We investigate the resonant and non-resonant Auger spectra of ozone with a newly implemented multi-reference protocol based on the one-center approximation [Tenorio , 2022, , 4387-4407]. The results of our calculations are compared to existing experimental data, where we elucidate the resonant Auger spectrum measured at 530.8 and 536.7 eV, that correspond to the 1s → π*(2b) and 1s → σ*(7a) resonances, and at 542.3 eV, which lies near the 1s → *(7a) excited state and above the 1s ionization threshold. Using molecular dynamics simulations, we demonstrate the relevance of few-femtoseconds nuclear dynamics in the resonant Auger spectrum of ozone following the 1s → π*(2b) core-excitation.
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J Phys Chem A
January 2025
Department of Chemistry, University of Southern California, Los Angeles, California 90089, United States.
We present ab initio calculations of the resonant Auger spectrum of benzene. In the resonant process, Auger decay ensues following the excitation of a core-level electron to a virtual orbital. Hence, resonant Auger decay gives rise to higher-energy Auger electrons compared to nonresonant decay.
View Article and Find Full Text PDFNano Lett
January 2025
Wyant College of Optical Sciences, University of Arizona, 1630 East University Boulevard, Tucson, Arizona 85721, United States.
Microscopic many-body models based on inputs from first-principles density functional theory are used to calculate the carrier losses due to free carrier Auger-Meitner recombination (AMR) processes in Mo- and W-based monolayer transition metal dichalcogenides as a function of the carrier density, temperature, and dielectric environment. Despite the exceptional strength of Coulomb interaction in the two-dimensional materials, the AMR losses are found to be similar in magnitude to those in conventional III-V-based quantum wells for the same wavelengths. Unlike the case in III-V materials, the losses show nontrivial density dependencies due to the fact that bandgap renormalizations on the order of hundreds of millielectronvolts can bring higher bands into or out of resonance with the optimal energy level for the AMR transition, approximately one bandgap from the lowest band.
View Article and Find Full Text PDFPhys Chem Chem Phys
December 2024
Jožef Stefan Institute, Jamova cesta 39, 1000 Ljubljana, Slovenia.
We present an theoretical method to calculate the resonant Auger spectrum in the presence of ultrafast dissociation. The method is demonstrated by deriving the L-VV resonant Auger spectrum mediated by the 2pσ* resonance in HCl, where the electronic Auger decay and nuclear dissociation occur on the same time scale. The Auger decay rates are calculated within the one-center approximation and are shown to vary significantly with the inter-nuclear distance.
View Article and Find Full Text PDFNeurology
January 2025
From the Multiple Sclerosis Centre of Catalonia (Cemcat) & Neurology Department (N.M.-O., P.C.-M., N.B., A.V.-J., M.T., X.M., J.S.-G.), and Section of Neuroradiology (D.P., M.A., C.A., À.R.), Department of Radiology (IDI), Vall Hebron University Hospital, Barcelona; Neuroimaging Research Unit (P.V., M.M., A.M., P.P., M.A.R., M.F.), Division of Neuroscience, Neurology Unit, and Neurorehabilitation Unit (M.M., M.F.), IRCCS San Raffaele Scientific Institute, Milan, Italy; Multiple Sclerosis Center (MSC) (C.G., C.Z.), Department of Neurology, Neurocenter of Southern Switzerland, Ente Ospedaliero Cantonale; Faculty of Biomedical Sciences (C.G., C.Z.), Università della Svizzera Italiana (USI), Lugano, Switzerland; Faculty of Brain Sciences (F.B.), University College London Queen Square Institute of Neurology, University College London; National Institute for Health Research (F.B.), University College London Hospitals Biomedical Research Centre, United Kingdom; MS Center Amsterdam (F.B., M.M.S., E.M.M.S.), Vrije Universiteit Amsterdam, Amsterdam Neuroscience, Amsterdam UMC location VUmc, the Netherlands; Clinic of Neurology (A. Gallo, A.B.), and MRI Research Center SUN-FISM (A. Gallo, A.B.), Second University of Naples, Italy; Queen Square MS Centre (O.C., F.D.A., M.C.Y.), Department of Neuroinflammation, UCL Queen Square Institute of Neurology, Faculty of Brain Sciences, University College London; National Institute for Health Research (O.C., F.D.A.), Biomedical Research Centre, University College London Hospitals; Nuffield Department of Clinical Neurosciences (J.P., L.M.), Oxford, United Kingdom; Department of Neurology (A. Gass, P.E.), Mannheim Center of Translational Neurosciences (MCTN), Medical Faculty Mannheim, Heidelberg University; Institute of Neuroradiology (C.L., B.B.), St. Josef-Hospital Bochum, Ruhr University Bochum, Germany; Vita-Salute San Raffaele University (P.P., M.A.R., M.F.); Neurology Unit (P.P., M.A.R., M.F.), and Neuropshysiology Service (M.F.), IRCCS San Raffaele Scientific Institute, Milan, Italy.
Background And Objectives: In multiple sclerosis (MS), brain reserve serves as a protective factor against cognitive impairment. Previous research has suggested a structural counterpart in the spine-spinal cord reserve-seemed to be associated with physical disability. This study aimed to investigate the potential of the cervical canal area (CCaA) as a proxy for spinal cord reserve in a multicentric cohort of people with MS (PwMS).
View Article and Find Full Text PDFPhys Chem Chem Phys
December 2024
Graduate School of Science, Hiroshima University, Higashi-Hiroshima 739-8526, Japan.
Understanding electron transport in self-assembled monolayers on metal nanoparticles (NPs) is crucial for developing NP-based nanodevices. This study investigates ultrafast electron transport through aromatic molecules on NP surfaces resonant Auger electron spectroscopy (RAES) with a core-hole-clock (CHC) approach. Aromatic molecule-coated Au NPs are deposited to form condensed NP films, and flat monolayers are prepared for comparison.
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