Q-Chem

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Q-Chem provides a comprehensive ab initio quantum chemistry program, allowing scientists worldwide to model chemical problems quickly and accurately. http://q-chem.com/

One of the things we're most excited about in Q-Chem 7 is QC-PBC: A new module that uses a GTO basis for modeling periodic systems. Highlights include fast hybrid DFT; CC and MP2; analytic derivatives; excited states; solvation; and EDA. Pre-order today: q-chem.com/purchase/

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Q-Chem offers state-of-the-art tools for handling electron correlation, such as MP2 and CC methods; the Q-Chem 6 generation has included new correlated methods like EOM-CCSDT, BW-s2, TDDFT/TDA-SOC, and MRSF-TDDFT. Stay tuned as we highlight recent and upcoming features!

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Q-Chem provides a wave-function analysis toolkit (libwfa) that enables visualization of excited states, automatic assignment of properties, and deeper insight into the underlying physics. QC6 has included several new additions, including CT metrics for TDDFT and Δ-ALMO(MSDFT2).

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Q-Chem provides one of the most extensive libraries for computational #spectroscopy, including: IR, UV-Vis, and vibronic spectra; X-ray spectra; restricted and unrestricted VCD; and more. Follow along this week as we discuss the latest spectroscopy developments in Q-Chem!

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Density functional theory is an essential method in any #compchem toolkit. Popular and general-purpose, it allows researchers to study electronic structure, predict geometries, model spectra, and much more. Follow along this week as we talk about #DFT in Q-Chem!

Text reads: "On the road to Q-Chem 7. Key Feature of the Week: Density Functional Theory. Use our vast library of functionals to model ground and excited states; Get faster results with optimized integral algorithms, RI, and great parallel performance; Improve convergence with new features like “Robust SCF”"

Check out the latest paper from Q-Chem developers at KU Leuven, in which they present a new method for computing partial Auger decay widths faster and more robustly! doi.org/10.1021/acs.... Follow us to stay up-to-date on new features and papers from Q-Chem developers!

Computation of Partial Auger Decay Widths from Complex-Valued Equation-of-Motion Coupled-Cluster Energies

We discuss the computation of partial Auger decay widths with equation-of-motion ionization-potential coupled-cluster (EOMIP-CCSD) theory in the framework of non-Hermitian quantum mechanics (NHQM). In NHQM, the decaying character of metastable states is described with complex energies and the total decay width is obtained directly from the total energy. In contrast, the computation of partial decay widths, i.e., the contributions of different decay channels to the total width, requires further analysis. However, partial widths are important for Auger spectroscopy as they determine the probability with which different final states are formed and hence the shape of the Auger spectrum. Recently, we introduced Auger channel projectors (ACPs), which selectively remove decay channels from the EOMIP-CCSD excitation manifold. This method requires a separate EOMIP-CCSD calculation for each decay channel. Here, we suggest an alternative: We solve the EOMIP-CCSD equations for the core-ionized state in the full excitation manifold and decompose the imaginary part of the resulting energy. In this way, we obtain all partial decay widths at once. We compute Auger spectra for K-edge-ionized states of methane, ethane, and hydrogen sulfide, and a Coster–Kronig spectrum for L1-edge-ionized hydrogen sulfide. The results obtained with our new approach differ only negligibly from ACP results. We also present the first Auger spectra for the cyanide anion, including vibrational broadening, and discuss the differences between the spectra of the carbon core hole and the nitrogen core hole.

doi.org