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TRANSCRIPT
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Itos formula for fractional Brownian motion
and fractional Bessel processes
Joao Guerra (Departamento de Matematica, ISEG, UTL)
ENSPM, June 23, 2006
Its formula for fBm and fractional Bessel processes
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Fractional Brownian motion
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Fractional Brownian motion
fractional Brownian motion (fBm) is a centered Gaussian process BH =
BHt t0 with covarianceRH(s, t) =
1
2
t2H+ s2H |t s|
2H
, (1)
H (0, 1).
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Fractional Brownian motion
fractional Brownian motion (fBm) is a centered Gaussian process BH =
BHt t0 with covarianceRH(s, t) =
1
2
t2H+ s2H |t s|
2H
, (1)
H (0, 1).
1. BH has Holder continuous paths with < H.
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Fractional Brownian motion
fractional Brownian motion (fBm) is a centered Gaussian process BH =
BHt t0 with covarianceRH(s, t) =
1
2
t2H+ s2H |t s|
2H
, (1)
H (0, 1).
1. BH has Holder continuous paths with < H.
2. IfH = 1/2 then BH has dependent increments.
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Fractional Brownian motion
fractional Brownian motion (fBm) is a centered Gaussian process BH =
BHt t0 with covarianceRH(s, t) =
1
2
t2H+ s2H |t s|
2H
, (1)
H (0, 1).
1. BH has Holder continuous paths with < H.
2. IfH = 1/2 then BH has dependent increments.
Its formula for fBm and fractional Bessel processes 1
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3. BH is self-similar.
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3. BH is self-similar.
4. BH exhibits long range dependence if H > 12.
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3. BH is self-similar.
4. BH exhibits long range dependence if H > 12.
5. IfH = 1/2 then BH is not a semimartingale =There is no Ito integralfor BH.
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3. BH is self-similar.
4. BH exhibits long range dependence if H > 12.
5. IfH = 1/2 then BH is not a semimartingale =There is no Ito integralfor BH.
H = 0.2
Its formula for fBm and fractional Bessel processes 2
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H = 0.5
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H = 0.5
Its formula for fBm and fractional Bessel processes 3
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H = 0.7
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H = 0.7
p-variation properties:
n1k=0
BHtnk+1
BHtnk
p L1()
if p < 1HTE
BH1 1/H if p = 1H0 if p > 1H
Its formula for fBm and fractional Bessel processes 4
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Malliavin calculus for fBm
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Malliavin calculus for fBm
H 12, 1
. Hilbert space H:
1[0,t],
1[0,s]
H = RH(t, s).
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Malliavin calculus for fBm
H 12, 1
. Hilbert space H:
1[0,t],
1[0,s]
H = RH(t, s).
The map 1[0,t] BHt can be extended to an isometry between H and
the Gaussian space G:
E
BHt BHs
=1[0,t],1[0,s]
H
. (2)
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Malliavin calculus for fBm
H 12, 1
. Hilbert space H:
1[0,t],
1[0,s]
H = RH(t, s).
The map 1[0,t] BHt can be extended to an isometry between H and
the Gaussian space G:
E
BHt BHs
=1[0,t],1[0,s]
H
. (2)
Its formula for fBm and fractional Bessel processes 5
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Wiener integral ( H): BH() = T
0dBH
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Wiener integral ( H): BH() = T
0dBH
|H|-Function space:
2|H| := H
T
0 T
0
|r| |u| |r u|2H2 drdu < .
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Wiener integral ( H): BH() = T
0dBH
|H|-Function space:
2|H| := H
T
0 T
0
|r| |u| |r u|2H2 drdu < .
S: random variables of the form
F = f
BH(1), . . . , BH(n)
, n 1, f Cb (Rn) ei H.
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Wiener integral ( H): BH() = T
0dBH
|H|-Function space:
2|H| := H
T
0 T
0
|r| |u| |r u|2H2 drdu < .
S: random variables of the form
F = f
BH(1), . . . , BH(n)
, n 1, f Cb (Rn) ei H.
Its formula for fBm and fractional Bessel processes 6
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Malliavin derivative in S (with values in H)
DF :=ni=1
f
xi
BH(1), . . . , B
H(n)
i. (3)
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Malliavin derivative in S (with values in H)
DF :=ni=1
f
xi
BH(1), . . . , B
H(n)
i. (3)
D1,2
: closure of S w.r.t. the norm
F21,2 := E
|F|2
+ E
DF2H
.
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Malliavin derivative in S (with values in H)
DF :=ni=1
f
xi
BH(1), . . . , B
H(n)
i. (3)
D1,2
: closure of S w.r.t. the norm
F21,2 := E
|F|2
+ E
DF2H
.
Divergence operator is the adjoint operator of D:
E [F (u)] = E [DF,uH] , u L2 (; H) (4)
Its formula for fBm and fractional Bessel processes 7
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Dom() is the set of random variables (processes). u L2 (; H) such
that |E
DF,uH| c F2, F S.
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Dom() is the set of random variables (processes). u L2 (; H) such
that |E
DF,uH| c F2, F S.
D1,2(H) Dom() e
E
(u)2
= E
u2H
+ E
Du, (Du)HH
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Dom() is the set of random variables (processes). u L2 (; H) such
that |E
DF,uH| c F2, F S.
D1,2(H) Dom() e
E
(u)2
= E
u2H
+ E
Du, (Du)HH
Integration by parts formula: F D1,2 and u Dom():
(F u) = F (u) DF,uH
Its formula for fBm and fractional Bessel processes 8
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Relationship between and the pathwise integral:
T0
utdBHt = (u) + H
T0
T0
Dsut |t s|2H2 dsdt (5)
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Relationship between and the pathwise integral:
T0
utdBHt = (u) + H
T0
T0
Dsut |t s|2H2 dsdt (5)
L1,pH : processes u D1,p(|H| ) such that
upL1,pH
:= E
up
L1/H([0,T])+ E
Dup
L1/H([0,T]2)
< .
Estimate: (u)pp Cp up
L1,pH
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Relationship between and the pathwise integral:
T0
utdBHt = (u) + H
T0
T0
Dsut |t s|2H2 dsdt (5)
L1,pH : processes u D1,p(|H| ) such that
upL1,pH
:= E
up
L1/H([0,T])+ E
Dup
L1/H([0,T]2)
< .
Estimate: (u)pp Cp up
L1,pH
Its formula for fBm and fractional Bessel processes 9
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Let u L1,pH , with p >1H and
T0
|E [us]|p ds +
T0
E
T0
|Dsur|1/Hds
pHdr < .
Then0 usBHs is -Holder continuous if < H 1/p.
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Let u L1,pH , with p >1H and
T0
|E [us]|p ds +
T0
E
T0
|Dsur|1/Hds
pHdr < .
Then0 usBHs is -Holder continuous if < H 1/p.
Theorem 1. Let u L1,1/HH . Then
n1i=0
tni+1
tni
usBHspL1()
n CHT0
|us|1/Hds,
Its formula for fBm and fractional Bessel processes 10
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Itos formula
F of class C2 and H > 12 =t0
F(BHs )ds (Riemann-Stieltjes) existsand
F
BHt
= F(0) +t0
F(BHs )dBHs . (6)
F
BHt
t[0,T] D1,2 (|H|) and
t
0
F(BHs )dBHs =
t
0
F(BHs )BHs + H
t
0
F(BHs )s2H1ds (7)
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Itos formula
F of class C2 and H > 12 =t0
F(BHs )ds (Riemann-Stieltjes) existsand
F
BHt
= F(0) +t0
F(BHs )dBHs . (6)
F
BHt
t[0,T] D1,2 (|H|) and
t
0
F(BHs )dBHs =
t
0
F(BHs )BHs + H
t
0
F(BHs )s2H1ds (7)
Its formula for fBm and fractional Bessel processes 11
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Theorem 2. If F is of class C2 and maxxR
{|F(x)| , |F(x)| , |F(x)|}
c exp
x2
then (Itos formula):
F(BHt ) = F(0) +
t0
F(BHs )BHs + H
t0
F(BHs )s2H1ds (8)
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Theorem 2. If F is of class C2 and maxxR
{|F(x)| , |F(x)| , |F(x)|}
c exp
x2
then (Itos formula):
F(BHt ) = F(0) +
t0
F(BHs )BHs + H
t0
F(BHs )s2H1ds (8)
Multidimensional Itos formula (BH-d-dimensional fBm ):
FBHt = F (0)+d
i=1
t
0
F
xi(BHs )B
(i)s +H
d
i=1
t
0
2F
x2i
(BHs )s2H1ds.
(9)
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Fractional Bessel processes
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Fractional Bessel processes
d 2, H (1/2, 1), d-dimensional fBm:
BH =
BHtt[0,T]
=
B(1)t , . . . , B
(d)t
t[0,T]
Fractional Bessel processes:
Rt :=BHt = B(1)t 2 + . . . + B(d)t 2, (10)
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Fractional Bessel processes
d 2, H (1/2, 1), d-dimensional fBm:
BH =
BHtt[0,T]
=
B(1)t , . . . , B
(d)t
t[0,T]
Fractional Bessel processes:
Rt :=BHt = B(1)t 2 + . . . + B(d)t 2, (10)
Its formula for fBm and fractional Bessel processes 13
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Theorem 3. B(i)sRs
L1,1/HH,i for each i = 1, . . . , d and we have the repre-
sentation
Rt =di=1
t0
B(i)s
RsB(i)s + H(d 1)
t0
s2H1
Rsds. (11)
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Theorem 3. B(i)sRs
L1,1/HH,i for each i = 1, . . . , d and we have the repre-
sentation
Rt =di=1
t0
B(i)s
RsB(i)s + H(d 1)
t0
s2H1
Rsds. (11)
Analogous representation for standard Brownian motion:
RWt =di=1
t0
W(i)s
RWsdW(i)s +
1
2(d 1)
t0
1
Rsds (12)
and the process Wt :=
di=1
t0W
(i)sRs
dW(i)s
t[0,T]
is a one dimensional
standard Brownian motion
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Theorem 3. B(i)sRs
L1,1/HH,i for each i = 1, . . . , d and we have the repre-
sentation
Rt =di=1
t0
B(i)s
RsB(i)s + H(d 1)
t0
s2H1
Rsds. (11)
Analogous representation for standard Brownian motion:
RWt =di=1
t0
W(i)s
RWsdW(i)s +
1
2(d 1)
t0
1
Rsds (12)
and the process Wt :=
di=1
t0W
(i)sRs
dW(i)s
t[0,T]
is a one dimensional
standard Brownian motion
Its formula for fBm and fractional Bessel processes 14
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Is Ht := di=1 t
0B(i)sRs
B(i)s a fBm?
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Is Ht := di=1
t
0B(i)sRs
B(i)s a fBm?
1. Ht is self-similar2. Ht has finite 1/H-variation as fBm.
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Is Ht := di=1
t
0B(i)sRs
B(i)s a fBm?
1. Ht is self-similar2. Ht has finite 1/H-variation as fBm.
Partial results:
1. If 12 < H 12, then Ht is not a B-adapted fBm.
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Is Ht := di=1
t
0B(i)sRs
B(i)s a fBm?
1. Ht is self-similar2. Ht has finite 1/H-variation as fBm.
Partial results:
1. If 12 < H 12, then Ht is not a B-adapted fBm.
Its formula for fBm and fractional Bessel processes 15
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References
[1] E. Alos and D. Nualart, Stochastic integration with respect to the frac-tional Brownian motion, Stochastics and Stoch. Reports, 75 (2003),129-152.
[2] J. M. E. Guerra and D. Nualart, The 1/H-variation of the divergenceintegral with respect to the fractional Brownian motion for H>1/2and fractional Bessel processes, Stochastic Processes and their Appli-cations, 115 (2005), 91-115.
[3] Y. Hu and D. Nualart, Some processes associated with fractional Bessel
Processes, J. Theoretical Probability 18 (2005), 377-397.
Its formula for fBm and fractional Bessel processes 16