Matrix Exponential

The matrix exponential of Square Matrix XX is defined by a power series

eXn=0Xnn!\begin{gather*} e^X\triangleq \sum_{n=0}^\infty\frac{X^n}{n!} \end{gather*}

Properties of this

  • differential equations

    • the function U(t)=etXU(t)=e^{tX} is the only unique soln. to
dUdt=XU(t)U(0)=I\begin{gather*} \frac{dU}{dt}=XU(t)\quad U(0)=I \end{gather*} eX=Pdiag(eλ1,...,eλn)P1\begin{gather*} e^X=Pdiag(e^{\lambda_1},...,e^{\lambda_n})P^{-1} \end{gather*}

where PP is the basis matrix — a matrix whose columns are the eigenvectors XX w.r.t A^\hat{A}.

Specifically, if v1,v2,,vnv_1,v_2,…,v_n are eigenvectors of XX corresponding to eigenvalues λ1,λ2,,λn\lambda_1,\lambda_2,…,\lambda_n then

P=[v1v2vn]\begin{gather*} P = \begin{bmatrix} | & | & & | \\ v_1 & v_2 & \cdots & v_n \\ | & | & & | \end{bmatrix} \end{gather*}
  • Hermitian and skew-Hermitian matrices → if H=H+H=H^+ then eiHe^{iH} is unitary this means
(eiH)+eiH=I\begin{gather*} (e^{iH})^+e^{iH}=I \end{gather*}

Note that if AA is a matrix, then, via Taylor Series, we have

eAt=k=0Aktkk!=I+At+(At)22!+(At)33!+e^{At} = \sum_{k=0}^{\infty}\frac{A^k t^k}{k!} = I + At + \frac{(At)^2}{2!} + \frac{(At)^3}{3!} + \cdots ddteAt=k=1kAktk1k!=Ak=1Ak1tk1(k1)!=AeAt=eAtA\frac{d}{dt}e^{At} = \sum_{k=1}^{\infty}\frac{kA^k t^{k-1}}{k!} = A\sum_{k=1}^{\infty}\frac{A^{k-1}t^{k-1}}{(k-1)!} = Ae^{At} = e^{At}A