2023
DOI: 10.1039/d2cp05299g
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Jahn–Teller effects in initial and final states: high-resolution X-ray absorption, photoelectron and Auger spectroscopy of allene

Abstract: Carbon K-edge resonant Auger spectra of gas-phase allene following excitation of the pre-edge 1s → π* transitions are presented and analysed with the support of EOM-CCSD/cc-pVTZ calculations.

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Cited by 7 publications
(10 citation statements)
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“…[53] The active space of 3 electrons in 2 active orbitals (singly occupied molecular orbital (SOMO) and doubly occupied molecular orbital (HDMO)) is chosen because these are sufficient to reproduce the emission energies utilizing the ∆SCF approach with PBE0-D3(BJ)/def2-SVP (see Figure S7). [36][37][38][39][40][41][42][43][44][45] Here the transition of the spin-down electron from HDMO to SOMO matches the experimentally observed emission energy (see also Supporting Information for further clarification).…”
Section: Quantum Chemical Calculations On the Photophysicssupporting
confidence: 78%
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“…[53] The active space of 3 electrons in 2 active orbitals (singly occupied molecular orbital (SOMO) and doubly occupied molecular orbital (HDMO)) is chosen because these are sufficient to reproduce the emission energies utilizing the ∆SCF approach with PBE0-D3(BJ)/def2-SVP (see Figure S7). [36][37][38][39][40][41][42][43][44][45] Here the transition of the spin-down electron from HDMO to SOMO matches the experimentally observed emission energy (see also Supporting Information for further clarification).…”
Section: Quantum Chemical Calculations On the Photophysicssupporting
confidence: 78%
“…We optimize their ground (D0) with Kohn-Sham DFT and first excited state (D1) geometries using ∆SCF initial maximum overlap method ((IMOM-), both at the PBE0-D3(BJ)/def2-SVP level. [36][37][38][39][40][41][42][43][44][45] We determine the canonical orbitals involved in the transition using (∆SCF -)PBE0-D3(BJ)/def2-SVP (see Figure 3). These are the highest occupied spin-down orbitals in D0 and D1.…”
Section: Excited State Characteristicsmentioning
confidence: 99%
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“…Here, we employ the core-valence separation (CVS) approximation, , which allows us to efficiently compute core-excited states by neglecting their interaction with excitations from the remaining occupied orbitals. CVS has been widely used for simulating core-level excited states and X-ray absorption spectra in combination with a variety of electronic structure theories. ,,,,,,,, …”
Section: Theorymentioning
confidence: 99%
“…38 and 39, and the method has been successfully used in numerous cases. [40][41][42][43][44][45][46] The ground state MD simulations were performed at the B3LYP/6-31+g* level using the quantum thermostat, 47,48 with the temperature set to 300 K. The total length of the simulation was 50 ps and the time step was set to 0.5 fs. Within the NEA approach, a larger set of 400 and a smaller set of 50 geometries were selected from the ground state MD.…”
Section: Experimental Methodsmentioning
confidence: 99%