spmeng

Upload: joao-guerra

Post on 03-Apr-2018

215 views

Category:

Documents


0 download

TRANSCRIPT

  • 7/28/2019 spmeng

    1/52

    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

  • 7/28/2019 spmeng

    2/52

    Fractional Brownian motion

  • 7/28/2019 spmeng

    3/52

    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).

  • 7/28/2019 spmeng

    4/52

    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.

  • 7/28/2019 spmeng

    5/52

    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.

  • 7/28/2019 spmeng

    6/52

    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

  • 7/28/2019 spmeng

    7/52

    3. BH is self-similar.

  • 7/28/2019 spmeng

    8/52

    3. BH is self-similar.

    4. BH exhibits long range dependence if H > 12.

  • 7/28/2019 spmeng

    9/52

    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.

  • 7/28/2019 spmeng

    10/52

    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

  • 7/28/2019 spmeng

    11/52

  • 7/28/2019 spmeng

    12/52

    H = 0.5

  • 7/28/2019 spmeng

    13/52

    H = 0.5

    Its formula for fBm and fractional Bessel processes 3

  • 7/28/2019 spmeng

    14/52

    H = 0.7

  • 7/28/2019 spmeng

    15/52

    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

  • 7/28/2019 spmeng

    16/52

    Malliavin calculus for fBm

  • 7/28/2019 spmeng

    17/52

    Malliavin calculus for fBm

    H 12, 1

    . Hilbert space H:

    1[0,t],

    1[0,s]

    H = RH(t, s).

  • 7/28/2019 spmeng

    18/52

    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)

  • 7/28/2019 spmeng

    19/52

    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

  • 7/28/2019 spmeng

    20/52

    Wiener integral ( H): BH() = T

    0dBH

  • 7/28/2019 spmeng

    21/52

    Wiener integral ( H): BH() = T

    0dBH

    |H|-Function space:

    2|H| := H

    T

    0 T

    0

    |r| |u| |r u|2H2 drdu < .

  • 7/28/2019 spmeng

    22/52

    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.

  • 7/28/2019 spmeng

    23/52

    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

  • 7/28/2019 spmeng

    24/52

    Malliavin derivative in S (with values in H)

    DF :=ni=1

    f

    xi

    BH(1), . . . , B

    H(n)

    i. (3)

  • 7/28/2019 spmeng

    25/52

    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

    .

  • 7/28/2019 spmeng

    26/52

    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

  • 7/28/2019 spmeng

    27/52

    Dom() is the set of random variables (processes). u L2 (; H) such

    that |E

    DF,uH| c F2, F S.

  • 7/28/2019 spmeng

    28/52

    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

  • 7/28/2019 spmeng

    29/52

    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

  • 7/28/2019 spmeng

    30/52

    Relationship between and the pathwise integral:

    T0

    utdBHt = (u) + H

    T0

    T0

    Dsut |t s|2H2 dsdt (5)

  • 7/28/2019 spmeng

    31/52

    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

  • 7/28/2019 spmeng

    32/52

    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

  • 7/28/2019 spmeng

    33/52

    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.

  • 7/28/2019 spmeng

    34/52

    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

  • 7/28/2019 spmeng

    35/52

  • 7/28/2019 spmeng

    36/52

  • 7/28/2019 spmeng

    37/52

    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)

  • 7/28/2019 spmeng

    38/52

    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

  • 7/28/2019 spmeng

    39/52

    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)

  • 7/28/2019 spmeng

    40/52

    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)

  • 7/28/2019 spmeng

    41/52

  • 7/28/2019 spmeng

    42/52

    Fractional Bessel processes

  • 7/28/2019 spmeng

    43/52

    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)

  • 7/28/2019 spmeng

    44/52

    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

  • 7/28/2019 spmeng

    45/52

    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)

  • 7/28/2019 spmeng

    46/52

    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

  • 7/28/2019 spmeng

    47/52

    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

  • 7/28/2019 spmeng

    48/52

    Is Ht := di=1 t

    0B(i)sRs

    B(i)s a fBm?

  • 7/28/2019 spmeng

    49/52

    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.

  • 7/28/2019 spmeng

    50/52

    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.

  • 7/28/2019 spmeng

    51/52

    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

  • 7/28/2019 spmeng

    52/52

    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