Chapter 18

Itô’s formula

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Problem 18.1

Let (Bt)t⩾0\left(B_{t}\right)_{t \geqslant 0} be BM1B M^{1}. Use Itô's formula to obtain representations of

Xt=∫0texp⁡(Bs)dBs and Yt=∫0tBsexp⁡(Bs2)dBs X_{t} = \int _{0}^{t} \exp \left(B_{s}\right) d B_{s} \quad \text{ and } \quad Y_{t} = \int _{0}^{t} B_{s} \exp \left(B_{s}^{2}\right) d B_{s}

which do not contain Itô integrals.

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Problem 18.2

Let Π={0=t0<t1<⋯<tN=T}\Pi = \left\{ 0 = t_{0} < t_{1} < \cdots < t_{N} = T\right\} be a generic partition of the interval [0,T][0, T] and denote by ∣Π∣=max⁡j∣tj−tj−1∣\left|\Pi \right| = \max_{j}\left|t_{j} - t_{j - 1}\right| the mesh of the partition. Show that the limit

lim⁡∣Π∣→0∑j=1N(tj−tj−1)y \lim _{\left|\Pi \right| \rightarrow 0} \sum _{j = 1}^{N}\left(t_{j} - t_{j - 1}\right)^{y}

is ∞,T\infty , T or 0 according to γ<1,γ=1\gamma < 1, \gamma = 1 or γ>1\gamma > 1.

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Problem 18.3

Show that the limits (18.5) and (18.6) actually hold in L2(P)L^{2}(\mathbb {P}) and uniformly for TT from compact sets.

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Problem 18.4

Give a direct proof for the identity

E[(∑l=1Ng(Btl−1)[(Btl−Btl−1)2−(tl−tl−1)])2]=E[∑l=1N∣g(Btl−1)∣2[(Btl−Btl−1)2−(tl−tl−1)]2]. \begin{aligned} \mathbb {E} & {\left[\left(\sum _{l = 1}^{N} g\left(B_{t_{l - 1}}\right)\left[\left(B_{t_{l}} - B_{t_{l - 1}}\right)^{2} - \left(t_{l} - t_{l - 1}\right)\right]\right)^{2}\right] } \\ & = \mathbb {E}\left[\sum _{l = 1}^{N}\left|g\left(B_{t_{l - 1}}\right)\right|^{2}\left[\left(B_{t_{l}} - B_{t_{l - 1}}\right)^{2} - \left(t_{l} - t_{l - 1}\right)\right]^{2}\right] . \end{aligned}

appearing in the proof of Lemma 18.4.

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Problem 18.5

The following exercise contains an alternative proof of Itô's formula (18.1) for a one - dimensional Brownian motion (Bt)t⩾0\left(B_{t}\right)_{t \geqslant 0}.

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(a)

Let f∈C1(R)f \in \mathcal{C}^{1}(\mathbb {R}). Show that for Π={t0=0<t1<⋯<tn=t}\Pi = \left\{ t_{0} = 0 < t_{1} < \cdots < t_{n} = t\right\} and suitable intermediate values ξl\xi_{l}

Btf(Bt)=∑lBtl(f(Btl)−f(Btl−1))+∑lf(Btl−1)(Btl−Btl−1)+∑lf′(ξl)(Btl−Btl−1)2. \begin{gathered} B_{t} f\left(B_{t}\right) = \sum _{l} B_{t_{l}}\left(f\left(B_{t_{l}}\right) - f\left(B_{t_{l - 1}}\right)\right)+\sum _{l} f\left(B_{t_{l - 1}}\right)\left(B_{t_{l}} - B_{t_{l - 1}}\right) \\ +\sum _{l} f^{\prime }\left(\xi _{l}\right)\left(B_{t_{l}} - B_{t_{l - 1}}\right)^{2} . \end{gathered}

Conclude from this that the differential expression Btdf(Bt)B_{t} d f\left(B_{t}\right) is well - defined.

(b)

Show that d(Btf(Bt))=Btdf(Bt)+f(Bt)dBt+f′(Bt)dtd\left(B_{t} f\left(B_{t}\right)\right) = B_{t} d f\left(B_{t}\right)+f\left(B_{t}\right) d B_{t}+f^{\prime }\left(B_{t}\right) d t.

(c)

Use (b) to find a formula for dBtn,n⩾2d B_{t}^{n}, n \geqslant 2, and show that for every polynomial p(x)p(x) Itô's formula holds:

dp(Bt)=p′(Bt)dBt+12p′′(Bt)dt. d p\left(B_{t}\right) = p^{\prime }\left(B_{t}\right) d B_{t}+\frac{1}{2} p^{\prime \prime }\left(B_{t}\right) d t .
(d)

Show the following stability result for Itô integrals:

L2(P)−lim⁡n→∞∫0Tgn(s)dBs=∫0Tg(s)dBs L^{2}(\mathbb {P}) - \lim _{n \rightarrow \infty } \int _{0}^{T} g_{n}(s) d B_{s} = \int _{0}^{T} g(s) d B_{s}

for any sequence (gn)n⩾1\left(g_{n}\right)_{n \geqslant 1} which converges in LT2\mathcal{L}_{T}^{2}.

(e)

Use a suitable version of Weierstraß' approximation theorem and the stopping technique from the proof of Theorem 18.1, Step 4∘4^{\circ }, to deduce from c) Itô's formula for f∈C2f \in \mathcal{C}^{2}.

Problem 18.6
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(a)

Use the (two - dimensional, deterministic) chain rule d(F∘G)=F′∘GdGd(F \circ G) = F^{\prime } \circ G d G to deduce the formula for integration by parts for Stieltjes integrals:

∫0tf(s)dg(s)=f(t)g(t)−f(0)g(0)−∫0tg(s)df(s) for all f,g∈C1([0,∞),R) \int _{0}^{t} f(s) d g(s) = f(t) g(t) - f(0) g(0) - \int _{0}^{t} g(s) d f(s) \quad \text{ for all } f, g \in \mathcal{C}^{1}([0, \infty ), \mathbb {R})
(b)

Use the Itô formula for a Brownian motion (bt,βt)t⩾0\left(b_{t}, \beta_{t}\right)_{t \geqslant 0} in R2\mathbb {R}^{2} to show that

∫0tbsdβs=btβt−∫0tβsdbs,t⩾0 \int _{0}^{t} b_{s} d \beta _{s} = b_{t} \beta _{t} - \int _{0}^{t} \beta _{s} d b_{s}, \quad t \geqslant 0

What happens if bb and β\beta are not independent?

Problem 18.7

Prove the following time - dependent version of Itô's formula: let (Bt)t⩾0\left(B_{t}\right)_{t \geqslant 0} be a BM1\mathrm{BM}^{1} and f:[0,∞)×R→Rf:[0, \infty ) \times \mathbb {R} \rightarrow \mathbb {R} be a function of class C1,2\mathcal{C}^{1,2}. Then

f(t,Bt)−f(0,0)=∫0t∂f∂x(s,Bs)dBs+∫0t(∂f∂t(s,Bs)+12∂2f∂x2(s,Bs))ds. f\left(t, B_{t}\right) - f(0,0) = \int _{0}^{t} \frac{\partial f}{\partial x}\left(s, B_{s}\right) d B_{s}+\int _{0}^{t}\left(\frac{\partial f}{\partial t}\left(s, B_{s}\right)+\frac{1}{2} \frac{\partial ^{2} f}{\partial x^{2}}\left(s, B_{s}\right)\right) d s .

Prove and state the dd - dimensional counterpart.

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Problem 18.8

Prove Theorem 5.6 using Itô's formula.

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Problem 18.9

Let (Bt,Ft)t⩾0\left(B_{t}, \mathscr {F}_{t}\right)_{t \geqslant 0} be a BM1\mathrm{BM}^{1}. Use Itô's formula to verify that the following processes are martingales:

Xt=et/2cos⁡Bt and Yt=(Bt+t)exp⁡(−Bt−t/2).  X_{t} = e^{t / 2} \cos B_{t} \quad \text{ and } \quad Y_{t} = \left(B_{t}+t\right) \exp \left( - B_{t} - t / 2\right) \text{. }
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Problem 18.10

Let Bt=(bt,βt),t⩾0B_{t} = \left(b_{t}, \beta_{t}\right), t \geqslant 0 be a BM2\mathrm{BM}^{2} and set rt:=∣Bt∣=bt2+βt2r_{t}: = \left|B_{t}\right| = \sqrt{b_{t}^{2}+\beta_{t}^{2}}.

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(a)

Show that the stochastic integrals ∫0tbs/rsdbs\int_{0}^{t} b_{s} / r_{s} d b_{s} and ∫0tβs/rsdβs\int_{0}^{t} \beta_{s} / r_{s} d \beta_{s} exist.

(b)

Show that Wt:=∫0tbs/rsdbs+∫0tβs/rsdβsW_{t}: = \int_{0}^{t} b_{s} / r_{s} d b_{s}+\int_{0}^{t} \beta_{s} / r_{s} d \beta_{s} is a BM1\mathrm{BM}^{1}.

Problem 18.11

Let Bt=(bt,βt),t⩾0B_{t} = \left(b_{t}, \beta_{t}\right), t \geqslant 0 be a BM2\mathrm{BM}^{2} and f(x+iy)=u(x,y)+iv(x,y),x,y∈Rf(x+i y) = u(x, y)+i v(x, y), x, y \in \mathbb {R}, an analytic function. If ux2+uy2=1u_{x}^{2}+u_{y}^{2} = 1, then (u(bt,βt),v(bt,βt)),t⩾0\left(u\left(b_{t}, \beta_{t}\right), v\left(b_{t}, \beta_{t}\right)\right), t \geqslant 0, is a BM2\mathrm{BM}^{2}.

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Problem 18.12

Show that the dd - dimensional Itô formula remains valid if we replace the real - valued function f:Rd→Rf: \mathbb {R}^{d} \rightarrow \mathbb {R} by a complex function f=u+iv:Rd→Cf = u+i v: \mathbb {R}^{d} \rightarrow \mathbb {C}.

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Problem 18.13

Let χ∈Cc∞(−1,1)\chi \in \mathcal{C}_{c}^{\infty }( - 1,1) with 0⩽χ⩽1,χ(0)=10 \leqslant \chi \leqslant 1, \chi (0) = 1 and ∫χ(x)dx=1\int \chi (x) d x = 1. Set χn(x):=nχ(nx)\chi_{n}(x): = n \chi (n x).

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(a)

Show that supp χn⊂[−1/n,1/n]\chi_{n} \subset [ - 1 / n, 1 / n] and ∫χn(x)dx=1\int \chi_{n}(x) d x = 1.

(b)

Let f∈C(R)f \in \mathcal{C}(\mathbb {R}) and fn:=f⋆χnf_{n}: = f \star \chi_{n}. Show that ∣∂kfn(x)∣⩽nksup⁡y∈B(x,1/n)∣f(y)∣∥∂kχ∥L1\left|\partial^{k} f_{n}(x)\right| \leqslant n^{k} \sup_{y \in \mathbb {B}(x, 1 / n)}\left|f(y)\right|\left\| \partial^{k} \chi \right\|_{L^{1}}.

(c)

Let f∈C(R)f \in \mathcal{C}(\mathbb {R}) uniformly continuous. Show that lim⁡n→∞∥f⋆χn−f∥∞=0\lim_{n \rightarrow \infty }\left\| f \star \chi_{n} - f\right\|_{\infty } = 0. What can be said if ff is continuous but not uniformly continuous?

(d)

Let ff be piecewise continuous. Show that lim⁡n→∞f⋆χn(x)=f(x)\lim_{n \rightarrow \infty } f \star \chi_{n}(x) = f(x) at all xx where ff is continuous.

Problem 18.14

Show that βt=∫0tsgn⁡(Bs)dBs\beta_{t} = \int_{0}^{t} \operatorname {sgn}\left(B_{s}\right) d B_{s} is a BM1\mathrm{BM}^{1}.

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Problem 18.15

Let (Bt)t⩾0\left(B_{t}\right)_{t \geqslant 0} be a BM1,Φ∈Cb2(R),Φ(0)=0\mathrm{BM}^{1}, \Phi \in \mathcal{C}_{b}^{2}(\mathbb {R}), \Phi (0) = 0 and f,g∈LT2f, g \in \mathcal{L}_{T}^{2} for some T>0T > 0. Show that for all t∈[0,T]t \in [0, T]

E[∫0tf(r)dBr⋅Φ(∫0tg(r)dBr)]=E[∫0tf(s)g(s)Φ′(∫0sg(r)dBr)ds]+12E[∫0t∫0sf(r)dBrΦ′′(∫0sg(r)dBr)g2(s)ds]. \begin{aligned} & \mathbb {E}\left[\int _{0}^{t} f(r) d B_{r} \cdot \Phi \left(\int _{0}^{t} g(r) d B_{r}\right)\right] \\ & = \mathbb {E}\left[\int _{0}^{t} f(s) g(s) \Phi ^{\prime }\left(\int _{0}^{s} g(r) d B_{r}\right) d s\right] \\ & +\frac{1}{2} \mathbb {E}\left[\int _{0}^{t} \int _{0}^{s} f(r) d B_{r} \Phi ^{\prime \prime }\left(\int _{0}^{s} g(r) d B_{r}\right) g^{2}(s) d s\right] . \end{aligned}
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Problem 18.16

Let σΠ,bΠ∈ST\sigma_{\Pi }, b_{\Pi } \in \mathcal{S}_{T} which approximate σ,b∈LT2\sigma , b \in \mathcal{L}_{T}^{2} as ∣Π∣→0\left|\Pi \right| \rightarrow 0, and consider the Itô processes XtΠ=X0+∫0tσΠ(s)dBs+∫0tbΠ(s)dsX_{t}^{\Pi } = X_{0}+\int_{0}^{t} \sigma_{\Pi }(s) d B_{s}+\int_{0}^{t} b_{\Pi }(s) d s and Xt=X0+∫0tσ(s)dBs+∫0tb(s)dsX_{t} = X_{0}+\int_{0}^{t} \sigma (s) d B_{s}+\int_{0}^{t} b(s) d s. Adapt the proof of Lemma 18.5 to show that

∫0Tg(XsΠ)dXsΠ→∣Π∣→0P∫0Tg(Xs)dXs for all g∈Cb(R) \int _{0}^{T} g\left(X_{s}^{\Pi }\right) d X_{s}^{\Pi } \xrightarrow [\left|\Pi \right| \rightarrow 0]{\mathbb {P}} \int _{0}^{T} g\left(X_{s}\right) d X_{s} \quad \text{ for all } g \in \mathcal{C}_{b}(\mathbb {R})
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Problem 18.17

Let Xt=Mt+AtX_{t} = M_{t}+A_{t} and Xt=Mt′+At′X_{t} = M_{t}^{\prime }+A_{t}^{\prime } where M,M′M, M^{\prime } are continuous local martingales and A,A′A, A^{\prime } are continuous processes which have locally a.s. bounded variation. Show that M−M′M - M^{\prime } and A−A′A - A^{\prime } are a.s. constant.

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