theorem 4.3requires k
> 1. For k = 1 thecorresponding
assertion is(relating
asymmetric
measure M and u =03C8(03BC)
where03C8(x) = x2) : C[x]
isdense in
L2(03BC)
if andonly
ifC[t]
is dense inL2(03C3)
and inL2(t do-(t» .
(ii)
Theorem 4.3 ispart
of thefollowing general
result[13] about M
EM*(Rk)
notneccessarily
rotation invariant and o-03C8(03BC):
Let1 ~
a oo.If
C[t]
is dense inL03B1(t(1/2)d03B1 d03C3(t))
for d =0, 1,
..., thenC[x]
is dense inL03B1(03BC).
As a consequence of this result weget
thefollowing
relation between the criticalexponents of p
and cr.COROLLARY 4.4.2013
Let ~ M*(Rk)
and u =03C8(03BC). If
103C1(03C3)
then03C1(03C3) ~ 03C1(03BC).
Proof.
- Assume thatC[t]
is dense inL03B1(03C3),
where 1 03B1 00. Itsuffices to prove that
C[t]
is dense inL03B1’(t(1/2)d03B1’d03C3(t))
for d =0, 1,
...and 1
a’
a. For p eC[t]
andf
ECc([0, ~[)
we findby
H61der’sinequality
where s is the dual
exponent
of03B1/03B1’.
The first factor can be made as smallas we
please by assumption.
0Combining
Theorems 4.2 and 4.3 weget
thefollowing
result.THEOREM 4.5.
Let 03BC
EM*rot(Rk), k
> 1 withcorresponding
u EM*([0, ~[).
Then 03BC is determinate andC[x] is
not dense inL2(03BC) if
and
only if u is det(S)
and thereexists p ~ N
such thatC[t] is
not dense inL2 (tP du(t)).
fihe measures a in the theorem above are
necessarily
obtained from someN -extren1al measure r E
M*([0 , ~[) by removing
a finite number of itsmasses
(cf.
sect.5).
Inparticular 03BC
has the formwhere wr is the normalized uniform distribution on the
sphere /1 x Il
= r.COROLLARY 4.6.2013
If J1
EM*rot(Rk) is
determinate andabsolutely continuous,
thenC[x]
is dense inL2(03BC).
Example.
- Let vo beindet(S)
and the N-extremal solutioncorrespond- ing
to theparameter value )0 ==
0. The measure cr = vo -v0({0}) bo
hasthe
properties (cf. [13]):
03C3 isdet(H),
andC[t]
is dense inL2(tp du(t))
forp =
0, 1,
2 but not forp ~
3. Thecorresponding
rotation invariant measurehas the
following properties (cf. [13], [7]):
(i)
p is determinate.(ii) C[x]
is dense inL03B1(03BC)
for1 ~
cx 2 but not for a = 2.(iii) dim (L 2 ~ C[x])
= oo.(iv)
Themarginal
distributions are indeterminate.An
explicit example
of a measure Po as above isgiven
in section 6.5. Measures of finite index
Inspired by
Theorem 4.5 thefollowing (Stieltjes)
index ofdeterminacy
was introduced in
[13]
for measures cr eM* ([ 0, ~[)
which aredet(S):
and the
following
result was obtained.- 27 -
THEOREM 5.1. 2013 For u E M*
([0, 00 [)
which isdet(S)
thefollowing
conditions are
equivalent : (i) i(03C3)
=0,
(ii) (j
= VO -v0({0}) 80,
where vo is the N-extremal solution withparameter
value 0corresponding
to aStieltjes
momentproblem
whichis
indet(S).
Furthermore,
the measure o- hasfinite index j ~
1if
andonly if
(j =
a 80
+t-3 d(t),
where 7 EM*([0,
oo[)
has index zero anda ~ 0.
Motivated
by
the above andpolynomials orthogonal
withrespect
to a matrix of measures,Berg
and Duran[10]
introduced thefollowing
index ofdeterminacy
for determinate measures J-l EM*(R)
and z~ C
and the
following
result wasproved:
THEOREM 5.2
(i) if
7 =ZACA
aA6A
is indeterminate andN-extremal,
andif 0
C Ahas k + 1
points,
thenfor
J-l =03A303BB~B0
a03BB6A
we have(ii) If 03BC is
determinate andindz(03BC)
ocfor
some z EC,
then p is derivedfrom
an N -extremal measure T as above andindz(03BC)
isgiven by (5.3).
Let m
eM*(R)
be determinate. We defineind(p) = k
if(5.3) holds;
otherwise
indz (p)
= oo for all z e C and weput ind(03BC)
= oo.if 0- E
M*([0 , ~[)
isdet(H)
and a fortioridet(S),
thefollowing
relationholds between the two indices of
determinacy:
where
[x]
is theintegral part
of x in case x oo and[00]
= oo.A determinate measure 03BC E
M*(R)
of finite index is discrete and can be written aswhere an > 0 and
0 ~ |03BB1| ~ |03BB2| ~
.... The canonicalproduct
7B.T
(with
1 -z/03BB1 replaced by z
if03BB1
=0)
convergesuniformly
oncompact
subsets of C to an entire function of minimalexponential type vanishing
atA =
{03BBn}
=supp(03BC),
cf.[10].
Let
(Pn )
be thecorresponding
orthonormalpolynomials.
The result ofHamburger
in section 2 can be stated that(Pn(z)) E f,2
if andonly
ifF03BC(z)
= 0. In[10]
we considered thequestion
whether(P(m)n(z))n
C£2,
and it turned out that for
ind(03BC)
>0, m ~
1 this is never the case, but forind(03BC)
= 0 it was establishedthat (P(m)n(z))n ~ ~2
if andonly
if
F(m)03BC(z)
=0,
and this holds forcountably
manypoints.
In
[11]
we consideredgeneral
discrete differentialoperators
of the formwhere k~ ~ 0, aÊ,,
eC,
and z1, ..., zN are differentcomplex
numbers. iveare interested in the
question
whether(T(Pn))
e~2,
which is of interest because this condition isequivalent
to the assertion thathas a continuous linear extension from
C[t]
toL2(03BC).
THEOREM 5.3. -
Suppose ind(J1)
00 and letF03BC
be as above. Then(T(Pn))n ~ ~2 if and only if T(zkF03BC(z)) = 0 for k = 0, 1, ..., ind(03BC).
If
Zl, ...,ZN E rc B supp(J1)
andk1,
...,kN ~
0 arefixed
buta~,j ~ C
variable then
-29-
This result can be used to realize
L2 (p)
as a Hilbert space of entirefunctions in the sense of de
Branges [16]
in caseind(03BC)
oo. For detailssee [12].
Determinate measures of finite index are in a certain sense indeterminate
measures which are canonical
of negative
order. This is to be understoodin the
following
sense:If p
is indeterminate and canonical oforder n ~ 0,
and if
0 ~ k
masses areremoved,
then the modifiedmeasure P
is canonicalof order n - k
if k ~
n. However if k > n, then the modified measurefi
isdeterminate and
ind()
= k - n - 1.The
analogy
can bepursued
further in the direction of Theorem 2.2.It turns out that for determinate measures M of finite
index k,
notonly
the
polynomials
are dense inL2(03BC),
but also a certainpolynomial
ideal ofco-dimension k + 1 in
C[x]
is dense inL2(03BC):
THEOREM 5.4
([11]).2013
Assume thatind(03BC) = k
and let R EC[x]
be apolynomial of degree
k + 1 such thatR(z) e
0for
z Esupp(p).
Then theideal RC[x] is
dense inL2(03BC).
6.
Examples
Let 0 q 1 be fixed. We define
and shall also use the short notation
Let
where
is the Gauss binomial coefficient.
Al-Salam and Carlitz
[2]
noticed thatis a
Stieltjes
moment sequence for 0 a and found a measure with these momentsThese measures were considered further
by
Chihara([20], [21]),
whoproved
that the momentproblem
is indeterminate as aHamburger
momentproblem
for q a1/q
and otherwise determinate. Furthermorem(a)
is the N-extrenial measurecorresponding
to theparameter
value i = 0 whenq a
1/q.
Ismail[26]
found theright
normalization of the measuresm (a)
and
0’( a).
For a self-contained treatment of this momentproblem
we refer tothe paper
[15] by Berg
and Valent. It also contains anexplicit
determination of the functionsA, B, C,
D in the indeterminate case. In addition it is shown that Carleman’s series03A3 1/
2ns2n(a)
converges for 0 a, 0 q 1.(This
is a concreteexample demonstrating
that Carleman’s condition is not necessary fordeterminacy.)
For further
examples
of N-extremal measures see[15]
and[27].
References
[1] AKHIEZER (N. I.) . 2014
The classical moment problem, Oliver and Boyd, Edinburgh1965.
[2]
AL-SALAM (W.A.) and CARLITZ (L.) . 2014 Some orthogonal q-polynomials. Math.Nachr., 30 (1965), pp. 47-61.
[3]
BAILLAUD (B.) and BOURGET(H.) .
2014 Correspondance d’Hermite et de Stieltjes I, II, Gauthier-Villars, Paris 1905.[4]
BERG(C.) .
2014 Critical exponents for measures. in: Open problems, ed. W. Van Assche, J. Comput. Appl. Math., 48(1993),
p. 227.[5]
BERG(C.) .
2014L2-approximation
with respect to rotation invariant measures, Suppl. Rend. Circ. Mat. Palermo. Serie II, 33 (1993). pp. 211-217.- 31 -
[6]
BERG(C.) .
2014 Indeterminate moment problems and the theory of entire functions, J. Comput. Appl. Math., 65(1995),
pp. 27-55.[7]
BERG(C.) .
2014 Recent results about moment problems, in: Probability measureson groups and related structures XI, World Scientific, Singapore 1995.
[8]
BERG(C.)
and CHRISTENSEN(J.
P.R.) .
2014 Density questions in the classical theory of moments, Ann. Inst. Fourier, 31, n° 3(1981),
pp. 99-114.[9]
BERG(C.)
and CHRISTENSEN(J.
P.R.) .
2014 Exposants critiques dans le problème des moments, C.R. Acad. Sci. Paris Série I, 296(1983),
pp. 661-663.[10]
BERG(C.)
and DURAN(A. J.) .
2014 The index of determinacy for measures and the l2-norm of orthonormal polynomials, Trans. Amer. Math. Soc., 347(1995),
pp. 2795-2811.[11]
BERG(C.)
and DURAN(A. J.) .
2014 When does a discrete differential perturbationof a sequence of orthonormal polynomials belong to l2? J. Funct. Anal., 136
(1996),
pp. 127-153.[12]
BERG(C)
and DURAN(A. J.) .
2014 Orthogonal polynomials,L2-spaces
and entirefunctions, Math. Scand.
(to appear).
[13]
BERG(C.)
and THILL(M.).2014
Rotation invariant moment problems, Acta Math.167
(1991),
pp. 207-227.[14]
BERG(C.)
and THILL(M.) .
2014 A density index for the Stieltjes moment problem,in: Orthogonal Polynomials and their Applications, ed. C. Brezinski, L. Gori and
A. Ronveaux, IMACS Annals on computing and applied mathematics, 9
(1991),
pp. 185-188.
[15]
BERG(C.)
and VALENT(G.).
2014 The Nevalinna parametrization for some inde-terminate Stieltjes moment problems associated with birth and death processes, Methods and Applications of Analysis, 1
(1994),
pp. 169-209.[16]
DE BRANGES(L.) .
2014 Hilbert spaces of entire functions, Prentice-Hall, Englewood Cliffs, N.J., 1968.[17]
BUCHWALTER(H.)
and CASSIER(G.) .
2014 Mesures canoniques dans le problème classique des moments, Ann. Inst. Fourier, 34(1984),
pp. 45-52.[18]
CASSIER(G.) .
2014 Mesures canoniques dans le problème classique des moments, C.R. Acad. Sci., 296, Série I(1984),
pp. 717-719.[19]
CASSIER(G.) .
2014 Problème des moments sur un compact de Rn et représentation de polynômes à plusieurs variables, J. Funct. Analysis, 58(1984),
pp. 254-266.[20]
CHIHARA(T. S.) .
2014 On indeterminate Hamburger moment problems, Pac. J.Math., 27
(1968),
pp. 475-484.[21]
CHIHARA(T. S.) .
2014 Indeterminate symmetric moment problems, Math. Anal.Appl., 85
(1982),
pp. 331-346.[22]
CHOQUET(G.) .
2014 Le problème des moments, Séminaire d’initiation à l’analyse(1962),
Paris.[23]
FUGLEDE(B.) .
2014 The multidimensional moment problem, Expo. Math., 1(1983),
pp. 47-65.
[24]
HAMBURGER(H.) .
2014 Über eine Erweiterung des Stieltjesschen Momentenpro- blems, Math. Ann., 81(1920),
pp. 235-319.; 82(1921),
pp. 120-164. 168-187.[25]
HAVIN(V. P.)
et al.(editors) .
2014 Linear and complex analysis problem book.199 research problems, Lecture Notes in Mathematics, 1043, Springer, Berlin - Heidelberg - New York 1984.
[26]
ISMAIL(M.
E.H.) .
2014 A queueing model and a set of orthogonal polynomials, J.Math. Anal. Appl., 108
(1985),
pp. 575-594.[27]
ISMAIL(M.
E.H.)
and MASSON(D. R.) .2014
Q-Hermite polynomials,biorthogonal
rational functions and Q-beta integrals, Trans. Amer. Math. Soc., 346
(1994),
pp. 63-116.
[28]
KJELDSEN(T. H.) .
2014 The early history of the moment problem, Historia Math.,20
(1993),
pp. 19-44.[29]
KOOSIS(P.) .
2014 The logarithmic integral I, Cambridge University Press, Cam- bridge 1988.[30]
NAIMARK(M. A.) .
2014 Extremal spectral functions of a symmetric operator, Izv.Akad. Nauk. SSSR ser. matem., 11
(1947),
pp. 327-344; Dokl. Akad. Nauk. SSSR,54
(1946),
pp. 7-9.[31]
NEVANLINNA(R.) .
2014 Asymptotische Entwicklungen beschränkter Funktionen und das Stieltjessche Momentenproblem, Ann. Acad. Scient. Fennicae,(A),
18, n° 5(1922),
pp. 1-53.[32]
PETERSEN(L. C.) .
2014 On the relation between the multidimensional momentproblem and the one-dimensional moment problem, Math. Scand., 51
(1982),
pp. 361-366.
[33]
RIESZ(M.) .
2014 Sur le problème des moment. Troisième Note, Arkiv för mate- matik, astronomi och fysik, 17, n° 16 (1923), pp. 1-52.[34]
RIESZ(M.) .
2014 Sur le problème des moments et le théorème de Parseval corres-pondant, Acta Litt. Ac. Sci. Szeged, 1
(1923),
pp. 209-225.[35]
SCHMÜDGEN(K.) .
2014 On determinacy notions for the two dimensional momentproblem, Ark. Mat., 29