Compactified Morse trajectory spaces

Consider a smooth manifold $L$ equipped with a Morse function $f:L\to \mathbb{R}$ and a metric so that the gradient vector field $\nabla f$ satisfies the Morse-Smale conditions. Then the Morse trajectory spaces

${\begin{alignedat}{4}{\mathcal {M}}(L,L)&=\{\gamma :&[0,a]\;\;\to L&\,|\,{\dot \gamma }=-\nabla f(\gamma ),a\geq 0\},\\{\mathcal {M}}(p^{-},L)&=\{\gamma :&(-\infty ,0]\to L&\,|\,{\dot \gamma }=-\nabla f(\gamma ),\lim _{{s\to -\infty }}\gamma (s)=p^{-}\},\\{\mathcal {M}}(L,p^{+})&=\{\gamma :&[0,\infty )\;\to L&\,|\,{\dot \gamma }=-\nabla f(\gamma ),\lim _{{s\to +\infty }}\gamma (s)=p^{+}\},\\{\mathcal {M}}(p^{-},p^{+})&=\{\gamma :&\mathbb{R} \;\;\;\to L&\,|\,{\dot \gamma }=-\nabla f(\gamma ),\lim _{{s\to \pm \infty }}\gamma (s)=p^{\pm }\}/\mathbb{R} .\end{alignedat}}$

can - under an additional technical assumption specified in [1] - be compactified to smooth manifolds with boundary and corners ${\mathcal {M}}(\cdot ,\cdot )$. These compactifications are constructed such that the codimension-1 strata of the boundary are given by single breaking at a critical point (except in the first case we have to add one copy of $L$ to represent trajectories of length 0),

$\textstyle \partial ^{1}\overline {\mathcal {M}}(\cdot ,\cdot )\;=\;{\bigl (}\;L\cup \;{\bigr )}\;\bigsqcup _{{q\in {\text{Crit}}(f)}}\overline {\mathcal {M}}(\cdot ,q)\times \overline {\mathcal {M}}(q,\cdot ).$