13 Multiple Variables

1 Joint Distribution

Now we want to explore multiple variables and their interaction. Here we focus on bivariate jointly continuous RVs.

Jointly Continuous

(X,Y) are jointly continuous if ∃ a function with joint density function f(x,y), s.t.P((X,Y)∈B)=∬Bf(x,y)dxdy,
For B⊂R2 measurable.
So fX,Y(x,y)=limΔ→(x,y)P((x,y)∈Δ)Area(Δ).

A joint density function satisfies

In the one dimensional case, for continuous RV, we have the approximation P(X∈[x,x+ε))≈fX(x)ε.
Similarly in two dimentional case, take a small neighborhood Δ containing (x,y), then we have P((X,Y)∈Δ)≈fX,YArea(Δ).

How to recover the marginal density fX or fY given fX,Y?

P(X≤t)=∫−∞t∫−∞∞fX,Y(x,y)dydx=∫−∞tfX(x)dx.
Fact

fX(x)=∫RfX,Y(x,y)dy=∫RfX,Y(x,y)dx.

X=dW,Y=dZ will not lead to (X,Y)=d(W,Z): let X,W,V∼i.i.dExp(1), and Z∼Gamma(2,1). Let Y=X+V. By this result we know Y∼dGamma(2,1). Then X=dW,Y=dZ. However, we always have X≤Y, and W>Z has positive probability, so (X,Y)≠d(W,Z).

1.1 Independence

X,Y are independent if fX,Y(x,y)=fX(x)fY(y),∀(x,y)∈R2.
By independence, the value of X will not give us anything about Y.

2 Bivariate Transformation

Transformation of random variables: T:R2→R2,(X,Y)↦(W,Z).
Polar coordinates: (x,y)↦(r,θ),x=rcos⁡θ,y=rsin⁡θ.

Fact (Polar Coordinates)

fR,Θ(r,θ)=rfX,Y(rcos⁡θ,rsin⁡θ).

Linear transformation

T:R2→R2 is a linear transformation if T(xy)=MT(xy)+PT.MT∈R2×2,PT∈R2×1.

Some properties:

Let T be a linear transformation with inverse S. Given the joint p.d.f of (X,Y), what's the joint p.d.f of (W,Z)=T(X,Y)?
On one hand, P((W,Z)∈P)≈fW,Z(w,z)Area(P).
Similarly P((W,Z)∈P)=P(T(X,Y)∈P)=P((X,Y)∈S(P))≈fX,Y(x,y)Area(S(P))=fX,Y(S(w,z))Area(P)|det(MS)|.
We conclude that for invertible transformation T,

fW,Z(w,z)=fX,Y(S(w,z))|det(MS)|.
Orthogonal transformation

T is an orthogonal transformation if it preserves the inner product: ⟨v→,w→⟩=⟨Tv→,Tw→⟩. I.e.: PT=0, MT is an orthogonal matrix, MT−1=MTT.

They preserve angles, lengths, Areas, det(MT)=±1.

Fact

For R2, all orthogonal transformations are rotation, reflection, and composition of the two.

3 Invertible Affine Transformation

Suppose T:R2→R2,T(X,Y)=(U,V) has inverse S(U,V)=(X,Y).
Pasted image 20241201150847.png|400
Define linear translation T(X,Y)=MT[XY]+PT=[UV], where MT is 2×2 invertible matrix, and PT is 2×1 vector.
Since ST(X,Y)=S(U,V)=(X,Y), S(U,V)=MT−1[UV]−MT−1PT=MS[UV]+PS.
Since P((U,V)∈B)=P((X,Y)∈S(B))⇒∬BfU,V(u,v)dudv=∬S(B)fX,Y(x,y)dxdy, we have (3.1)fU,V(u,v)=fX,Y(S(u,v))|detMS|.

4 General Invertible Transformations

T:R2→R2. Assume differentiable, but not necessarily affine. Also assume T(X,Y)=(U,V), S(U,V)=(X,Y), ST(X,Y)=(X,Y). So P((U,V)∈Δ)=P((X,Y)∈S(Δ))⇒fU,V(u,v)Area(Δ)≈fX,Y(S(u,v))Area(S(Δ)).
We want to know S(Δ).
If S is affine, then S(Δ) is a parallelogram. For general S, if δ,ε≪1, then S(Δ) can be approximated by a parallelogram, since S can be approximated by an affine transformation on Δ.
Let S(uv)=[S1(u,v)S2(u,v)]∈R2, where Si:R2→R,i=1,2 are differentiable functions. Then for any point (a,b) near (u,v), the Taylor expansion in second order gives Si(a,b)≈Si(u,v)+(a−u)∂Si∂u(u,v)+(b−v)∂Si∂v(u,v).
In matrix notation, S[ab]≈[S1(u,v)S2(u,v)]+[∂S1∂u(u,v)∂S1∂v(u,v)∂S2∂u(u,v)∂S2∂v(u,v)][a−ub−v]. This is an affine transformation. Denote the yellow matrix as JS(u,v), which is the Jacobian matrix of S at (u,v).

Hence, P((X,Y)∈S(Δ))≈fX,Y(S(u,v))|detJS(u,v)|Area(Δ), so (4.1)fU,V(u,v)=fX,Y(S(u,v))|detJS(u,v)|.

In summary,