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Cheat sheet for math finance, Study notes of Mathematics

Cheat sheet for math finance With many formulas and some descriptions.

Typology: Study notes

2019/2020

Uploaded on 06/13/2022

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zi-wang 🇺🇸

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Download Cheat sheet for math finance and more Study notes Mathematics in PDF only on Docsity! MATHEMATICAL FINANCE CHEAT SHEET Normal Random Variables A random variable X is Normal N(µ,σ2) (aka. Gaussian) under a measure P if and only if EP  e θX  = e θµ+ 1 2 θ 2σ2 , for all real θ . A standard normal Z ∼N(0, 1) under a measure P has density φ(x ) = 1 p 2π e −x 2/2. P[Z ≤ x ] =Φ(x ) := ∫ x −∞ φ(z )d z . Let X = (X1, X2, . . . , Xn )′ with X i ∼N(µi , qi i ) and Cov[X i , X j ] = qi j for i , j = 1, . . . , n . We call µ := (µ1, . . . ,µn )′ the mean and Q := (qi j )ni , j=1 the covariance matrix of X . Assume detQ > 0, then X has a multivariate normal distribution if it has the den- sity φ(x ) = 1 p (2π)n detQ exp  − 1 2 (x −µ)′Q−1(x −µ) ‹ , x ∈Rn . We write X ∼ N(µ,Q ) if this is the case. Alternatively, X ∼ N(µ,Q ) under P if and only if EP[e θ ′X ] = exp  θ ′µ+ 1 2 θ ′Qθ ‹ , for all θ ∈Rn . If Z ∼N(0,Q ) and c ∈Rn then X = c ′Z ∼N(0, c ′Q c ). If C ∈Rm×n (i.e., m×n matrix) then X =C Z ∼N(0, C Q C ′) and C Q C ′ is a m ×m covariance matrix. Gaussian Shifts If Z ∼ N(0, 1) under a measure P, h is an integrable function, and c is a constant then EP[e c Z h (Z )] = e c 2/2EP[h (Z + c )]. Let X ∼N(0,Q ), h be a integrable function of x ∈Rn , and c ∈Rn . Then EP[e c ′X h (X )] = e 1 2 c ′Q c EP[h (X + c )]. Correlating Brownian Motions Let (W (t ))t≥0 and (fW (t ))t≥0 be independent Brownian motions. Given a correla- tion coefficient ρ ∈ [−1, 1], define cW (t ) :=ρW (t ) + p 1−ρ2 fW (t ), then (cW (t ))t≥0 is a Brownian motion and E[W (t )cW (t )] =ρt . Identifying Martingales If X t = X (t ) is a diffusion process satisfying d X (t ) =µ(t , X t )d t +σ(t , X t )d W (t ) and EP[( ∫ T 0 σ(s , X s )2 d s )1/2]<∞ (or,σ(t , x )≤ c |x | as |x | →∞), then X is a martingale ⇐⇒ X is driftless (i.e., µ(t )≡ 0 with P-prob. 1). Novikov’s Condition In the case d X (t ) =σ(t )X (t )d W (t ) for someF -previsible process (σ(t ))t≥0, then we have the simpler condition EP – exp ‚ 1 2 ∫ T 0 σ(s )2 d s Œ™ <∞⇒ X is a martingale. Itô’s Formula For X t = X (t ) given by d X (t ) =µ(t )d t +σ(t )d W (t ) and a function g (t , x ) that is twice differentiable in x and once in t . Then for Y (t ) = g (t , X t ), we have d Y (t ) = ∂ g ∂ t (t , X t )d t + ∂ g ∂ x (t , X t )d X t + 1 2 σ(t )2 ∂ 2g ∂ x 2 (t , X t )d t . The Product Rule Given X (t ) and Y (t ) adapted to the same Brownian motion (W (t ))t≥0, d X (t ) =µ(t )d t +σ(t )d W (t ), d Y (t ) = ν(t )d t +ρ(t )d W (t ). Then d (X (t )Y (t )) = X (t )d Y (t ) +Y (t )d X (t ) +d 〈X , Y 〉(t ) ︸ ︷︷ ︸ σ(t )ρ(t )d t . In the other case, if X (t ) and Y (t ) are adapted to two different and independent Brownian motions (W (t ))t≥0 and (fW (t ))t≥0, d X (t ) =µ(t )d t +σ(t )d W (t ), d Y (t ) = ν(t )d t +ρ(t )d fW (t ). Then d (X (t )Y (t )) = X (t )d Y (t ) +Y (t )d X (t ) as d 〈X , Y 〉(t ) = 0. Radon-Nikodým Derivative Given P and Q equivalent measures and a time horizon T , we can define a random variable d Q d P defined on P-possible paths, taking positive real values, such that • EQ[XT ] = EP • d Q d P XT ˜ , for all claims XT knowable by time T , • EQ[X t |Fs ] = ζ −1 s EP [ζt X t |Fs ], for s ≤ t ≤ T , where ζt is the process EP[ d Q d P |Ft ]. Cameron-Martin-Girsanov Theorem If (W (t ))t≥0 is a P-Brownian motion and (γ(t ))t≥0 is anF -previsible process satis- fying the boundedness condition EP ” exp € 1 2 ∫ T 0 γ(t )2 d t Š— <∞, then there exists a measure Q such that: • Q is equivalent to P, • d Q d P = exp ‚ − ∫ T 0 γ(t )d W (t )− 1 2 ∫ T 0 γ(t )2 d t Œ , • fW (t ) :=W (t ) + ∫ t 0 γ(s )d s is a Q-Brownian motion. In other words, W (t ) is a drifting Q-Brownian motion with drift −γ(t ) at time t . Cameron-Martin-Girsanov Converse If (W (t ))t≥0 is a P-Brownian motion, and Q is a measure equivalent to P, then there exists aF -previsible process (γ(t ))t≥0 such that fW (t ) :=W (t ) + ∫ t 0 γ(s )d s is a Q-Brownian motion. That is, W (t ) plus drift γ(t ) is a Q-Brownian motion. Ad- ditionally, d Q d P = exp ‚ − ∫ t 0 γ(t )d W (t )− 1 2 ∫ T 0 γ(t )2 d t Œ . Martingale Representation Theorem Suppose (M (t ))t≥0 is a Q-martingale process whose volatility Æ EQ[M (t )2] = σ(t ) satisfiesσ(t ) 6= 0 for all t (with Q-probability one). Then if (N (t ))t≥0 is any other Q- martingale, there exists anF -previsible process (φ(t ))t≥0 such that ∫ T 0 φ(t )2σ(t )2 d t < ∞ (with Q-prob. one), and N can be written as N (t ) =N (0) + ∫ t 0 φ(s )d M (s ), or in differential form, d N (t ) =φ(t )d M (s ). Further,φ is (essentially) unique. Multidimensional Diffusions, Quadratic Covariation, and Itô’s Formula If X := (X1, X2, . . . , Xn )′ is a n-dimensional diffusion process with form X (t ) = X (0)+ ∫ t 0 µ(s )d s + ∫ t 0 Σ(s )d W (s ), where Σ(t ) ∈Rn×m and W is a m-dimensional Brownian motion. The quadration covariation of the components X i and X j is 〈X i , X j 〉(t ) = ∫ t 0 Σi (s ) ′Σ j (s )d s , or in differential form d 〈X i , X j 〉(t ) = Σi (t )′Σ j (t )d t , where Σi (t ) is the i th column of Σ(t ). The quadratic variation of X i (t ) is 〈X i 〉(t ) = ∫ t 0 Σi (s )′Σi (s )d s . The multi-dimensional Itô formula for Y (t ) = f (t , X1(t ), . . . , Xn (t )) is d Y (t ) = ∂ f ∂ t (t , X1(t ), . . . , Xn (t ))d t + n ∑ i=1 ∂ f ∂ xi (t , X1(t ), . . . , Xn (t ))d X i (t ) + 1 2 n ∑ i , j =1 ∂ 2 f ∂ xi ∂ x j (t , X1(t ), . . . , Xn (t ))d 〈X i , X j 〉(t ). The (vector-valued) multi-dimensional Itô formula for Y (t ) = f (t , X (t )) = ( f1(t , X (t )), . . . , fn (t , X (t )))′ where fk (t , X ) = fk (t , X1, . . . , Xn )and Y (t ) = (Y1(t ), Y2(t ), . . . , Yn (t ))′ is given component- wise (for k = 1, . . . , n) as d Yk (t ) = ∂ fk (t , X (t )) ∂ t d t + n ∑ i=1 ∂ fk (t , X (t )) ∂ xi d X i (t ) + 1 2 n ∑ i , j =1 ∂ 2 fk (t , X (t )) ∂ xi ∂ x j d 〈X i , X j 〉(t ). Stochastic Exponential The stochastic exponential of X is Et (X ) = exp(X (t )− 1 2 〈X 〉(t )). It satisfies E (0) = 1, E (X )E (Y ) = E (X +Y )e 〈X ,Y 〉, E (X )−1 = E (−X )e 〈X ,X 〉. The process Z = E (X ) is a positive process and solves the SDE d Z = Z d X , Z (0) = e X (0). Solving Linear ODEs The linear ordinary differential equation d z (t ) d t =m (t ) +µ(t )z (t ), z (a ) = ζ, for a ≤ t ≤ b has solution given by z (t ) = ζεt + ∫ t a εt ε −1 u m (u )d u , εt := exp ∫ t a µ(u )d u  , = ζexp € ∫ t a µ(u )d u Š + ∫ t a m (u )exp € ∫ t u µ(r )d r Š d u . Solving Linear SDEs The linear stochastic differential equation d Z (t ) = [m (t ) +µ(t )Z (t )]d t + [q (t ) +σ(t )Z (t )]d W (t ), Z (a ) = ζ, for a ≤ t ≤ b has solution given by Z (t ) = ζEt + ∫ t a Et E−1 u [m (u )−q (u )σ(u )]d u + ∫ t a Et E−1 u q (u )d W (u ), where Et := Et (X ) and X (t ) = ∫ t a µ(u )d u + ∫ t a σ(u )d W (u ). In other words, Et = exp ∫ t a µ(u )d u + ∫ t a σ(u )d W (u )− 1 2 ∫ t a σ(u )2 d u  .
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