There is a pretty clear resemblance between the Lagrangians for SUSY QM (1-dim susy sigma model) and various superstring theories (2-dim susy sigma models).
Again intuitively, one should expect the point particle theory to emerge as a zero-length/infinite string tension limit of the string theory.
How precisely is SUSY QM a limit of supersymmetric string theory?
From the nLab, we have
This deformed supersymmetric quantum mechanics arises as the point-particle limit of the type II superstring regarded as quantum mechanics on the smooth loop space (the string’s Wheeler superspace), a relation that is stated more explicitly in
Edward Witten, p. 92-94 in: Global anomalies in string theory, in: W. Bardeen and A. White (eds.) Symposium on Anomalies, Geometry, Topology, World Scientific (1985) 61-99 [pdf, spire:214913] and then in
Edward Witten, The Index Of The Dirac Operator In Loop Space, in: Elliptic Curves and Modular Forms in Algebraic Topology, Lecture Notes in Mathematics 1326, Springer (1988) 161-181 [doi:10.1007/BFb0078045, spire]
What is the precise statement and where does it occur in these two cited works?