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Assessinglongmemorycharacteristicsofenergyprices
11
Usingproperties(1)and(3)GrangerandJoyeux
4andHosking5haveshown
thatlongmemoryprocesscanbedescribedparametricallybyfractionallyinte-
gratedprocess:
(1L)
d(y
t
μ
)=
μ
t,
(5)
whereL
ky
t=yt
kisalagoperator,disafractionaldifferenceparameter(d>1),
μ
istheexpectedvalueofyt,utisastationaryprocesswithshortmemoryand
E(ut)=0,
(
1
L
)
d
=
k
=
0
d
k
(
1
)
k
L
k
isafractionaldifferencefilter,
d
k
=
k
!
(
d
d
!
k
)
!
=
Γ
(
k
+
Γ
1
)
(
Γ
d
(
+
d
1
)
k
+
1
)
.
If|d|>1/2thenytisnon-stationary.If0<d<1/2thenytisstationaryand
haslongmemory.If1/2<d<0thenytisstationaryandhasshortmemory.Of-
tentheHurstcoefficientisusedinsteadofdinequation(5)followingtherela-
tion:
d=H1/2.
(6)
Henceif0<HorH>1thenytisnonstationary.If1/2<H<1thenytissta-
tionaryandhaslongmemorysothetimeseriesischaracterizedbypositiveauto-
correlationandsmallrisk,becausethereisahighprobability,thattrenddirection
willnotbechanged.If0<H<1/2thenytisstationaryandhasshortmemory,
timeseriesischaracterizedbynonpositiveautocorrelation,andsmallrisk,be-
causeytwillreactonnewinformationfromthemarket.IfH=0.5thenytis
arandomprocess(forexampleWiener,sprocessorrandomwalk)
6.
4C.W.J.Granger,R.Joyeux:AnIntroductiontoLong-MemoryTimeSeriesModelsand
FractionalDifferencing."JournalofTimeSeriesAnalysis”1980,No.1,p.15-29.
5J.R.M.Hosking:FractionalDifferencing."Biometrika”1981,No.68,p.165-176.
6J.Stawicki,I.Frączek-Miller:żnicowaniefraktalneszeregówczasowych.W:Dynamiczne
modeleekonometryczne.MateriałynaVOgólnopolskieSeminariumNaukowe.TNOiK„DomOr-
ganizatora”,Toruń1997.