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S Manti

Publications and source records attributed to S Manti.

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First Kaonic Boron Isotopes Measurements with SIDDHARTA-2 at DA$\Phi$NE

A precision measurement of X-ray transitions in kaonic boron, performed by the SIDDHARTA-2 collaboration at the DA$\Phi$NE collider, is reported. The energies and yields of the $5g\rightarrow4f$ and $4f\rightarrow3d$ transitions were determined for both boron isotopes, kaonic ${}^{10}$B and kaonic ${}^{11}$B. For the $5g\rightarrow4f$ transition, the measured energies are $7064.62 \pm 16.93~(\mathrm{stat.}) \pm 2.00~(\mathrm{sys.})$~eV for kaonic ${}^{11}$B and $6920.96 \pm 58.23~(\mathrm{stat.}) \pm 2.00~(\mathrm{sys.})$~eV for kaonic ${}^{10}$B. For the $4f\rightarrow3d$ transition, the corresponding values are $15293.33 \pm 4.80~(\mathrm{stat.}) \pm 5.30~(\mathrm{sys.})$~eV and $15180.11 \pm 20.86~(\mathrm{stat.}) \pm 5.30~(\mathrm{sys.})$~eV, respectively. The yields for the $5g\rightarrow4f$ transition are $0.076 \pm 0.013~(\mathrm{stat.})^{+0.012}_{-0.011}~(\mathrm{sys.})$ for kaonic ${}^{11}$B and $0.079 \pm 0.014~(\mathrm{stat.})~^{+0.013}_{-0.011}~(\mathrm{sys.})$ for kaonic ${}^{10}$B. For the $4f\rightarrow3d$ transition, the corresponding yields are $0.115 \pm 0.006~(\mathrm{stat.})~^{+0.002}_{-0.005}~(\mathrm{sys.})$ and $0.107\pm 0.007~(\mathrm{stat.})~^{+0.002}_{-0.005}~(\mathrm{sys.})$, respectively. No statistically significant deviation from pure electromagnetic (QED) calculations was observed in the measurement of the $4f\rightarrow3d$ X-ray transition in kaonic ${}^{11}$B. Interpreted as upper limits, these results impose stringent constraints on the strong-interaction energy shift and width of the 3d level in light nuclei. Translating these limits into bounds on phenomenological kaon-nucleus optical potentials, and, within specific theoretical models, on the complex scattering amplitude, we constrain and disfavor scenarios predicting large shifts or widths in boron.

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High precision X-ray spectroscopy of kaonic neon

The high-precision kaonic neon X-ray transitions measurement performed by the SIDDHARTA-2 collaboration at the DA$\Phi$NE collider is reported. Both the X-ray energies and yields for high-n transitions were measured, demonstrating the feasibility of sub-eV Xray spectroscopy for kaonic atoms using low-Z gaseous targets. The measurement provides valuable insights into the de-excitation processes in kaonic atoms, providing new input data for the refinement of the corresponding theoretical models, and a framework for testing Quantum Electrodynamics in strange exotic atoms.

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First measurement of kaonic helium-4 M-series transitions

In this paper we present the results of a new kaonic helium-4 measurement with a 1.37 g/l gaseous target by the SIDDHARTA-2 experiment at the DA{\Phi}NE collider. We measured, for the first time, the energies and yields of three transitions belonging to the Mseries. Moreover, we improved by a factor about three, the statistical precision of the 2p level energy shift and width induced by the strong interaction, obtaining the most precise measurement for gaseous kaonic helium, and measured the yield of the L{\alpha} transition at the employed density, providing a new experimental input to investigate the density dependence of kaonic atoms transitions yield.

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Novel Machine Learning and Differentiable Programming Techniques applied to the VIP-2 Underground Experiment

In this work, we present novel Machine Learning and Differentiable Programming enhanced calibration techniques used to improve the energy resolution of the Silicon Drift Detectors (SDDs) of the VIP-2 underground experiment at the Gran Sasso National Laboratory (LNGS). We achieve for the first time a Full Width at Half Maximum (FWHM) in VIP-2 below 180 eV at 8 keV, improving around 10 eV on the previous state-of-the-art. SDDs energy resolution is a key parameter in the VIP-2 experiment, which is dedicated to searches for physics beyond the standard quantum theory, targeting Pauli Exclusion Principle (PEP) violating atomic transitions. Additionally, we show that this method can correct for potential miscalibrations, requiring less fine-tuning with respect to standard methods.

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