Controlled field evaporation of organic materials has been a long-term challenge for 3-dimensional (3D) atom probe tomography (APT) [1]. Complications arising from sample electrical/thermal requirements, sample preparation methodologies, and hardware configurations have all conspired to limit APT application for this class of materials. Although polymer laser APT studies have been reported on various polymers including polystyrene [2], polypyrrole [2], and polythiophene [3], these reports have focused on field ionized mass spectroscopy (FIMS) of the polymer and have not even attempted 3D reconstructions.We present data on laser local electrode atom probe (LEAP®) [4] investigations of alkanethiol self-assembled monolayers (SAMs) and poly-3-alkylthiophenes (P3ATs). Alkanethiols represent an opportunity to understand APT field ionization and reconstruction issues, as applied to polymers, at their most basic level. Alkanethiols are monodisperse short-chain molecules which are covalently bonded to a pre-sharpened metal specimen to form a dense, well-ordered SAM on the tip surface. The well understood microstructure [5] and limited potential for molecular fragment permutations of alkanethiols provides a desirable set of well-defined boundaries for subsequent analyses.P3ATs are another family of conducting polymers that have a chemical architecture similar to polypyrrole and polythiophene and thus invite comparison to previously reported results. At their heart, P3ATs are polythiophene with alkane side-chains attached to the conducting polymer main-chain so that P3ATs also bear some similarity to alkanethiols. This investigation of two families of polymers promises to provide a more complete understanding of laser APT than studies of each polymer family individually. 10000 4 CH3+ t o lo 20 30 4SCH2040Hi 7 'CHji. mv;}~~~~~~~~~~~~~mlq (ani) -RoJ u~, |Figure 1: Laser LEAP analIysis of dodecanethiol on Pd tip. 3D reconstruction [left] of mass-to-charge spectrum [top] can be interpreted as low-field alkane fragments (small 7 dark circles) originating from the tip surface. A lack of events at intermediate field results 3 e in a gap artifact in the reconstruction. Peaks at 12, 32, and 33 amu (large gray squares) 0 o |~~~~reside exclusively within the Pd bulk. A number of molecules oniginate from the interface ><. U between alkane and Pd corresponding to peaks at 63, 64, and 65 amu (large light shaded 7 6 5 4 3 2 1 circles). Their location is highly suggestive of fragments corresponding to a missing thiol Depth (nm) component of the dodecanethiol molecule (see chemical diagram top-right insert). Figure 1 shows laser LEAP data for a dodecanethiol coated Pd specimen. Pd wire (99.995 %/ purity) was electropolished to form an APT compatible specimen. A SAM was formed on the tip by submersion in a~-5 mM solution of dodecanethiol in ethanol for~3 hrs. Field evaporation evolution was consistent with fragments of dodecanethiol molecules evaporating at very low field. Once the Pd surface was uncovered, a significantly higher field was n...