| |
Nicolaas, R., Caron, S., Stoppa, F., Bhattacharyya, S., Ruiz de Austri, R., Groot, P. J., et al. (2026). BGRem: A background noise remover for astronomical images based on a diffusion model. Astron. Astrophys., 710, A131–14pp.
Abstract: Context. Astronomical imaging aims to maximize signal capture while minimizing noise. It is difficult and expensive to enhance the signal-to-noise ratio directly on detectors, which has led to extensive research into advanced post-processing techniques. Aims. Removing background noise from images is a valuable preprocessing step for catalog-building tasks. We introduce BGRem, a machine-learning (ML)-based tool to remove background noise from astronomical images. Our aim is to improve image quality and enhance the performance of the subsequent analysis pipeline, from detecting faint sources to performing source characterization tasks. Methods. The BGRem tool uses a diffusion-based model with an attention U-Net as backbone, trained on simulated images for optical and gamma (gamma)-ray data from the MeerLICHT and Fermi-LAT telescopes. The tool learns to denoise astronomical images in a supervised manner over several diffusion steps. We performed preprocessing and postprocessing techniques, including normalization and median subtraction, on these images to make them suitable for the analysis pipeline. Results. We compared the performance of BGRem with SourceExtractor (SExtractor), a widely used tool for cataloging astronomical sources. The number of true positive sources using SExtractor increased by about 7% for MeerLICHT data when we used BGRem as a preprocessing step. We also show the generalizability of BGRem by testing it with optical images from different telescopes and on simulated gamma-ray data representative of the Fermi-LAT telescope. In both cases, BGRem improves the source detection efficiency. Conclusions. The BGRem tool improves the source detection accuracy of traditional pixel-based methods by removing complex background noise. Using zero-shot approach, BGRem generalizes well to a wide range of optical images. The successful application of BGRem to simulated gamma-ray images, alongside optical data, demonstrates its adaptability to distinct noise characteristics and observational domains. This cross-wavelength performance highlights its potential as a general-purpose background removal framework for multiwavelength astronomical surveys.
|
|
Gomez Nicola, A., Molina, R., & Sanchez, J. A. (2026). Pion scattering in finite volume within the Inverse Amplitude Method. J. High Energy Phys., 06(6), 057–50pp.
Abstract: We study the effect of a finite volume for pion-pion scattering within Chiral Perturbation Theory (ChPT) and the Inverse Amplitude Method (IAM) in a L3 box (rest frame). Our full ChPT calculation takes into account the discretization not only in the s-channel loops but also in the t, u- channels and tadpole contributions. Hence, not only the unitarity right-hand cut but also the continuum contributions to the left-hand cut are calculated in the finite volume. A proper extension of the standard Veltman-Passarino identities is needed, as well as a suitable projection on the internal space spanned by the irreducible representations (irreps) of the octahedral group, based on either a finite set of cubic harmonics or the matrices which represent the irreps properly. From the ChPT we construct the IAM in the internal space, which provides the full volume dependence of the interacting energy levels of two pions scattering in the finite volume. Our results for various sets of low-energy constants show sizable corrections with respect to previous analyses in the literature for m pi L less than or similar to 2, being compatible with energy levels lattice data. We expect that our analysis and results will help to optimize the process of determining energy levels and phase-shifts with higher accuracy.
|
|
Garramone, M., Fornengo, N., & Gariazzo, S. (2026). Early-Universe constraints on the electron mass. Phys. Rev. D, 113(12), 123008–16pp.
Abstract: We investigate the impact of a nonstandard electron mass me on early-Universe thermal history, focusing on neutrino decoupling and big bang nucleosynthesis (BBN). In the standard cosmology, neutrino-electron interactions keep neutrinos in thermal contact with the electromagnetic plasma until shortly before et annihilation. Varying me shifts the decoupling epoch and the entropy transfer from et annihilation, thereby modifying the neutrino energy density and the inferred effective number of relativistic species, Neff. Independently, during BBN, the rates of charged-current weak processes, and hence the neutron-to-proton ratio, depend on me. By confronting BBN predictions for the primordial light-element abundances with observations and imposing cosmological constraints on Neff, we obtain the following 1 sigma bounds on me in the early Universe: me = 0.505+0.006 -0.007 MeV (for the NACRE II nuclear reaction network) or -0.004 MeV (for the PRIMAT nuclear reaction network). These bounds have been derived by adopting the recent determination of the primordial helium-4 abundance by the Large Binocular Telescope observations of 54 metal-poor H II regions. If instead we adopt the Particle Data Book helium-4 abundance, the bounds are me = 0.503 & thorn;0.011 -0.015 MeV (NACRE II) or me = 0.521 & thorn;0.009 obtained allowed ranges are close to the present laboratory value at the level of similar to 0.4%-2%, depending on the dataset and nuclear network, thus supporting the constancy of the electron mass over cosmological timescales.
|
|
Cho, Y. et al, & Perez-Vidal, R. M. (2026). Regularity of core coupled high-spin structure in neutron-rich 196-202Au isotopes approaching N=126. Phys. Lett. B, 878, 140558–7pp.
Abstract: Excited states built upon long-lived high-spin isomers in hard-to-reach neutron-rich Au (Z = 79) isotopes were populated using multi-nucleon transfer reactions between 136Xe and 198Pt at 7 MeV/u. These states in 196,198-202Au were identified for the first time using the powerful combination of the VAMOS++ spectrometer, the CATLIFE detection system, and the AGATA 1-ray tracking array. Their measured energies exhibit remarkable regularity as a function of neutron number and are seen to be inherited from the energies of yrast-band members in the corresponding Hg (Z = 80) isotope. Large-scale shell-model calculations reproduce the observed regularity and show that these states arise from the unique-parity orbitals 20h11/2 and v0i13/2 coupled to the Hg core. This regularity is due to the dominant proton configurations of the Hg and Au isotopes, where the level energies are almost independent of different neutron-orbital occupancies. The calculated Au wave functions show significant higher-spin components of the corresponding Hg core, unlike what is expected in the conventional interpretation in terms of the weak-coupling/decoupling limits of the particle-core coupling model.
|
|
Ramos, D., Caamaño, M., Farget, F., Rodriguez-Tajes, C., Lemasson, A., Rejmund, M., et al. (2026). Isotopic fission yields of 240Pu as a function of the excitation energy. Phys. Rev. C, 113(5), 054611–10pp.
Abstract: Complete isotopic fission yields distributions of 240Pu have been measured as a function of the initial excitation energy. The 240Pu fissioning system was produced through a two-proton transfer reaction between a 238U beam and a 12C target. The reaction was measured in inverse kinematics at Coulomb barrier energies, allowing for the full distribution of fission fragments to be isotopically identified with the VAMOS + + Spectrometer. The excitation energy of the system was measured on an event-by-event basis by detecting the targetlike recoil 10Be in a segmented silicon telescope. This manuscript reports on the evolution of the fission yields as a function of the excitation energy of the system between 8.2 to 11.9 MeV. The influence of the excitation energy is manifested in the damping of shell effects that feed the yields in the symmetry valley, as well as in a reduction of the neutron content of the fragments. This reduction, however, is observed only in the heavy fragment, while the neutron content of the light fragment remains unaffected. The comparison with previous measurements, models, and evaluations highlights the importance of correlated observables for improving fission models.
|
|
|