Deeply bound 1s and 2p states in pionic atoms
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Quantum Chemistry and Spectroscopy of Pionic Atomic Systems With Accounting for Relativistic, Radiative, and Strong Interaction Effects
2019, Advances in Quantum ChemistryCitation Excerpt :Namely the strong hadron–nuclear interaction is the reason for a shift in the energies of the low-lying levels from the purely electromagnetic values, and the finite lifetime of the state corresponds to an increase in the observed level width. At present time a few theoretical approaches to studying spectra and spectral properties of the exotic (pionic, kaonic, muonic, antiprotonic, etc.) atomic systems are usually used.1–46 Analyzing the bibliography of works on spectroscopy of pionic atoms, one should distinguish two groups of theoretical works based on the direct analytic or numerical solution of the Klein–Gordon–Fock equation (KGF), which relates either to the electromagnetic (atomic-optical) sector or to the purely nuclear sector (without precise studying the QED contributions to energy levels).
In-medium nuclear interactions of low-energy hadrons
2007, Physics ReportsStrong interaction physics from hadronic atoms
1997, Physics ReportNeutron-induced peaks in Ge detectors from evaporation neutrons
1997, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentA theoretical approach to pionic atoms and the problem of anomalies
1993, Nuclear Physics, Section ATotal reaction cross sections for 20-30 MeV pions and the anomaly of pionic atoms
1991, Physics Letters B