fur Angewandte Analysis und Stohastik
imForshungsverbund Berline.V.
Preprint ISSN 0946 { 8633
Optimal alibration of exponential Levy models
Denis Belomestny 1
andMarkus Rei 2
submitted: 21thMarh2005
1
WeierstrassInstitute
forAppliedAnalysisandSto hastis,
Mohrenstr.39,10117
Berlin,Germany
E-Mail:belomestwias-berlin.de 2
WeierstrassInstitute
forAppliedAnalysisandSto hastis,
Mohrenstr.39,10117 Berlin,Germany E-Mail: mreisswias-berlin.de No. 1017 Berlin2005
W
I
A
S
2000MathematisSubjet Classiation. 60G51;62G20;91B28.
Keywordsand phrases. Europ eanoption,jumpdiusion,minimaxrates,severelyill-p osed,nonlinearinverse
Weierstra-InstitutfurAngewandte AnalysisundSto hastik(WIAS)
Mohrenstrae39
10117Berlin
Germany
Fax: +49302044975
E-Mail: preprintwias-b erlin.de
Basedonoptionsdataatthemarkettheproblemofalibratinganexp onentialLevymo del
fortheunderlying assetisinvestigated. Itisshownthatthis statistialinverseproblemisin
general severelyill-p osedandexatminimaxratesofonvergenearederived. Theestimation
pro edure we prop ose is based on the expliit inversion of the option prie formula in the
sp etral domainand aut-oshemeforhighfrequeniesas regularisation . Itsp erformane
is illustratedbynumerialsimulations.
1 Introdution
Already shortly after the intro dution of the Blak-Sholes mo del Merton (1976) argued that
basedonempirialevideneshareprie mo delsshould inorp orateajumpomp onent. Nowadays,
standard problems of mathematialnane like derivative priing have b een suessfully solved
for manygeneral Levy mo dels, as has b eomemanifest inthe monographby Cont and Tankov
(2004a). Ontheotherhand,theinvestigationofalibrationmetho ds forLevy mo delshasmainly
fo usedonertainparametrisationsoftheunderlyingLevypro ess. Sinetheharateristitriplet
ofaLevypro essisapriorianinnite-dimensionalobjet,thisapproahisalwaysexp osedtothe
problemof missp eiation, in partiularwhen there is no inherent eonomi foundationof the
parametersand theyareonlyusedtogenerate dierentshap es ofp ossiblejumpdistributions.
Thegoalofthispap eristoinvestigatemathematiallytheproblemofnonparametriinferenefor
theLevy tripletwhentheasset prie(S
t
)followsanexp onentialLevymo del
S
t =Se
r t+Xt
withaLevypro ess X
t
fort>0: (1.1)
We supp ose that at timet=0we disp ose ofpries for vanillaEurop eanallandput optionson
this asset with dierent strike pries andp ossiblydierentmaturities. Bybasing ourestimation
on optiondata we draw inferene onthe underlying risk neutral prie pro ess, whih in general
annotb e determinedfromhistorialpriedatadue totheinompletenessoftheLevymarket.
Theobservedoptionprieswillb eslightlyunpreiseduetobid-askspreadsorotherfritionsinthe
market. Itiswellknownthat intheidealaseofpreiseobservations forallp ossiblestrike pries
thestate prie density andhene theLevy tripletanb e uniquelyidentied,see e.g. At-Sahalia
andDuarte (2003). Under therealistimo delofnitely manynoisyobservations we annothop e
to determinethetriplet orretly, we shouldrather try to providean estimatorwhih is asgo o d
asp ossible forthegivenaurayofthedata. Thisoptimalityprop ertyisusuallyassessed bythe
minimaxparadigm,whih measurestheinherentomplexityofthestatistialproblemlass. One
mainresult ofthepresentpap erisalower b ound,showingthat alreadyinthesimpleexp onential
Levymo deltheestimationproblemisingeneralseverelyill-p osed,thatis,theestimationerrorfor
anypart of the Levy tripletas afuntionof theauray of theobservations willonly onverge
withalogarithmirateforanyoneivableestimationpro edure.
Onthe otherhand,we prop ose anexpliitonstrution of anestimatorthatattains thisoptimal
minimaxrate. Thepro edureis basedontheinversionoftheexpliitpriingformulaviaFourier
transformsbyCarrandMadan(1999)andaregularisationinthesp etraldomain. UsingtheFast
FourierTransformation,thepro edureiseasytoimplementandyieldsgo o dresultsinsimulations
asnonparametripart andthedriftanddiusiono eÆientas parametriparts.
The exp onential Levy mo delreets theassumption that thelog returns of the asset evolve
in-dep endently and withidential distributionforthesametimesteps, whih is plausiblefor liquid
marketsand notto olongtimehorizons. Thisbasi mo dellass hasb eenonsidered reently for
avariety ofpriing and optimisationproblems innane. Let us mentionhere Mordeki (2002)
forpriingAmerian-typ ep erp etual options,Contand Volthkova(2005)forpriingother
path-dep endent optionsand Eb erlein andPapapantoleon(2004)forago o dsurvey andgeneralisations
tothetime-inhomogeneousase. Kallsen(2000)andEmmerandKlupp elb erg(2004)studymarket
mo delsinamultidimensionalframework.
When no mo del for the prie pro ess is sp eied, alibration from option data an b e used to
estimate the state prie density, see At-Sahaliaand Duarte (2003). This density yields the
dis-tributionoftheasset prie atthetimesofmaturity,butdo es notprovideanyinformationonthe
evolutionofthe prie intime. Astrutural assumptionontheprie pro ess allowstond pries
for path-dep endent options or to p erform a dynamirisk management. Innanial engineering
informationab out the timeevolution exp eted at the market is obtained by smo othing implied
Blak-Sholes volatilities,f. Fengler, Hardle, and Mammen(2003). For the generalised
Blak-Sholes mo delDupire'sformulap ermitsthealibrationfromoptionpries,see e.g. Jakson,Suli,
andHowison(1999)foranumerialapproahandCrep ey(2003)foratheoretialstudy. The
al-ibrationofparametriexp onentialLevymo delshasb eenstudied forexamplebyEb erlein,Keller,
andPrause (1998)andCarr,Geman,Madan,andYor(2002).
The study by Cont and Tankov (2004b), also desrib ed in Cont and Tankov (2004a),is losest
to ournonparametri approahfor exp onentialLevy mo dels. Inorderto op ewith theinvolved
ill-p osedness,these authorsemployaleastsquaresmetho dp enalizedbytherelativeentropywith
resp et toanapriorihosen Levy triplet. Thistyp eofp enalisationhasertaingenuine features:
themetho dtakesintoaountpriorinformationandtheresultingfuntionalisonvex. However,
thevalueofthediusion o eÆientis thus xedinadvane,and theregularisingeet do es not
take plaeforindep endent randomerrors intheobservations,essentially b eausewhitenoise an
only b eonsidered as anelement inaSob olevspaeofnegative regularity, f. theHilb ert sales
approah in Engl, Hanke, and Neubauer (1996). In ontrast, we strive for a metho d that has
only few tuning parameters,p ermits the alibrationof thediusion o eÆient and is suited for
observationswithrandomerrors. Themetho dwe present b elowwillhaveallthese prop ertiesand
isinadditionprovablyrate-optimaloverstandardsmo othnesslasses. Insteadofminimizingsome
data-dep endent riterion,forwhihineah steptheoptionprie fortheurrenttripletvaluehas
tob eevaluated,wepreferusingtheexpliitnonlinearinversiondiretly. ThisresultsinaneÆient
straight-forward algorithm. Combiningthis metho dwith astage-wise aggregation pro edure, a
robust data-drivenmetho disobtained.
After intro duingthe nanialand statistialmo delinSetion 2, theestimationmetho dforthe
nite intensity ase is develop ed in Setion 3. The main theoretial results are formulatedin
Setion 4. A typialinniteintensityase is treated inSetion 5and we onlude inSetion 6.
Thepro ofsoftheupp er andlowerb oundsaredeferredtoSetions7and8,resp etively, whilethe
App endixprovidessomefurthertehnialresults.
2 The model
2.1 The exponential Levy model and option pries
Wesupp osethattheprieS
t
ofanassetattimetfollowstheLevymo del(1.1),whereS>0isthe
presentvalueoftheassetandr>0istherisklessinterestrate,whihisassumedtob eknownand
variationand absolutelyontinuousjump distribution. Its harateristi funtionis givenbythe Levy-Khinthinerepresentation ' T (u):=E[exp(iuX T )℄=exp T 2 2 u 2 +iu+ Z 1 1 (e iux 1)(x)dx : (2.1)
>0isalledvolatility,2Rdriftandthenon-negativefuntion,satisfying R
(jxj^1)(x)dx<
1, isthejump density. Itsjump intensityis dened as:=kk
L 1
(R)
. Theharateristi triplet
T := ( 2
;;)hasfor nite the intuitive explanationthat X isthe sum ofthree indep endent
lassial pro esses, namelya Wiener pro ess of volatility , a deterministi linear pro ess with
trend and a omp ound Poisson pro ess of intensity with jump distribution =. Pro esses
with inniteativityare obtainedbyalimitingpro edure and theirsamplepathshave innitely
manyjumps,butwithjumpsizesaumulatingatzero. ByexludingLevypro essesofunb ounded
variationweensureanintuitiveexplanationoftheparametersandweareinlinewiththeempirial
parametrindingsofCarr,Geman,Madan,andYor(2002),thoughsomeusefulparametrimo dels
likegeneralized hyp erb olidistributionsareexluded.
A Europ ean alloptionwith maturityT and strike K foran underlying asset grants theholder
therighttobuytheasset atthefuturetimeT fortheprieK. Ariskneutralprie attimet=0
forthisoptionisgivenby
C(K ;T)=e r T E Q [(S T K) + ℄; (2.2) where (A) +
:=max(A;0) andQisamartingalemeasureequivalenttothe realworldprobability
P. By onsidering optionpries we immediately draw inferene on this priing measure Qand
we assume from now on that S follows anexp onential Levy mo del (1.1) under Qand that the
disounted prie pro ess e r t
S
t
is amartingaleon the ltered probability spae (;F;Q;(F
t )),
xedthroughoutthepap er. Asisstandardinthealibrationliterature,themeasureQisassumed
tob e settledbythemarketandto b eidentialforalloptionstraded.
Bytheindep endene ofinrementsinX themartingaleonditionmayb e expliitlystatedas
8t>0: E[e Xt ℄=1 () 2 2 ++ Z 1 1 (e x 1)(x)dx=0: (2.3)
Observethatwehaveimp osedimpliitlytheexp onentialmomentondition R 1 0 (e x 1)(x)dx<1
to ensure the existene of E[S
t
℄. Another onsequene is that the harateristi funtion '
T is
denedonthewholestripfz 2C j Im(z)2[ 1;0℄gintheomplexplane,whihwillb eimp ortant
later. We reduethenumb erofparametersbyintro duingthenegative log-forwardmoneyness
x:=log(K =S) r T;
suh thattheallprie intermsofxisgivenby
C(x;T)=SE[(e X T e x ) + ℄:
Theanalogousformulafortheprieofaputoption,whihgivestheownertherighttosellanasset
at timeT fortheprie K,isP(x;T)=SE[(e x e X T ) +
℄. Thenthewell-knownput-allparityis
easilyestablished: C(x;T) P(x;T)=SE[e X T e x ℄=S(1 e x ): (2.4) 2.2 The observations
We fo us onthe alibrationfromoptionswithaxedmaturityT >0andmentionthe
straight-forward extension to several maturities in Setion 3.1. We observe the pries of N alloptions
(or by the put-all parity (2.4) alternatively put options) at dierent strikes K
j , j = 1;:::;N, orruptedbynoise Y j =C(K j ;T)+ j " j ; j=1;:::;N: (2.5)
j E[" 2 j ℄=1andsup j E[" 4 j
℄<1. Thenoise levels(
j
) areassumedto b ep ositive andknown. This
randomobservationmo delreetsthebid-askspread andotherfritionsatthemarket.
AsweneedtoemployFourier tehniques,we intro duethefuntion
O (x):= ( S 1 C(x;T); x>0; S 1 P(x;T); x<0 (2.6)
inthespiritofCarrandMadan(1999). Oreordsnormalisedallpries forx>0andnormalised
putpries forx60. Thefollowingimp ortantprop ertiesofO areprovedintheApp endix.
Prop osition2.1. (a) Wehave O (x)=S 1 C(x;T) (1 e x ) + forallx2R. (b) O (x)2[0;1^e x
℄holds forallx2R.
() If C
:=E[e
X
T
℄is niteforsome>1,thenO (x)6C
e
(1 )x
holdsforallx>0.
(d) Atanyx2Rnf0g,respetivelyx2R nf0;Tginthease=0and <1,thefuntion O
is twiedierentiablewith
Z Rnf0;Tg jO 00 (x)jdx63: The rst derivative O 0
has ajump of height 1atzeroand, in the ase=0and <1,
ajump of height+e T( )
oursin O 0
atT.
(e) The Fouriertransformof O satises
FO (v )= 1 ' T (v i) v (v i) ; v 2R : (2.7)
Thisidentityextendstoallomplexvaluesv withIm(v )2[0;1℄. Notethe properties'
T (0)=
1 and '
T
( i) = 1 derived from the general property of harateristi funtions and the
martingale ondition (2.3),respetively.
We transformourobservations(Y
j )andpreditors (K j )to O j :=Y j =S (1 K j e r T =S) + =O (x j )+Æ j " j ; (2.8) x j :=log(K j =S) r T; (2.9) where Æ j =S 1 j
. Inpratie, thedesign(x
j
)willb e ratherdense aroundx=0and sparsefor
optionsfurtheroutofthemoneyorinthemoney,f. Fengler, Hardle,andMammen(2003)fora
studyontheGermanDAX index.
In order to failitate the subsequent analysis we make a mildmomentassumptionon the prie
pro ess,whihguarantees byProp osition2.1(b,)theexp onentialdeayofO .
Assumption1. WeassumethatC
2 :=E[e
2XT
℄isnite. This isequivalenttopostulating forthe
assetprieanite seond moment: E[S 2
T ℄<1.
3 The estimation for bounded jump densities
LetusassumeherethattheLevypro esshasniteintensity. Laterweshallimp osealsoaertain
tehniqueneeds tob e employedandthepropagationoferrorsismoretransparent.
Sineourassetfollowsanexp onentialLevymo del,thejumpsintheLevypro essapp earexp
onen-tiallytransformedintheassetpriesanditisintuitivethatinfereneontheexp onentiallyweighted
jumpmeasure
(x):=e x
(x); x2R;
willleadtospatiallymorehomogeneousprop ertiesoftheestimatorthanforitself.Ouralibration
pro edure reliesessentiallyup ontheformula
(v ):= 1 T log 1+iv (1+iv )FO(v ) = 1 T log(' T (v i)) = 2 v 2 2 +i( 2 +)v+( 2 =2+ )+F(v ); (3.1)
whihis asimpleonsequene of theformulae(2.1)and(2.7). Note thatthe funtion is upto
a shift inthe argumentthe umulant-generating funtionof the Levy pro ess and a ontinuous
version of the logarithmmustb e taken suh that (0) = 0, whih is impliedby the martingale
ondition. Formula(3.1)showsthattheLevytripletisuniquelyidentiablegiventheobservation
of thewhole optionprie funtionO withoutnoise: F(v ) tends to zero as jv j !1due to the
Riemann-Leb esgueLemmaand 2
,, areidentiableaso eÆientsinthep olynomial,whihin
turnyieldsthefuntionF(v ). Aprop erlyrenedappliationofthis approahwillequipuswith
estimatorsfor thewhole tripletT =( 2
;;) (we parametrize Levytriplets equivalentlywith
or).
3.1 The basi proedure
Letusformulatethebasialgorithmtob eusedwhenaertainsmo othnessprop ertyisimp osedon
,thatisunderthepriorknowledge2G,whereGisasmo othnesslass. Thepro edureonsists
offoursteps: (a)webuildanapproximation ~
OofOfromthedata;(b)weobtainanapproximation
~
of byformula(3.1);()we estimatetheo eÆientsofthequadratip olynomialonthe
right-handsidein(3.1)from ~
underthepreseneofanoiseomp onentandthenonparametrinuisane
partF;(d)we obtainanestimatorforFbyonsideringtheremainder.
Themo del(3.1)hasasimilarstrutureasthewell-knownpartiallinearmo dels,butinfatthereis
onesubstantialdierene: thefuntionFisnotsupp osedtob esmo oth,butinsteaditisdeaying
forhigh frequeniesb eausewe workinthesp etraldomain. This isalsowhywe shallregularize
theproblembyuttingo frequeniesjv j higherthanaertain thresholdlevelU,whihdep ends
onthenoise levelandthesmo othnessassumptionsinG.
We nowgive adetailed desriptionofthedierentstepsinthepro edure.
(a) WeapproximatethefuntionObybuilding ~
Ofromtheobservations (O
j )intheform ~ O (x)= 0 (x)+ N X j=1 O j b j (x); x2R; and onsequentlyFO by F ~ O (u)=F 0 (u)+ N X j=1 O j Fb j (u); u2R; where (b j
)aresomebasisfuntions tob e hosen and thefuntion
0
isadded to take are
ofthejumpinthederivativeofOat zero: 0
0
(0+)
0
0
8x2R: b k (x)2[0;1℄; 8j;k=1;:::;N: b k (x j )=Æ jk ; lim juj!1 b k (u)=0:
Westress here that step (a)shouldnotb e understo o das asmo othingstep,but ratherasa
meansto ndareasonable approximationofFObased ondisrete data. As anb e seenin
thetheoretial analysisandthenumerialsimulationsb elow,itsuÆes to usesimplelinear
B-splines as basisfuntions. Theoretially, we need that theresults of Prop osition7.1 and
estimate(7.7)aresatised.
(b) For(v )2(0;1),sp eiedlaterin(4.1),wealulate
~ (v ):= 1 T log >(v ) 1+iv (1+iv )F ~ O(v ) ; v2R; (3.2)
where thefuntionlog
> :C nf0g!C isgivenby log > (z):= ( log(z); jzj log(z=jzj); jzj< (3.3)
and log()is takeninsuh away that ~
(v ) isontinuous with ~
(0)=0(almostsurelythe
argumentofthelogarithmin(3.2)do es notvanish). Ifweobserveoptionpriesfordierent
maturitiesT
k
,we p erformthesteps (a)and(b)foreahT
k
separatelyandaggregateatthis
p ointthedierentestimatorsfor toobtainoneestimatorwithless variane.
() Withanestimate ~
of athand,we obtainestimatorsfortheparametripart( 2
;;)by
an averagingpro edure takinginto aount thep olynomialstruture in(3.1). Up onxing
thesp etralut-ovalueU =U(G;(Æ
j );(x j )),weset ^ 2 := Z U U Re( ~ (u))w U (u)du; (3.4) ^ := ^ 2 + Z U U Im( ~ (u))w U (u)du; (3.5) ^ := ^ 2 2 +^ Z U U Re( ~ (u))w U (u)du; (3.6)
where theweightfuntionsw U ;w U and w U satisfy Z U U w U (u)du=0; Z U U u 2 w U (u)du= 2; Z U U uw U (u)du=1; (3.7) Z U U u 2 w U (u)du=0; Z U U w U (u)du=1: (3.8)
Forstandardsmo othnesslassesGasymptotiallyoptimalhoiesoftheut-ovalueU and
the weight funtionsare given in(4.9)and(4.2)-(4.4). Theestimateof theo eÆients an
b e understo o d as an orthogonal projetion estimate with resp et to an L 2
-salar pro dut
weightedaordingtothesupp oseddeayprop ertyofF.
(d) Finally,wedenetheestimateforastheinverseFouriertransformoftheremainder:
^ (u):=F 1 h ~ ()+ ^ 2 2 ( i) 2 i^( i)+ ^ 1 [ U;U℄ ( ) i (u); u2R : (3.9)
Notethat theomputationalomplexityofthis basiestimationpro edure isvery low. Theonly
funtions Fb
k
andthe funtionF
0
, whihwith ourhoie as linearB-splines an b e omputed
expliitly: Fb k (u):=u 2 e iux k e iux k 1 x k x k 1 e iux k+1 e iux k x k +1 x k ; F 0 (u)=u 2 1+ e iux j 0 x j0 1 e iux j 0 1 x j0 x j0 x j0 1 (3.10)
withk=1;:::;N,someextrap olateddesignp ointsx
0 andx N+1 ,whereweset ~ O (x 0 )= ~ O(x N+1 )=
0,andwiththeindexj
0 dened byx j0 1 <06x j0 .
3.2 A data-driven estimator for the jump density
Letusbrieydesrib etheonstrutionofadata-drivenpro edurewhihrequiresnopriorsmo
oth-nessassumptionsontoadjustthetuningparameters. Theideaistolterouttheparametripart
and to obtainastandard 'funtioninnoise'-estimationprobleminthesp etral domain. Instead
ofho osingoneut-ovalueU,wetakeageometrigridU
1 >U
2
>>U
J
ofut-ovaluesand
aggregatetheorresp ondingestimatorsadaptively.
Forlteringquadratip olynomialswe intro duetheonvolutionop erator
A g f(x):=f(x) 1 2 Z 1 1 f(y )Fg (x y )dy (3.11)
withasuÆientlyregularandnielydeayingfuntiong:R!Rsatisfying
Z 1 1 Fg (y )d y=1; Z 1 1 y k Fg (y )dy=0; k=1;2,thatisg (0)=1;g 0 (0)=g 00 (0)=0: (3.12)
Thersttwostepsofthedata-drivenpro edureareidential tothesteps(a)and(b)ofthebasi
pro edure. Thesubsequent stepsareas follows:
() Weapply theop eratorA
g to ~ andobtain ~ g (v ):=A g ~ (v ), whihby(3.1)isareasonable estimateof A g (v )=A g F(v )=F((1 g ))(v ).
(d) Weonsiderthefamilyofbasiestimators~ (j) g givenby ~ (j) g :=F 1 ~ g 1 [ U j ;U j ℄ (y ); j=1;:::;J:
(e) We onstrut the aggregated estimator ^
g as a onvex ombination of (~ (j) g ) j=1;:::;J with
data-dep endentweights. Theseweightsareobtainedbythefollowingalgorithm:
(i) Initialize^ (1) g =~ (1) g .
(ii) For j=2;:::;J sequentiallydene
^ (j) g := j ~ (j) g +(1 j )^ (j 1) g ; where j =K(m (j)
=)forsome>0,aompatlysupp orted kernel K and
m (j) := k~ (j) g ^ (j 1) g k 2 L2 kVar[~ (j) g ℄k L1 : (iii) Put^ g :=^ (J) g . AlthoughVar[~ (j) g
℄isnotknownexatly,itanb eeasilyestimatedfromab ove. The
param-eter istakeninaordanewiththesuggestionsgiveninBelomestnyandSp okoiny(2004),
−1.0
−0.5
0.0
0.5
1.0
0.00
0.02
0.04
0.06
0.08
0.10
0.12
−2
−1
0
1
2
0
5
10
15
data.driven
basic
0.16
0.17
0.18
0.19
0.20
0.21
Figure 1: Kou mo del. Left: Sample(O
j
) and true funtion O (dashed line). Center: True
(dashed) and estimated ^ (blak)mo diedLevy densities. Right: Box plot for the data-driven
andthebasipro edure basedon1000Monte-Carlosimulations.
(f) Thenalestimatorfor(x)isdenedas(x)^ =^
g
(x)=(1 g (x))forallx2Rwithg (x)6=1.
Example1. Apossiblefamilyoffuntionsgsatisfying(3.12)isgivenbyg
(x)=1 (1 e x 2 = 2 ) 2 ,
x 2 R, > 0, whih gives rise to the onvolution lter Fg
(u) = p e 2 u 2 =4 p 8 e 2 u 2 =8 . Observe that 1 g
only vanishes at zero and that for smaller values of the weight 1 g
is
losertooneoutsidethe origin, butthe lterFg
doesnot deaysorapidly.
3.3 Numerial Example
Twoempirialphenomenainnanialdatahaveattratedmuhattentionreently: theleptokurti
return distributionofassets withahigherp eakandtwo(asymmetri)heavier tailsthanthose of
thenormaldistribution,andtheimpliedvolatilitysmile. Toinorp oratethesefeatures,thedouble
exp onential jumpdiusion mo delwas prop osed by Kou (2002). Inhis mo del theLevy triplet is
sp eied bythejumpdensity
(x)= p + e +x 1 [0;1) (x)+(1 p) e x 1 ( 1;0) (x) ; x2R;
andtheparameters;;
+
; >0andp2[0;1℄,whileisuniquelydeterminedbythe
martin-galeondition. We simulatetheKou mo delwith parameters =0:1;=5; =4;
+
=8;p=
1=3and apply thenonparametri estimationpro edure giventheobservation ofnoisy Europ ean
optiondata withT =0:25,N =50,r=0:06and Æ
j =O (x
j )=10.
InFigure1(left)thesimulatedobservations(O
j
)andthetrueurve Oaredepited as funtions
ofthelog-forwardmoneyness. TheestimatedtransformedLevydensityintheenterisobtained
using thebasipro edure, assp eied inthemathematialanalysis,withahuman-drivenhoie
oftheut-oparameterU. Theparameterswereestimatedas^=0:035; ^
=7:56;^=0:556(=
0:423). Weobserve thattheestimatedtransformedLevydensityreoversthemainfeaturesofthe
Koumo dellikethemo deatzeroandtheskewness. Fromthefuntionalformoftheestimatorwe
aneasilyderiveestimatesforotherimp ortantquantities,e.g. fortheprop ortionofnegativejumps
byalulating ^ 1 R 0 1 ^ (x)dx= ^ 1 R 0 1 e x ^
(x)dx,whihinthesimulationexampleevaluates
to0:72(truevalue: 1 p=2=3).
IntherightpartofFigure1weomparethep erformaneofthedata-drivenaggregatedestimator
withtheoraleestimator(i.e,ho osingtheb estp ossibleU)obtainedfromthebasipro edurein
termsoftheempirialL 2
-loss. Ab oxplotisshownfor1000Monte-Carlorepliations. Inthisplot,
as provided by the statistial software pakage R, the b oxstrethes fromthe 25% p erentile to
the75%p erentile,rossed bythemedian,andthep ositionoftheremaining50%ofthevaluesis
basiestimators. Asp ointedoutbyCavalierandGolub ev(2004),standarddata-drivenestimation
pro eduresoftenp erformbadlyforinverseproblemssuhthatthemetho dofaggregationusedhere
anb e onsideredasomparativelyverystable.
4 Risk bounds for bounded jump densities
4.1 Mathematial results
We shall use throughout the notation A . B if A is b ounded by a onstant multiple of B,
indep endent of the parameters involved, that is, in the Landau notation A = O (B). Equally
A&B meansB.AandAsB standsforA.B andA&B simultaneously.
In order to assess the quality of the estimators, we quantify their risks under a Sob olev-typ e
smo othnessonditionofordersonthetransformedjumpdensity.
Denition4.1. For s 2Nand R;
max
>0 let G
s (R;
max
) denote the set of all Levy triplets
T =( 2
;;),satisfying the martingale onditionand Assumption 1withC
2
6R,suh that is
s-times (weakly)dierentiable and
2[0; max ℄; jj;2[0;R℄; max 06k 6s k (k ) k L 2 (R) 6R; k (s) k L 1 (R) 6R: We have enfored j ~ T
(v )j > log((v )) in (3.2) to prevent unb oundedness in the ase of large
sto hasti errors. For Levy triplets inG
s (R;
max
)a reasonable hoie for (v ) an b e obtained
fromthefollowingalulationusing theidentity
2
2
++F(0)=derivedfromthemartingale
ondition(2.3): 1 2 j' T (v i)j= 1 2 exp T 2 2 v 2 TF(0)+TRe(F(v )) > 1 2 exp T 2 max 2 v 2 4TR =:(v ): (4.1)
Theonlyreasonforthefator1=2isthemathematialtratabilitygivinglatertheb oundofLemma
7.2.
Conerning the hoie of the weight funtions, we take advantage of the smo othness s of by
takingfuntionswsuhthatFwhassvanishingmoments.Equivalentlyexpressedinthesp etral
domain,theweightfuntions w (u) growwithfrequenies juj like juj s
toprot fromthedeay of
jF(u)j. Hene, we dene for allU >0familiesofweightfuntions by resalingthose funtions
satisfyingrestritions(3.7)and(3.8)for U=1:
w U (u)=U 3 w 1 (U 1 u) withw 1 satisfying(3.7)andkF(w 1 (u)=u s )k L 1<1; (4.2) w U (u)=U 2 w 1 (U 1 u) withw 1 satisfying(3.7)andkF(w 1 (u)=u s )k L 1<1; (4.3) w U (u)=U 1 w 1 (U 1 u) withw 1 satisfying(3.8)andkF(w 1 (u)=u s )k L 1 <1: (4.4)
Inthesedenitionsitisundersto o dthatthesupp ortoftheweightfuntionsisontainedin[ U;U℄.
Notethat theprop erty F(w (u)=u s
)2L 1
(R)means inpartiular thatw (u)=u s
is ontinuousand
b oundedsuh that
jw U (u)j.U (s+3) juj s ; jw U (u)j.U (s+2) juj s and jw U (u)j.U (s+1) juj s : (4.5)
For the simulationswe have used symmetri weight funtions that are onstant multiplesof u 2
exept for three(at 0andU for)resp etivelyfour (atU 0 ;U with someU 0 <U for 2 ,)
theasymptotisofagrowingnumb erof observationswith := max j=2;:::;N (x j x j 1 )!0 and A:=min(x N ; x 1 )!1: (4.6)
WeuselinearB-splinesforthebasisfuntions(b
k
)andthefuntion
0
. Toeasethemathematial
treatmentof theextrap olation error,weassume that alldata isontainedintheinterval( A
;A+)andaddtheartiialobservationsx
0 = A ,x N+1 =A+withO 0 =O N+1 =0.
The reason why we ho ose a pieewise linear approximationis that this yields rate-optimal
in-terp olation errors for ~
O , knowing that O is twie dierentiable exept at nitely many p oints,
f. Prop osition 7.1 b elow. Of ourse, when assuming some p ositive regularity on or by some
adaptivemetho d,thenumerialapproximationratewithresp et toanb eaelerated,butthis
improvementisonlyvalidforavery smalldisretisation distanewhenthesto hasti
observa-tionerrorisusuallydominantanyway.Inontrasttostandardregressionestimatesweshallalways
trak expliitlythedep endene onthelevel(Æ
k
)of thenoiseintheobservations,whih isusually
rathersmallforobserved optionpries.
Thesubsequentanalysis an ertainly b e improvedforaonrete design(x
j
)and onrete noise
levels(Æ
j
),butforrevealingthemainfeaturesitismoretransparentandonisetostatetheresults
intermsoftheabstratnoise level
":= 3=2 + 1=2 kÆk l 1 ; (4.7)
omprisingthelevelofthenumerialinterp olationerrorandofthesto hastierrorsimultaneously.
HereandinthesequelweusethenormskÆk
l 1 :=sup k Æ k andkÆk 2 l 2 := P k Æ 2 k .
We arenowinap ositionto statethemainresultsab outtheriskupp er b oundsof theestimators
obtainedbythebasipro edureandab outtherisklowerb oundsvalidforanyestimationpro edure
whatso ever. Thepro ofsaregiveninSetions7and8fortheupp erandlowerb ounds,resp etively.
Theorem4.2. Assume e A . 2 and kÆk 2 l2 .kÆk 2 l 1
. Choosing forsome>
max the ut-o U := 1 (2log(" 1 )=T) 1=2
,weobtain fortherisk of^ 2
the uniformonvergenerate
sup T=( 2 ;;)2G s (R; max ) E T [j^ 2 2 j 2 ℄ 1=2 . s+3 (log(" 1 )) (s+3)=2 : (4.8)
Theasymptotiriskintheestimationoftheotherunknownquantitiesshowsadihotomy. While
usuallyitislargerthantheriskfor^ 2
,itismuhsmallerifweknowthat=0holds,thatis,for
theomp oundPoissonase.
Theorem4.3. Assume e A . 2 andkÆk 2 l 2 .kÆk 2 l 1 . For any> max wehoose U := 1 2log(" 1 )=T 1=2 ; U 0 :=" 2=(2s+5) ; (4.9) inthe ases max >0and max
=0, respetively. Then the riskbounds for^and ^ are sup T=( 2 ;;)2Gs(R;max) E T [j^ j 2 ℄ 1=2 . ( s+2 (log(" 1 )) (s+2)=2 ; 2[0; max ℄unknown ; " (2s+4)=(2s+5) ; = max =0; (4.10) sup T=( 2 ;;)2G s (R; max ) E T [j ^ j 2 ℄ 1=2 . ( s+1 (log(" 1 )) (s+1)=2 ; 2[0; max ℄unknown, " (2s+2)=(2s+5) ; = max =0: (4.11) Theorem4.4. Assume e A . 2 and kÆk 2 l 2 .kÆk 2 l 1. For some> max we hooseU and U 0
asin (4.9)toobtainthe followingrisk estimatesfor:^
sup T=( 2 ;;)2Gs(R;max) E T h Z 1 1 j(x)^ (x)j 2 dx i 1=2 . ( s (log(" 1 )) s=2 ; 2[0; max ℄ unknown, " 2s=(2s+5) ; = max =0: (4.12)
thewidth A of thedesignonly needs to growlogarithmiallyandthe error levels (Æ
k
) needonly
b e square summableafter renormalisation. Thelatter onditionan ertainlyb e further relaxed
sine thistermisausedbyarough b oundonthequadratiremainderterm.
Forthelowerb oundsweapp ealtotheequivaleneb etweentheregressionandtheGaussianwhite
noisemo del,asestablishedbyBrownandLow(1996),andonsidermerelytheidealizedobservation
mo del
dZ(x)=O (x)dx+"dW(x); x2R; (4.13)
with the noise level asymptotis " ! 0, a two-sided Brownian motion W and with O = O
T
denotingthe optionprie funtion from(2.6)for thegiventriplet T. This simpliation avoids
tedious numerialapproximationsinthepro ofs.
Theorem 4.5. Lets 2N, R>0and
max
>0be given. For the observationmodel (4.13)and
any quantityq2f 2
;;;gthe following asymptotirisklowerbounds hold:
inf ^ q sup T2Gs(R;max) E T [k^q q k 2 ℄ 1=2 &v q ;max ;
wherekkdenotes theabsolutevalueforq2f 2
;;gand theL 2
(R)-normforq=,theinmum
isalways takenover allestimators, thatisallmeasurable funtions of the observationZ,and the
rate v
q ;
max
isgiven inthe followingtable:
2 max >0 log(" 1 ) (s+3)=2 log(" 1 ) (s+2)=2 log(" 1 ) (s+1)=2 log(" 1 ) s=2 max =0 0 " (2s+4)=(2s+5) " (2s+2)=(2s+5) " 2s=(2s+5) 4.2 Disussion
We have seen that for > 0 the rate orresp onds to a severely ill-p osed problem (f. Engl,
Hanke,andNeubauer (1996)and thereferenes there),whileforknown=0therates aremuh
b etter, but still ill-p osedompared to those obtainedinlassial nonparametriregression. The
reason forthesevereill-p osedness for>0isthat we fae anunderlyingdeonvolutionproblem
with a Gaussian distribution: thelaw of the diusion part of X
T
is onvolvedwith that of the
omp ound Poisson part to give the density of X
T
. This typ e of estimation problem has b een
studied thoroughlybyButuea andMatias(2005)inanidealizeddensity estimationsetup. Note
thegeneral orderinwhih the(asymptoti)qualityof estimationdereases: 2
, , and nally
,whihisrelatedtothedominationprop ertyformulatedinAt-SahaliaandJao d(2004). Inthe
upp er b oundswehave kepttrak ofthedep endene onb eauseforsmallvaluesof andnite
samplesthep erformaneisnotsobad,omparethesimulationsinSetion3.3;itjustneeds alot
moreobservationstoimproveonthat.
At rst sight the rates for the parametri estimation part in the ase = 0 are astonishing.
They are worse than in usual semi-parametri problems whih also indiates that missp eied
parametrimo delswillgiveunreliableestimatesforthevolatilityandjumpintensity. Theserates
are, however,easilyundersto o d whenemployingthelanguageofdistributions. WithÆ
0
denoting
theDiradistributioninzero andÆ 0
0
itsderivative we have
log(' T (u))=TF Æ 0 0 + Æ 0 (u):
EstimatingthedensityofX
T
andsimilarlyitsharateristi funtionfromthenoisyobservations
of O amountsroughly to dierentiate the observed funtion twie, f. At-Sahalia and Duarte
(2003)andtheremarkafterequation(7.6)b elow. Thisgivestheminimaxrateforandasthat
ofestimatingtheseondderivative ofaregression funtionofregularitys+2. For theparameter
it suÆes to estimate the jump in the antiderivative of F 1
(log('
T
analogyis the estimationof the regression funtionitself at zero. This explains also why inthe
lass G
s
we have measured theregularitynotonly in L 2
, but also uniformly. In fat, ifwe only
assumeanL 2
-Sob olevondition,thenthesamelowerb oundtehniques willyieldslower ratesfor
the parameters,as is typial for p ointwise estimationproblems. An interesting way to estimate
diretly andissuggestedbyProp osition2.1(d): ahangep ointdetetion algorithmforjumps
inthederivativeof O ,as prop osed by Goldenshluger,Tsybakov, andZeevi (2004), an equip us
with anestimateof and asubsequent estimateof thejumpsize yieldsan estimateof, whih
gives thesameminimaxrates.
Asusual,theestimationpro edureneedsertaintuningparameters.Theapproximatesizeof
max
and thenoise levelis ingeneral knownto thepratitioner. The stabilisationofthe logarithmby
the funtion(v ) was enfored mainlyfor theoretial reasons to prevent explosions due to large
deviations. Theusuallyunknownordersofsmo othnessofthetransformedjumpdensity,however,
is needed to determine ago o dhoie of theut-o frequeny U andalso app ears inthe weights
w 1 ;w 1 ;w 1
. Yet, for thelatter it suÆes to useweight funtions satisfying (4.2)-(4.4)for some
larges
max
likeinstandardnonparametriswheretheorderofthekernelmustonlyb esuÆiently
large. WearethusleftwithonlyonetuningparameterU,whihisthesameforallfourestimation
problems. Thedata-drivenpro edurepresentedinSetion3.2isonewaytoop ewiththisproblem
forthejumpdensity. Note,however,thataprop er mathematialanalysisforthegeneralproblem
seems hallengingduetotheunderlying nonlinear'hangep ointdetetion'-struture, forwhiha
data-drivenalgorithmeveninthe idealizedlinear settingof Goldenshluger,Tsybakov,andZeevi
(2004)isnotyetavailable. Finally,observethattheestimationofthejumpdensityatzeroisonly
p ossiblebyimp osingaertainregularitythere,otherwiseitislearlynotp ossibletodetetjumps
ofheightzero.
5 Estimation for unbounded jump densities
Letusnowdisussthease that isajumpdensitywithasingularityatzero. For simpliitywe
restritthepresentationtothease=0,whihisalsoinagreementwiththeempirialparametri
ndings by Carr, Geman, Madan,and Yor (2002). We then dedue as b efore for(x) =e x
(x)
using(2.3),(2.7)andthedenition(3.1)of intermsofO
(v )=iv+ Z 1 1 (e iv x 1)(x)dx=iv+ Z v 0 F(ix(x))(w )dw : UnderAssumption1x(x)2L 1
(R)holds. Bytakingderivativeswe nd
0 (v )= (i 2v )FO (v ) (v iv 2 )F(xO (x))(v ) T(1+(iv v 2 )FO(v )) =i+F(ix(x))(v ):
We rst onsider the problem of estimating in someweighted L 2
-loss with a weight funtion
vanishing inzero. More preisely, we aimatestimating
g
(x)=(x)(1 g (x)) inL 2
(R)-loss for
somedierentiableniely deaying funtiong :R![0;1℄with g (0)=1. We obtain
g 2L 1 (R) and F g (v )= 1 2 i F(ix(x))F((1 g (x))=x)( v ) =g 0 (0)+ 1 2 i (i 2)FO (+i 2 )F(xO (x)) T(1+(i 2 )FO ) F((1 g (x))=x) ( v ) (5.1)
The onvolution kernel F((1 g (x))=x) deays rapidly for smo oth funtions g suh that for a
go o d approximationof F
g
(v ) it suÆes to know the funtions FO and F(xO (x)) in a lose
g
~
O of O into formula(5.1) and using someg with g 0
(0)=0. Thenoise levelfor frequenies v in
theempirialounterpart of (5.1)willb eoforderv 2
intheniteintensityase =kk
L 1
(R) <1
exatly asintheprevious analysisfor=0. For=1theharateristi funtiontendstozero
andtheestimationerror willdeteriorate signiantly,seethedisussion b elow.
Whendrawinginfereneontheb ehaviourofnearzero,wehavetosp eifythekindofsingularity
andsmo othnesswe exp etthere. Letustherefore p ostulatethat
(x)= (x) jxj with2(0;2)andjF (u)j.(1+juj) (s+1) ; s2N: (5.2)
To avoid additional onsiderations we assume that 6= 1. Note that this mo del inludes for
example temp ered stable pro esses with regularity index s = 1, when their transformed jump
densityisgivenby (x)=e x (x)=C e (1+ )x jxj 1 ( 1;0) (x)+ e (1 + )x jxj 1 (0;1) (x) ; C ; >0; + >1; x2R;
f. Chapter4 inCont andTankov(2004a) whih also gives further examples. Under themo del
(5.2) an interesting information on the b ehaviour of near zero is given by the value
(0),
for whih we now want to derive an estimationpro edure. Beause of x(x) = x 1 (x) (we understand always x := jxj sgn (x)) we an draw inferene on F(x 1
(x)), but this Fourier
transformdeaysslowlyduetoitsnon-dierentiableargumentandwillnotyieldawellp erforming
estimator. Consequently, we have to use more rened frational dierentiation results for the
preisestruture ofthis Fouriertransform. Thefollowingresult isderived intheApp endix.
Prop osition5.1. The followingasymptotiestimate holdsforjuj!1:
F(ix 1 (x))(u) 2 (2 )sin( =2) s 1 X k =0 2 k (k ) (0)i k u 2 k .juj s min(1;2 ) ;
where denotes the EulerGamma funtion.
Hene, we anexpand 0
inanon-integerp ower series:
0 (u)=i+2 (2 )sin( =2) s 1 X k =0 2 k (k ) (0)i k u 2 k +R(u)
with the remaindersatisfyingjR(u)j .juj
s max(1;2 )
. Exatly as inthe expansion (3.1), this
p ermitstoestimate (0)based onanestimator ~ by^ (0):= R U U ~ 0 (u)w U
(u)duwithaweight
funtionw U satisfying Z U U u 2 w U (u)du= 1 2 (2 )sin( =2) ; Z U U u w U (u)du=0for=0;= 2 k
with k 2 f1;:::;s 1g. For this estimator a similar analysis as in the ase of b ounded jump
densities an b ep erformed. Themaindigressionisthat for>1,theinniteintensityase,the
harateristi funtionis not b ounded away fromzero anymore and the risk willb e essentially
determinedbythegrowthofj'
T (u i)j
1
withjuj!1,whih isusuallyexp onential(e juj
1
in
thetemp eredstablease)and thusyields againaseverelyill-p osedproblem.
6 Conlusion
Wehavedevelop edanestimationpro edureforthenonparametrialibrationofexp onentialLevy
thatthealibrationisingeneralahardproblemtosolve,atleastifveryhigh aurayisdesired.
Nevertheless the estimationpro edure is well suited to gain general insight into the size of the
parametersandthestruture ofthejumpdensity. Evenifreasonableparametrimo delsexistthat
anb e b ettertted,ago o dness-of-ttestbasedonournonparametriapproahshouldalwaysb e
usedto hekagainstmissp eiation.
As already seen inthe ase of unb ounded jumpdensities, our pro edure an b e adapted to
dif-ferent mo delsas long as the inverse transformationfrom the optionpries to the harateristi
funtionan b ealulated and theunknown quantities an b e determined fromthestruture of
theharateristifuntion. Asempirialoptiondatasuggests,theriskneutralpriepro ess isnot
homogeneousintimeandtheexp onentialLevymo delshouldb eextendedinthatdiretion. A
suit-ablemo dellassisforinstane givenbytheaÆnemo delsofDuÆe,Filip ovi,andShahermayer
(2003). Web elievethat thequestion ofalibrationformo delsinnanialmathematisshouldb e
addressedwiththesamerigourandintensityasotherprimaryquestionslikepriing,hedgingand
riskmanagement.
7 Proof of the upper bounds
Allalulationstake plaeinthesettingofSetion 4. Asgeneral referene forFourier tehniques
like the Planherel identity and normestimates we reommend Rudin (1991). To failitate the
alulationswe intro duetheexp onentiallyinreasingfuntion
E(x):= e x 1 x ; x>0; andsetE(0):=1: (7.1)
UsinglinearB-splines(f. Setion 3.1)weenounter thefollowinglinearinterp olationofO
O l (x):=E[ ~ O (x)℄= N X j=1 O (x j )b j (x)+ 0 (x); x2R : (7.2)
7.1 A numerial approximation result
Prop osition 7.1. Under the hypothesis e A
.
2
we obtain uniformly over all Levy triplets
satisfying Assumption1
sup
u2R jE[F
~
O(u) FO (u)℄j=sup
u2R jFO l (u) FO (u)j. 2 : (7.3)
Proof. BystandardFourierestimatestheassertionfollowsonewehaveprovedkO
l O k L 1 . 2 . Note that O 0
is twie dierentiable exept at the p oints x
j 0 1 ;0;x j 0 and p ossibly T by
Prop osition2.1(d). Whilethedisontinuitiesof(O
l
0 )
0
attheknotp ointsdonotdoanyharm,
O
0
hasaderivativenearzerowhihisuniformlyb oundedbyaonstantC
0
aordingto(9.1).
Starting with the ase > 0, that is without a jump at T, we obtain using the mean value
theoremwithsuitable
j 2(x j 1 ;x j ): Z x N x1 j ~ O l (x) O (x)jdx = N X j=2 Z xj x j 1 (O 0 )(x j ) x x j 1 x j x j 1 +(O 0 )(x j 1 ) x j x x j x j 1 + 0 (x) O (x) dx
= N+1 X j=1 xj x j 1 x x j 1 ((O 0 ) 0 ( j ) (O 0 ) 0 (y ))d y dx 6 X j2f2;:::;Ngnfj 0 g Z x j x j 1 Z x x j 1 Z x j x j 1 jO 00 (z)jdzdydx+2C 0 2 6kO 00 k L 1 2 +2C 0 2 :
ByAssumption1andProp osition2.1(b,)theextrap olationerror isb oundedby
Z [x0;x1℄[[xN;xN+1℄ jE[ ~ O(x) O (x)℄jdx64C 2 e (A ) :
An appliationofProp osition2.1(d)therefore showsfor>0
Z 1 1 jE[ ~ O (x) O (x)℄jdx6e A +3 2 +2C 0 2 +4C 2 e (A ) . 2 :
Inthe ase =0we onsider the index j
with x
j 1
6 T <x
j
andfae an additionalerror
estimatedby Z xj xj 1 jE[ ~ O (x) O (x)℄jdx6 Z xj xj 1 k(O 0 ) 0 k L 1 2(x x j 1 )(x j x) x j x j 1 dx 6k(O 0 ) 0 k L 1 (x j x j 1 ) 2
Withalo okat(9.1)we inferthatthiserror termisalsooforder 2
andthusdo esnotenlargethe
onvergenerate.
7.2 Proof of Theorem 4.2
Theassertedrate(4.8)followsonethegeneralriskestimate
E[j^ 2 2 j 2 ℄.U 2(s+3) +E(T 2 U 2 )U 1 " 2 +E(T 2 max U 2 ) 2 U 4 " 4 (7.4)
hasb een shown for U . 1
uniformlyover G
s (R;
max
), sine theexpliit hoie of U renders
theseondandthirdtermasymptotiallynegligible.
Consider inthedenition(3.2)of ~
separatelythelinearisationL,negletingthestabilisationby
,andtheremaindertermR:
L(u):=T 1 ' T (u i) 1 (u i)uF( ~ O O )(u); (7.5) R(u):= ~
(u) (u) L(u): (7.6)
Whennegletingtheremainderterm,we mayview ~
(u) asobservation of (u)inadditivenoise,
whoseintensitygrowslikej'
T (u i)j 1 j(u i)ujsu 2 e T 2 u 2
forjuj!1. Thisheteroskedastiity
reets thedegreeofill-p osednessoftheestimationproblem.
Lemma 7.2. Forallu2Rtheremainder termsatises
jR(u)j6T 1 (u) 2 (u 4 +u 2 )jF( ~ O O )(u)j 2 :
Proof. Letusset'~
T
(u i):=1 u(u i)F ~
O (u)whihequalse T
~
(u)
ifj'~
T
(u i)j>(u). Using
je T
~
(u)
j>(u),u2R,weobtainbyaseond-orderexpansion ofthelogarithm
jT ~ (u) log(' T (u i))) ' T (u i) 1 (e T ~ (u) ' T (u i))j6 1 2 (u) 2 je T ~ (u) ' T (u i)j 2 :
T T (u)6j' T (u i)j=2toinfer j' T (u i) 1 (e T ~ (u) ~ ' T (u i))j6 1 2 (u) 1 je T ~ (u) ~ ' T (u i)j j'~ T (u i) ' T (u i)j(u) 1 6 1 2 (u) 2 j'~ T (u i) ' T (u i)j 2 = 1 2 (u) 2 (u 4 +u 2 )jF( ~ O O )(u)j 2 :
Togetherwiththeprevious result thisgivesfor allu2Rtheassertion ofthelemma.
We shall frequently use the following norm b ounds for the B-splines (b
k
), whih follow from
kb k k 1 =1andjx k +1 x k 1 j62: kFb k k L 2 = p 2 kb k k L 26(4 ) 1=2 ; kFb k k 1 6kb k k L 1 62: (7.7) We deomp ose^ 2
intermsofLandRfrom(7.5)and(7.6):
^ 2 = Z U U 2 2 (u 2
1)++Re(F(u)) +Re(L(u)+R(u)) w U (u)du = 2 + Z U U
Re F(u)+L(u)+R(u) w U (u)du; (7.8) whihyields E[j^ 2 2 j 2 ℄63 Z U U F(u)w U (u)du 2 +3E h Z U U L(u)w U (u)du 2 i +3E h Z U U R(u)w U (u)du 2 i :
Letusonsiderthethreetermsinthesumseparately. ThenuisaneofFauses adeterministi
error whih anb eb oundedusing(iu) s
F(u)=F (s)
(u)and thePlanherelisometry:
Z U U F(u)w U (u)du =2 Z 1 1 (s) (x)F 1 (w U (u)=(iu) s )(x)d x 6 k (s) k 1 kF(w 1 (u)=u s )k L 1 U s+3 : (7.9)
Thelinearerror termanb e splitintoabiasandavarianepart (Var[Z℄:=E[jZ E[Z℄j 2 ℄): E h Z U U L(u)w U (u)du 2 i = Z U U ' T (u i) 1 (u i)uE[F( ~ O O )(u)℄w U (u)du 2 +Var h Z U U ' T (u i) 1 (u i)uF ~ O (u)w U (u)du i =:L 2 b +L v :
Thebiastermiseasilyb ounded byProp osition7.1,usingtheuniformb oundonU s+3 w U (u)=u s : jL b j6kF(O l O )k 1 Z U U j' T (u i)j 1 (u 4 +u 2 ) 1=2 jw U (u)jdu . 2 U (s+3) Z U U e T 2 2 u 2 +2Tkk L 1 juj s+2 du: Makinguseof R U 0 2ue u 2 du= e U 2 1 =E(U 2 )U 2
forany>0,we estimatethelast integralby
Z U U e T 2 2 u 2 +2Tkk L 1 juj s+2 du6e 2Tkk L 1 U s+3 E(T 2 2 U 2 )
L jL b j. 2 E(T 2 2 U 2 ): (7.10)
Forthe variane partof thelinearerror term we usethesupp ort prop erties supp (w U )2[ U;U℄ and supp(b k )=[x k 1 ;x k +1
℄. Severalappliations ofthePlanherel identity,the Cauhy-Shwarz
inequalityandestimate(7.7)thenyield
L v = Z U U Z U U Cov ' T (u i) 1 (u i)uF ~ O(u);' T (v i) 1 (v i)v F ~ O(v ) w U (u)w U (v )d udv = N X k =1 Æ 2 k Z U U ' T (u i) 1 (u i)uFb k (u)w U (u)du 2 =2 N X k =1 Æ 2 k Z 1 1 F 1 ' T (u i) 1 (u i)uw U (u) (x)b k ( x)dx 2 62 N X k =1 Æ 2 k Z x k+1 xk 1 F 1 ' T (u i) 1 (u i)uw U (u) ( x) 2 dxkb k k 2 L 2 .kÆk 2 l 1 Z 1 1 F 1 ' T (u i) 1 (u i)uw U (u) ( x) 2 dx skÆk 2 l 1 Z U U j' T (u i)j 2 (u 4 +u 2 )w U (u) 2 du .U 1 E(T 2 U 2 )kÆk 2 l 1 :
Altogether we obtainforthelinearerror term
E h Z U U L(u)w U (u)du 2 i .E(T 2 U 2 ) 4 +U 1 kÆk 2 l 1 : (7.11)
It remains to estimate the quadrati remainder term. We use Lemma 7.2, Prop osition7.1, the
indep endene of("
k
),thenitenessoftheirfourthorder momentsandestimates(4.5),(7.7):
E h Z U U R(u)w U (u)du 2 i . Z U U Z U U E h F( ~ O O )(u)F( ~ O O )(v ) 2 i u 4 w U (u)v 4 w U (v ) (u) 2 (v ) 2 dudv . Z U U Z U U kF(O l O )k 4 1 +E[jF( ~ O O l )(u)F( ~ O O l )(v )j 2 ℄ u 4 w U (u)v 4 w U (v ) (u) 2 (v ) 2 dudv . Z U U Z U U 8 +E h N X k ;l=1 Æ k Æ l " k " l Fb k (u)Fb l (v ) 2 i u 4 w U (u)v 4 w U (v ) (u) 2 (v ) 2 dudv . Z U U Z U U 8 + N X k ;l=1 Æ 2 k Æ 2 l jFb k (u)j 2 jFb l (v )j 2 u 4 w U (u)v 4 w U (v ) (u) 2 (v ) 2 du = 4 Z U U u 4 w U (u) (u) 2 du 2 + Z U U N X k =1 Æ 2 k jFb k (u)j 2 u 4 w U (u) (u) 2 du 2 . 8 U 4 + 4 U 4 kÆk 2 l 2 E(T 2 max U 2 ) 2 :
Thisgivestheresultthat thetotalriskof^ 2 is oforder E[j^ 2 2 j 2 ℄.U 2(s+3) + 4 +U 1 kÆk 2 l 1 E(T 2 U 2 )+ 8 U 4 + 4 U 4 kÆk 2 l 2 E(T 2 max U 2 ) 2 :
Beause ofU . and kÆk l 2 .kÆk l 1
theb oundsimpliesto(7.4).
7.3 Proof of Theorem 4.3
The rates (4.10)and (4.11)follow fromtherate-optimal hoie (4.9) of U and the G
s (R;
max
)-uniformriskestimates
E[j^ j 2 ℄.U 2(s+2) +E(T 2 U 2 )U" 2 +E(T 2 max U 2 ) 2 U 6 " 4 ; (7.12) E[j ^ j 2 ℄.U 2(s+1) +E(T 2 U 2 )U 3 " 2 +E(T 2 max U 2 ) 2 U 8 " 4 ; (7.13)
wheninserting=0inthease
max =0.
Sinethelaimedriskb oundfor^islargerthanfor^ 2
,we onlyneedtoestimatetheriskof^+ ^ 2
2
instead ofthat for^. Equally,wean restrit to ^ ^ 2 2 ^ instead of ^
. Then thepro of follows
exatly thelines of the pro of for ^ 2
, theonly dierene b eing the dierent norminginestimate
(4.5)givingrise toafatorU for andafatorU 2
for. Itremainsto notethat we obtainthe
b ounds inthe omp ound Poisson ase by setting =
max
=0and onsidering the ontinuous
extensionoftheb oundsforthatase: For^we obtainasbias
Z U U F(u)w U (u)du .U (s+2) : (7.14)
Thelinearerror termisestimatedby
E h Z U U L(u)w U (u)du 2 i . ( E(T 2 U 2 ) U 2 4 +UkÆk 2 l 1 ; 2[0; max ℄unknown, U 2 4 +UkÆk 2 l 1 ; = max =0: (7.15)
andtheremaindersatises
E h Z U U R(u)w U (u)du 2 i . ( 8 U 6 + 4 U 6 kÆk 2 l 2 E(T 2 max U 2 ) 2 ; 2[0; max ℄unknown, 8 U 6 + 4 U 6 kÆk 2 l 2 ; = max =0: (7.16)
Altogether we obtaintheriskestimate(7.12).
For ^
weobtainthesameasymptotierror b oundsas for,^ but multipliedbyU whenregarding
thero otmeansquareerror. Thisgives(7.13)and(4.11).
7.4 Proof of Theorem 4.4
Theassertionfollowsasso onasthefollowingG
s (R;
max
)-uniformriskb oundforgeneralU holds:
E h Z 1 1 j(x)^ (x)j 2 dx i .U 2s +E(T 2 U 2 )U 5 " 2 +E(2T 2 max U 2 )U 9 " 4 : (7.17)
Thebiasinestimatingdueto theutoatU an b eestimatedby
Z 1 1 jF(u)(1 1 [ U;U℄ )j 2 du6U 2s Z 1 1 juj 2s jF(u)j 2 d u=U 2s k (s) k 2 L 2: (7.18)
Thevariane terman b e split upaording to thedierent riskontributions. For u2[ U;U℄
we obtain E[jF(^ )(u)j 2 ℄64E[j ~ (u) (u))j 2 ℄+4(u 2 +1) 2 E[j^ 2 2 j 2 ℄ +4(u 2 +1)E[j^ j 2 ℄+4E[j ^ j 2 ℄ .E[jL(u)j 2 ℄+E[jR(u)j 2 ℄+U 4 E[j^ 2 2 j 2 ℄+U 2 E[j^ j 2 ℄+E[j ^ j 2 ℄ .E[jL(u)j 2 ℄+E[jR(u)j 2 ℄+U 2(s+1) +E(T 2 U 2 )U 3 " 2 +E(T 2 max U 2 ) 2 U 8 " 4 :
E[jL(u)j 2 ℄6j' T (u i)j 2 (u 4 +u 2 )(kF(O O l )k 2 1 +Var[F ~ O (u)℄).e T 2 u 2 u 4 4 + 2 kÆk 2 l 2 :
Withalo okatLemma7.2weestimatetheremainderby
E[jR(u)j 2 ℄616(u) 4 (u 4 +u 2 ) 2 E[jF(O l O )(u)j 4 +jF( ~ O O l )(u)j 4 ℄ .e 2T 2 max u 2 u 8 8 + 4 kÆk 4 l 2 :
ThePlanherel identityandtheseestimatesyieldtogether(7.17)via
Z 1 1 E[j^(x) (x)j 2 ℄dx.U 2s +E(T 2 U 2 )U 5 " 2 +E(2T 2 max U 2 )U 9 " 4 +E(T 2 U 2 )U 4 " 2 +E(T 2 max U 2 ) 2 U 9 " 4 sU 2s +E( 2 U 2 )U 5 " 2 +E(2T 2 max U 2 )U 9 " 4 :
8 Proof of the lower bounds
WefollowtheusualBayespriortehnique,seee.g.KorostelevandTsybakov(1993),andp erturba
xedLevytripletT
0 =(0; 0 ; 0 )intheinteriorofG s (R; max
)suhthatthep erturbationsremain
inG
s (R;
max ).
8.1 Lower bound for in the ase =0
Fix a p ositive integer j. Let (j)
2 C 1
(R) b e some funtion with supp ort in [0;1℄ satisfying
k (j) k L 2 =1, R (j) (x)e 2 j x d x=0and R jF (j) (u)u 2 j 2
du<1. Certainly,thereareinnitely
manyfuntions (j)
fulllingtheserequirements;thelastprop ertyfollowsforinstane if isthe
seondderivativeofanL 2
-funtion. Intro due thewavelet-likenotation
jk (x):=2 j=2 (j) (2 j x k ); j>0;k=0;:::;2 j 1:
Considerforanyr=(r
k
)2f 1;+1g 2
j
andsome>0thep erturb edLevytripletsT
r =(0; 0 ; r ) with r (x)= 0 (x)+2 j(s+1=2) 2 j X k =1 r k jk (x); x2R :
We note that due to F
jk (0)=0and R e x jk (x)dx=0thetriplet T r
satises themartingale
onditionsuhthat T
r 2G
s
(R;0)holdsforasuÆientlysmallhoieoftheonstant>0.
TheGaussianlikeliho o dratiooftheobservationsundertheprobabilitiesorresp ondingtoT
r 0
and
T
r
underthelawofT
r forsomer;r 0 withr k =r 0 k
forallk exept onek
0 isgivenby (r 0 ;r )=exp Z 1 1 (O r 0 O r )(x)" 1 dW(x) 1 2 Z 1 1 jO r 0 O r )(x)j 2 " 2 dx :
Hene, the Kullbak-Leibler divergene (relative entropy) b etween the two observation mo dels
equals KL(T r 0 jT r )= 1 2 Z 1 1 j(O r 0 O r )(x)j 2 " 2 dx:
ThestandardAssouadLemma(KorostelevandTsybakov1993,Thm. 2.6.4)nowyieldsthelower
b oundfortheriskofanyestimator^of
inf ^ sup T=(0;;)2G s (R;0) E T h Z j^(x) (x)j 2 dx i &2 j k r r 0k 2 L 2 s2 2js ;
providedtheKullbak-LeiblerdivergeneKL(T
r jT
r
)staysuniformlyb oundedbyasmallonstant.
Itremainstodetermineaminimalratefor2 j
!1suhthatthisholdswhenthenoise leveltends
tozero.
Arguinginthesp etraldomainandusingthegeneralestimateje z
1j62jzj,forjzj6Æ andsome
smallÆ>0,togetherwithk'
T;r 0=' T;r k 1 !1for2 j
!1,we obtainforallsuÆientlylargej
KL(T r 0 jT r )= 1 4 " 2 Z 1 1 jF(O r 0 O r )(u)j 2 du 6" 2 Z 1 1 ' T;r (u i) ' T;r 0 (u i) u(u i) 2 du 64" 2 Z 1 1 j' T;r (u i)j 2 T 2 jF( r r 0)(u)j 2 (u 4 +u 2 ) 1 d u ." 2 2 j(2s+1) Z 1 1 jF jk0 (u)j 2 u 4 du =" 2 2 j(2s+5) Z 1 1 jF (j) (v )j 2 v 4 dv : Hene,for2 j(2s+5) s" 2
withasuÆientlylargeonstanttheKullbak-Leiblerdivergeneremains
b oundedandtheasymptotilowerb oundforfollows.
8.2 Lower bound for and in the ase =0
Letusstartwiththelowerb oundfor. Wepro eedasb eforebyp erturbingatripletT
0 =(0; 0 ; 0 )
fromthe interiorof G
s
(R;0),but this timewe only onsider one alternative T
1 =(0; 1 ; 1 ) and
ho ose thep erturbation insuh awaythattheharateristi funtion'
T
(u i)do es nothange
forsmallvalues ofjuj.ForanyÆ>0andU >0put
1 := 0 +Æ; F 1 (u):=F 0
(u) Æi(u i)e u
2
=U 2
; u2R :
Thenthefuntion
1
isreal-valued. Moreover,themartingaleondition(2.3)issatised:
1 +F 1 (0) F 1 (i)= 0 +Æ+F 0 (0) Æ F 0 (i)+0=0: Beause of k (s) 1 (s) 0 k 1 62 Z 1 1 juj s jF( 1 0 )(u)jdu.Æ Z 1 1 juj s+1 e u 2 =U 2 dusÆU s+2
andevenb etter b oundsfork (k ) 1 (k ) 0 k L 2 ,k=0;:::;s,itsuÆes toho ose UsÆ 1=(s+2) small
enough to ensure that T
1
still lies in our nonparametri lass G
s
(R;0). The basi lower b ound
result (KorostelevandTsybakov1993,Prop. 2.2.2)thenyields
inf ^ sup (0;;)2Gs(R;0) E ; [j^ j 2 ℄&Æ 2 ;
providedtheKullbak-Leiblerdivergeneb etweenT
1 andT
0
remainsasymptotiallyb ounded. As
inthelowerb ound pro offorweobtainasymptotially
KL(T 1 jT 0 ) 64" 2 Z 1 1 j' 0;T (u i)j 2 T 2 ji( 1 0 )(u i)+F( 1 0 )(u) F( 1 0 )(i)j 2 (u 4 +u 2 ) 1 du ." 2 Æ 2 Z 1 1 ji(u i)(1 e u 2 =U 2 )j 2 (u 4 +u 2 ) 1 du =" 2 Æ 2 Z 1 1 (1 e v 2 ) 2 U 2 v 2 Udv ." 2 Æ 2 U 1 s" 2 Æ (2s+5)=(s+2) :
ThelatterremainssmallforÆ s" withasmallonstant,whihgivestheasymptoti
lowerb oundfor.
Forthelowerb oundofwep erturb thetripletT
0
leaving
0 and
0
=0xedandputting
F 1 (u):=F 0 (u)+Æe u(u i)=U 2 : Then 1 isreal-valued, 1 0 =F( 1 0
)(i) =Æ andthetriplet T
1 =(0; 0 ; 1 ) satisesthe
martingaleondition. ForU sÆ
1=(s+1)
withasuÆientlysmallonstantthep erturbation
1 lies inG s (R;0)dueto k (s) 1 (s) 0 k 1 .Æ Z 1 1 juj s e u 2 =U 2 dusÆU s+1
and even b etter b ounds for k (k ) 1 (k ) 0 k L 2,
k = 0;:::;s. The Kullbak-Leibler divergene is
asymptotiallyb ounded by KL(T 1 jT 0 )64" 2 Z 1 1 j' 0;T (u i)j 2 T 2 jF( 1 0 )(u) F( 1 0 )(i)j 2 (u 4 +u 2 ) 1 d u ." 2 Æ 2 Z 1 1 j1 e u(u i)=U 2 j 2 (u 4 +u 2 ) 1 du =" 2 Æ 2 Z 1 1 j1 e v 2 +iv =U j 2 (U 4 v 4 +U 2 v 2 ) 1 Udv ." 2 Æ 2 U 3 s" 2 Æ (2s+5)=(s+1)
andweobtaintheasymptotilowerb ound for.
8.3 Lower bound for in the ase >0
The interesting deviation from standard pro ofs of lower b ounds (see e.g. Butuea and Matias
(2005)) for severely ill-p osed problems is that we fae the restrition that F is analyti in a
strip parallelto thereal line andis uniquelyidentiablefromitsvalueson any op enset. So,let
T 0 = ( 2 0 ; 0 ; 0 ) with 0
> 0 b e a Levy triplet fromthe interiorof G
s (R; max ). Consider the p erturbation T 1 =( 2 0 ; 0 ; 1 )with F 1 (u):=F 0 (u)+Æm 1=4 e (T 2 0 u 2 =m) m =2 (T 2 0 =m) m u m (u i) m ; u2R :
form2N,Æ >0. Thenwe haveuniformlyform!1 andÆ !0
k 1 0 k 2 L 2 =2 kF( 1 0 )k 2 L 2 = 2 Æ 2 p T 2 0 Z 1 0 e v v (1+2m)=2m (1+m 1 v 1=m ) m dvsÆ 2 :
Similarly,fork=1;:::;swederiveuniformlyinmandÆ
k (k ) 1 (k ) 0 k L 2 = p 2 ku k F( 1 0 )(u)k L 2 sÆm k =2 ; k (s) 1 (s) 0 k 1 6ku s F( 1 0 )(u)k L 16Æm s=2 1=4 : Thereforeho osingÆsm s=2
withasmallonstantyieldsT
1 2G
s (R;
max
)b eausewethenalso
have that
1
isreal-valuedandT
1
satisesthemartingaleonditionandAssumption1.
By thesameargumentsas b eforeandbyStirling'sformulato estimatethe Gammafuntion,the
Kullbak-Leibler divergene b etween the observations under T
0
and under T
1
KL(T 1 jT 0 )64" 2 Z 1 1 j' 0;T (u i)j 2 T 2 jF( 1 0 )(u)j 2 (u 4 +u 2 ) 1 du ." 2 Æ 2 Z 1 1 e T 2 0 u 2 m 1=2 e (T 2 0 u 2 =m) m (T 2 0 =m) 2m u 2m 2 ju ij 2m 2 du =" 2 Æ 2 m 7=2 (T 2 0 m) 1=2 Z 1 0 e mv 1=m e v v (2m 1)=2m (1+m 1 v 1=m ) m 1 dv ." 2 Æ 2 m 4 Z 1 0 e mv 1=m dv =" 2 Æ 2 m 4 Z 1 0 e z z m 1 m 1 m dz =" 2 Æ 2 m m 3 (m)." 2 Æ 2 m m 3 (m 1) m 1=2 e 1 m s" 2 m 3 s e m
Consequently, theKullbak-Leiblerdivergene remains smallwhen ho osingm>2log(" 1
), but
m . log(" 1
), whih gives Æ s log(" 1
) s=2
. From the basi general lower b ound result we
therefore obtaintheasymptotilowerb oundfor.
8.4 Lower bound for 2
, and in the ase >0
Letusstartwiththelowerb oundfor. Wepro eedasinthease =0byp erturbingthetriplet
T 0 =( 0 ; 0 ; 0 ) with 0
> 0in suh awaythat the harateristi funtion '
T
(u i) do es not
hangemuhforsmallvalues ofjuj. ForanyÆ put
1 := 0 +Æ; F 1 (u):=F 0
(u) Æi(u i)e u 2m =U 2m : Then 1
isreal-valuedandthemartingaleondition(2.3)issatised. Beause of
k (s) 1 (s) 0 k 1 6 Z juj s jF( 1 0 )(u)jdu.Æ Z 1 1 juj s+1 e u 2m =U 2m dusÆU s+2
and smaller b ounds for k (k ) 1 (k ) 0 k L 2, k =0;:::;s, we ho ose U s Æ 1=(s+2) smallenough to
ensure that thep erturb ed tripletT
1
still lies inG
s (R;
max
). In thesamemanner as b efore and
usingj1 e x
j6jxj,x>0,aswellasStirling'sformula,weobtain
KL(T 1 jT 0 )64" 2 Z 1 1 j' 0;T (u i)j 2 T 2 ji( 1 0 )(u i)+ +F( 1 0 )(u) F( 1 0 )(i)j 2 (u 4 +u 2 ) 1 du ." 2 Æ 2 Z 1 1 e T 2 0 u 2 ji(u i)(1 e u 2m =(2U 2m ) )j 2 (u 4 +u 2 ) 1 du ." 2 Æ 2 Z 1 1 e T 2 0 u 2 u 4m U 4m u 2 du s" 2 Æ 2 U 4m (2m 1 2 ) s" 2 Æ 2+4m=(s+2) (2m) 2m e 2m
TokeeptheKullbak-Leiblerdivergenesmall,weho ose
Æ (2s+4m+4)=(s+2) s" 2 (2m) 2m e 2m
andthusobtainuniformlyoverm theb ound
inf ^ sup T=( 2 ;;)2G s (R; max ) E T [j^ j 2 ℄ 1=2 & " 2 (2m) 2m e 2m (s+2)=(2s+4m+4) :
Themaximizerof thisexpressionm slog(" )then yieldstheasymptotilowerb oundfor.
Forwe p erturbthetripletT
0
leaving
0 and
0
xedandputtingforanevenintegerm
F 1 (u):=F 0 (u)+Æe u m (u i) m =U 2m : Then 1 0 =F( 1 0
)(i)=ÆandthetripletT
1 =( 0 ; 0 ; 1
)satisesthemartingaleondition.
ForU sÆ
1=(s+1)
with asuÆientlysmallonstant thep erturbation
1 liesinG s (R; max ). As
b eforewe provethat theKullbak-Leiblerdivergeneremainsb oundedwhenever
Æ (2s+4m+2)=(s+1) s" 2 (2m) 2m+1 e 2m : Cho osingm slog(" 1
)as b eforegivestheasymptotilower b oundfor.
For 2
we p erturbthetripletT
0
leaving
0
invariantandputting
2 1 := 2 0 +2Æ; F 1 (u):=F 0 (u)+Æ(u i) 2 e u 2m =U 2m :
Thenthemartingaleondition(2.3)issatisedandforU sÆ
1=(s+3)
suÆientlysmallweremain
inG
s (R;
max
). ItisagainroutinetoprovethattheKullbak-Leiblerdivergeneremainsb ounded
whenever Æ (2s+4m+6)=(s+3) s" 2 (2m) 2m 1 e 2m : Cho osingm
as b eforegivestheasymptotilowerb oundfor 2
.
9 Appendix
9.1 Proof of Proposition 2.1
(a) This followsfromtheput-allparity(2.4).
(b) O (x)>0followsdiretly from(2.6)whileO (x)6E[e XT ℄ (1 e x ) + =1^e x followsfrom
(a) andthemartingaleondition.
() Weonlude byHolder'sandMarkov'sinequalityforx>0
O (x)6E[e X 1 fX>xg ℄6C 1= P(X >x) ( 1)= 6C 1= C e x ( 1)= =C e (1 )x : (d) Letusdenotebyf T
thedensityoftheabsolutelyontinuouspartofthedistributionofX
T .
TheonlyatominthedistributionofX
T
ano ur atT, namelyintheomp oundPoisson
ase whennojumpuntilT hastakenplae. For x6=0wehave
O 0 (x)= E[(e XT e x )1 fX T >xg ℄ 0 +e x 1 fx<0g =e x P(X T >x)+1 fx<0g : (9.1) This yieldsO 0 (0+) O 0
(0 )= 1andinthease =0,<1,6=0also
O 0 (T+) O 0 (T )=e T P(X T =T)=e ( )T :
Atallp ointsx6=0wherethelawof X
T
hasnoatomwe obtain
O 00 (x)= e x P(X T >x) 0 +e x 1 fx<0g =e x P(X T <x)+f T (x) 1 fx>0g :
Consequently,bypartialintegrationandusingE[e XT ℄=1we arriveat Z Rnf0;Tg jO 00 (x)jdx=O 0 (0 )+ Z 1 0 e x P(X T <x) 1+f T (x) dx 6P(X T <0)+ Z 1 0 e x (1 P(X T <x))dx+E 1 fXT>0g e XT =2P(X T <0) 1+2E 1 fX T >0g e XT 61+2E[e XT ℄=3:
FO (v )=S 1 Z 0 1 e iv x P T (x)dx+ Z 1 0 e iv x C T (x)dx = Z 0 1 e iv x E 1 fX T 6xg (e x e XT ) dx+ Z 1 0 e iv x E 1 fX T >xg (e XT e x ) dx:
By partialintegrationweobtain
Z 0 1 e (iv +1)x P(X T 6x)dx= 1 1+iv P(X T 60) 1 1+iv E 1 fX T 60g e (1+iv )XT ; Z 0 1 e iv x E 1 fXT6xg e XT dx= 1 iv E 1 fXT60g e XT 1 iv E 1 fXT60g e (1+iv )XT and onsequently Z 0 1 e iv x E 1 fXT6xg (e x e XT ) dx= 1 1+iv P(X T 60) 1 1+iv E 1 fXT60g e (1+iv )XT 1 iv E 1 fX T 60g e X T + 1 iv E 1 fX T 60g e (1+iv )X T :
Inthesamewaywe derive
Z 1 0 e iv x E 1 fXT>xg (e X T e x ) dx= 1 iv E 1 fXT>0g e X T + 1 iv E 1 fXT>0g e (1+iv )X T + 1 1+iv P(X T >0) 1 1+iv E 1 fXT>0g e (1+iv )XT :
TakingintoaountE[e X
T
℄=1,weobtainformula(2.7).
9.2 Proof of Proposition 5.1
We only sketh the main steps in the pro of, the reasoning b eing similar to that for frational
derivatives, f. Samko,Kilbas,and Marihev (1993). The followingformulais easilyestablished
andloselyrelatedtoequation(5.8)inSamko,Kilbas,andMarihev(1993):
F( (x)x 1 )(u)= (2 )sin( =2) i Z 1 0 z 2 F (u+z) F (u z) dz:
Letusonlyonsidertheaseu>0andset
G u (x):= 1 (s 1)! Z x 0 (x ) s 1 F (u+)d +2 1 ( 1; u℄ (x) s 1 X k =0 (k ) (0) ( i) k (u+x) s k 1 (s k 1)!k !
Thenwehaveinadistributionalsense
G (k ) u (0)=0; k=0;:::;s 1; G (s) u (x)=F (u+x)+2 s 1 X k =0 (k ) (0) ( i) k Æ (k ) u (x) k ! :
Hene, bys-foldpartialintegrationweobtain
Z 1 0 z 2 F (u+z) F (u z) dz 2 s 1 X k =0 (k ) (0)i k 2 k u 2 k = Z 1 0 z 2 G (s) u (z) G (s) u ( z) dz= s Y k =1 (k+1 ) Z 1 0 G u (z) ( 1) s G u ( z) z s+2 dz:
It therefore suÆes to show that the last integral is of order juj
s min(1;2 )
, whih is
aom-plishedbysplitting theintegrationintervalintotheparts [0;1℄,[1;u℄and[u;1)andmakinguse
ofjF
(u)j.(1+juj) s 1
and oftheprop erties ofG
u
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