Brownian half-integer sine expansion ($W={\sum }_n\frac{{\xi }_n{h}_n}{(n-1/2)\pi }\text{in }{L}^2[0,1]$)

The functions $h_n(t)=\sqrt{2}\sin ((n-1/2)\pi t)$ give the Brownian covariance eigenbasis on $[0,1]$, with eigenvalues ${\lambda }_n=((n-1/2)\pi {)}^{-2}$. Integrating by parts against $g_n=\sqrt{2}\cos ((n-1/2)\pi t)$ gives independent coefficients ${\xi }_n=\int g_{n}dW$. Pathwise L2 completeness yields $W={\sum }_n\sqrt{{\lambda }_n}{\xi }_n{h}_n$ in L2 and the squared-norm series.