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Chemical dynamics characteristics of Kapton polyimide damaged by electron beam irradiation (uncorrected proof)

PDF variant

Uncorrected proof. Curated VOR summary: 2019rahnamoun-polymer-176-chemical-dynamics.

Summary

The uncorrected proof corresponds to the Polymer article DOI 10.1016/j.polymer.2019.05.035 on Kapton (PMDA–ODA polyimide) degradation under electron irradiation, combining polarizable ReaxFF reactive molecular dynamics with Fourier-transform infrared spectroscopy, electron paramagnetic resonance, nuclear magnetic resonance, wide- and small-angle X-ray scattering, and dynamic mechanical analysis. The abstract in the proof describes approximating the electron beam as a dense column of negatively charged particles inserted at random positions in the polymer matrix, switching each beam on for 2 fs so that Coulomb interactions transfer an average energy of 21 eV per electron trajectory during the simulation window. It states that experimental samples are aged in vacuum with a 90 keV electron beam whose penetration depth exceeds the film thickness, and that after beam segments the authors run 0.5 ns of microcanonical MD to capture structural relaxation.

Methods

Document role. This file is the uncorrected proof PDF for the Polymer article; full simulation tables, the complete beam protocol, and all characterization parameters are in [[2019rahnamoun-polymer-176-chemical-dynamics]] and the version-of-record PDF at the same DOI.

1 — MD application (polarizable eReaxFF, electron-beam model). Molecular dynamics uses the ReaxFF program as in the VOR Methods. The abstract (also in the local proof extract) approximates the beam as a dense column of negatively charged particles inserted at random positions in the Kapton (PMDA–ODA) matrix; each beam is on for 2 fs, with Coulomb-mediated transfer of ~21 eV per electron trajectory; NVE for 0.5 ns after the beam sequence captures post-exposure relaxation (as stated in the proof). The VOR Methods give the eReaxFF line, the 20-chain Kapton model (C₁₅₄H₇₂O₃₅N₁₄ per chain, 7 repeat units, H-terminated), 0.1 fs integration where stated, and the NVT equilibration ~300 K (with thermostat type) before NVE beam segments. 3D PBC apply to the polyimide slab. Barostat / NPT production: N/A for the NVE-dominant damage stages after equilibration. Pressure control: N/A in the NVE stages. Shear, shock, external uniform E-field, umbrella / metadynamics: N/A—energy enters via local Coulomb deposition from the dummy beam model, not a continuum E-field fix in the FF sense.

2 — Experiments. 90 keV e-beam aging in vacuum; penetration depth > film thickness. FTIR, EPR, ¹³C MAS NMR, WAXD, SAXS, DMA on pristine vs irradiated films—full dose rates and sampling in the VOR.

3 — Force-field training. N/A (uses a published polarizable eReaxFF / ReaxFF line for this polymer; de novo fit is not the main result).

4 — Static DFT as sole outcome. N/A.

Findings

Corpus honesty. The proof abstract claims agreement between trajectory-level chemistry and FTIR / EPR / NMR / WAXD / SAXS / DMA, and refers to slab temperature and mechanical evolution under exposure; doseresponse curves and tables must be read from the final Polymer PDF on [[2019rahnamoun-polymer-176-chemical-dynamics]], not from proof pagination alone. Intro motivation ( space materials; e-beam vs heavy-ion literature ) is framing in the manuscriptverify wording on the VOR if citing verbatim.

Comparisons / limitations. For qualitative regimes ( imide damage, cross-linking vs cleavage ), use the VOR page; this proof slug is for provenance of this PDF hash only.

Limitations

Uncorrected proofs may differ slightly from the journal version. Use the VOR page for stable pagination and any publisher corrections.

Relevance to group

Van Duin-group contribution linking polarizable ReaxFF to radiation damage of aerospace polyimides with multi-technique validation.

The beam-on/off protocol described in the abstract (2 fs excitation segments, 10 fs NVE spacing, 0.5 ns post-beam NVE) is unusual compared with standard ReaxFF production runs; reproducers should copy segment counts and durations verbatim from the VOR Methods section rather than improvising continuous-beam approximations.

Reader notes (navigation)

Citations and evidence anchors

DOI: 10.1016/j.polymer.2019.05.035