2020
DOI: 10.1088/1361-6455/abc6bd
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From synchrotrons for XFELs: the soft x-ray near-edge spectrum of the ESCA molecule

Abstract: A predictive understanding of soft x-ray near-edge absorption spectra of small molecules is an enduring theoretical challenge and of current interest for x-ray probes of molecular dynamics. We report the experimental absorption spectrum for the ESCA molecule (ethyl trifluoroacetate) near the carbon 1s absorption edge between 285-300 eV. The ESCA molecule with four chemically distinct carbon sites has previously served as a theoretical benchmark for photoelectron spectra and now for photoabsorption spectra. We … Show more

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Cited by 16 publications
(31 citation statements)
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“…This formulation is naturally combined with the frozen-core approximation separating valence and core spaces. However, one may argue that it introduces at the same time an additional error from neglecting core correlation. , …”
Section: Methods and Implementationmentioning
confidence: 99%
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“…This formulation is naturally combined with the frozen-core approximation separating valence and core spaces. However, one may argue that it introduces at the same time an additional error from neglecting core correlation. , …”
Section: Methods and Implementationmentioning
confidence: 99%
“…Besides the original CC-CVS approach, we have also investigated other approximations: Further restricting the definition of the projectors to also drop excited configurations with two core indices (ND, for “No Doubly core hole determinants”); this corresponds to the method suggested, e.g., in ref , obtaining Freezing the core in the ground-state calculation, thus retaining only the valence orbitals, typically defined as the orbitals with the highest principal quantum number n (FC-V); this essentially corresponds to using eq while setting ϵ CV to a fairly high value (for example, in the atom of Xe, ϵ 4d < ϵ CV < ϵ 5s ). Freezing all core orbitals, except for those that are to be targeted in the EOM step (FC-V-except); for example, this means treating a core spinor k , that should make up the most important core-excited configurations for state μ, different from other core spinors in the ground-state calculation. This corresponds to setting projectors for ground and excited states such that This approach is equivalent to the one of Sorensen et al The definition of the core/valence spaces follows that of the CVS definition/threshold, that is, only the core orbitals with the same or lower energy than the ones belonging to the edge under investigation are frozen (FC-f). This is the same approach adopted in ref , and it corresponds to setting projectors for ground and excited states such that Further restricting the number of frozen-core spinors to only those below the ones of the edge of interest (FC-fpMO frozen corefollow previous MO).…”
Section: Computational Detailsmentioning
confidence: 99%
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“…Interpretation of ultrafast X-ray spectroscopic measurements is invariably linked with theory, which, for understanding structural dynamics of core-excited matter, is an ongoing challenge as described in some recent reviews [73,74]. There are already challenges at a very basic level, e.g., to predict the X-ray absorption spectrum of ground-state species with sub-eV accuracy [75] and to locate the positions of double-hole states [76]. Here, advances in equation-of-motion coupled-cluster (EOM-CC) approaches [77,78] have allowed a systematic convergence after application of the core-valence separation scheme [79] within the EOM-CC framework [80].…”
Section: Discussion and Applicationsmentioning
confidence: 99%