Browsing by Department "O.A. Abruzzo"
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Publication Open Access 7Be(n,p)7Li Reaction and the Cosmological Lithium Problem: Measurement of the Cross Section in a Wide Energy Range at n_TOF at CERN(2018) ;Damone, L. ;Barbagallo, M. ;Mastromarco, M. ;Mengoni, A. ;Cosentino, L. ;Maugeri, E. ;Heinitz, S. ;Schumann, D. ;Dressler, R. ;Käppeler, F. ;Colonna, N. ;Finocchiaro, P. ;Andrzejewski, J. ;Perkowski, J. ;Gawlik, A. ;Aberle, O. ;Altstadt, S. ;Ayranov, M. ;Audouin, L. ;Bacak, M. ;Balibrea-Correa, J. ;Ballof, J. ;Bécares, V. ;Bečvář, F. ;Beinrucker, C. ;Bellia, G. ;Bernardes, A. P. ;Berthoumieux, E. ;Billowes, J. ;Borge, M. J. G. ;Bosnar, D. ;Brown, A. ;Brugger, M. ;Busso, M. ;Caamaño, M. ;Calviño, F. ;Calviani, M. ;Cano-Ott, D. ;Cardella, R. ;Casanovas, A. ;Castelluccio, D. M. ;Catherall, R. ;Cerutti, F. ;Chen, Y. H. ;Chiaveri, E. ;Correia, J. G. M. ;Cortés, G. ;Cortés-Giraldo, M. A.; ;Diakaki, M. ;Dietz, M. ;Domingo-Pardo, C. ;Dorsival, A. ;Dupont, E. ;Duran, I. ;Fernandez-Dominguez, B. ;Ferrari, A. ;Ferreira, P. ;Furman, W. ;Ganesan, S. ;García-Rios, A. ;Gilardoni, S. ;Glodariu, T. ;Göbel, K. ;Gonçalves, I. F. ;González-Romero, E. ;Goodacre, T. D. ;Griesmayer, E. ;Guerrero, C. ;Gunsing, F. ;Harada, H. ;Heftrich, T. ;Heyse, J. ;Jenkins, D. G. ;Jericha, E. ;Johnston, K. ;Kadi, Y. ;Kalamara, A. ;Katabuchi, T. ;Kavrigin, P. ;Kimura, A. ;Kivel, N. ;Köster, U. ;Kokkoris, M. ;Krtička, M. ;Kurtulgil, D. ;Leal-Cidoncha, E. ;Lederer-Woods, C. ;Leeb, H. ;Lerendegui-Marco, J. ;Lo Meo, S. ;Lonsdale, S. J. ;Losito, R. ;Macina, D. ;Marganiec, J. ;Marsh, B. ;Martínez, T. ;Masi, A. ;Massimi, C. ;Mastinu, P. ;Matteucci, F. ;Mazzone, A. ;Mendoza, E. ;Milazzo, P. M. ;Mingrone, F. ;Mirea, M. ;Musumarra, A. ;Negret, A. ;Nolte, R. ;Oprea, A. ;Patronis, N. ;Pavlik, A.; ;Piscopo, M. ;Plompen, A. ;Porras, I. ;Praena, J. ;Quesada, J. M. ;Radeck, D. ;Rajeev, K. ;Rauscher, T. ;Reifarth, R. ;Riego-Perez, A. ;Rothe, S. ;Rout, P. ;Rubbia, C. ;Ryan, J. ;Sabaté-Gilarte, M.; ;Schell, J. ;Schillebeeckx, P. ;Schmidt, S. ;Sedyshev, P. ;Seiffert, C. ;Smith, A. G. ;Sosnin, N. V. ;Stamatopoulos, A. ;Stora, T. ;Tagliente, G. ;Tain, J. L. ;Tarifeño-Saldivia, A. ;Tassan-Got, L. ;Tsinganis, A. ;Valenta, S. ;Vannini, G. ;Variale, V. ;Vaz, P. ;Ventura, A. ;Vlachoudis, V. ;Vlastou, R. ;Wallner, A. ;Warren, S. ;Weigand, M. ;Weiß, C. ;Wolf, C. ;Woods, P. J. ;Wright, T. ;Žugec, P.n TOF CollaborationWe report on the measurement of the 7Be (n ,p ) 7Li cross section from thermal to approximately 325 keV neutron energy, performed in the high-flux experimental area (EAR2) of the n_TOF facility at CERN. This reaction plays a key role in the lithium yield of the big bang nucleosynthesis (BBN) for standard cosmology. The only two previous time-of-flight measurements performed on this reaction did not cover the energy window of interest for BBN, and they showed a large discrepancy between each other. The measurement was performed with a Si telescope and a high-purity sample produced by implantation of a 7Be ion beam at the ISOLDE facility at CERN. While a significantly higher cross section is found at low energy, relative to current evaluations, in the region of BBN interest, the present results are consistent with the values inferred from the time-reversal 7Li (p ,n )7Be reaction, thus yielding only a relatively minor improvement on the so-called cosmological lithium problem. The relevance of these results on the near-threshold neutron production in the p + 7Li reaction is also discussed.97 23 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 92Zr (n,γ) and (n,tot) measurements at the GELINA and n_TOF facilities(2022) ;Tagliente, G. ;Kopecky, S. ;Heyse, J. ;Krtička, M. ;Massimi, C. ;Mengoni, A. ;Milazzo, P. M. ;Plompen, A. J. M. ;Schillebeeckx, P. ;Valenta, S. ;Wynants, R. ;Tarifeño-Saldivia, A. ;Tarrío, D. ;Tassan-Got, L. ;Tsinganis, A. ;Vannini, G. ;Variale, V. ;Vaz, P. ;Ventura, A. ;Vermeulen, M. J.; ;Altstadt, S. ;Vlachoudis, V. ;Vlastou, R. ;Wallner, A. ;Ware, T. ;Weigand, M. ;Weiss, C. ;Wright, T. ;Žugec, P. ;Andrzejewski, J. ;Audouin, L. ;Bécares, V. ;Barbagallo, M. ;Bečvář, F. ;Belloni, F. ;Berthoumieux, E. ;Billowes, J. ;Boccone, V. ;Bosnar, D. ;Brugger, M. ;Calviño, F. ;Calviani, M. ;Cano-Ott, D. ;Carrapiço, C. ;Cerutti, F. ;Chiaveri, E. ;Chin, M. ;Colonna, N. ;Cortés, G. ;Cortés-Giraldo, M. A.; ;Diakaki, M. ;Domingo-Pardo, C. ;Dressler, R. ;Durán, I. ;Eleftheriadis, C. ;Ferrari, A. ;Fraval, K. ;Furman, V. ;Göbel, K. ;Gómez-Hornillos, M. B. ;Ganesan, S. ;García, A. R. ;Giubrone, G. ;Gonçalves, I. F. ;González-Romero, E. ;Goverdovski, A. ;Griesmayer, E. ;Guerrero, C. ;Gunsing, F. ;Heftrich, T. ;Hernández-Prieto, A. ;Jericha, E. ;Käppeler, F. ;Kadi, Y. ;Karadimos, D. ;Katabuchi, T. ;Ketlerov, V. ;Khryachkov, V. ;Kivel, N. ;Kokkoris, M. ;Kroll, J. ;Lampoudis, C. ;Langer, C. ;Leal-Cidoncha, E. ;Lederer, C. ;Leeb, H. ;Leong, L. S. ;Losito, R. ;Lugaro, M. ;Mallick, A. ;Manousos, A. ;Marganiec, J. ;Martínez, T. ;Mastinu, P. ;Mastromarco, M. ;Mendoza, E. ;Mingrone, F. ;Mirea, M. ;Paradela, C. ;Pavlik, A. ;Perkowski, J. ;Praena, J. ;Quesada, J. M. ;Rauscher, T. ;Reifarth, R. ;Riego-Perez, A. ;Robles, M. ;Rubbia, C. ;Ryan, J. A. ;Sabaté-Gilarte, M. ;Sarmento, R.; ;Schmidt, S. ;Schumann, D. ;Sedyshev, P.Tain, J. L.Background: Stellar nucleosynthesis of elements heavier than iron is driven by neutron capture processes. 92Zr is positioned at a strategic point along the slow nucleosynthesis path, given its proximity to the neutron magic number N =50 and its position at the matching region between the weak and main slow processes. Purpose: In parallel with recent improved astronomical data, the extraction of accurate Maxwellian averaged cross sections (MACSs) derived from a more complete and accurate set of resonance parameters should allow for a better understanding of the stellar conditions at which nucleosynthesis takes place. Methods: Transmission and capture cross section measurements using enriched 92Zr metallic samples were performed at the time-of flight facilities GELINA of JRC-Geel (BE) and n_TOF of CERN (CH). The neutron beam passing through the samples was investigated in transmission measurements at GELINA using a Li-glass scintillator. The γ rays emitted during the neutron capture reactions were detected by C6D6 detectors at both GELINA and n_TOF. Results: Resonance parameters of individual resonances up to 81 keV were extracted from a combined resonance shape analysis of experimental transmissions and capture yields. For the majority of the resonances the parity was determined from an analysis of the transmission data obtained with different sample thicknesses. Average resonance parameters were calculated. Conclusions: Maxwellian averaged cross sections were extracted from resonances observed up to 81 keV. The MACS for k T =30 keV is fully consistent with experimental data reported in the literature. The MACSs for k T ≲15 keV are in good agreement with those derived from the ENDF/B-VIII.0 library and recommended in the KADONIS database. For k T higher than 30 keV differences are observed. A comparison with MACSs obtained with the cross sections recommended in the JEFF-3.3 and JENDL-4.0 libraries shows discrepancies even for k T ≲15 keV .64 22 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A comparison between short GRB afterglows and kilonova AT2017gfo: shedding light on kilonovae properties(2020); ; ; ;D Spighi; ; ;A Gardini; ; ; ;M Branchesi; ; ; ; ; ; ;V D’Elia; ;L Izzo ;A Perego; ; ;J Selsing; ; ; ; Multimessenger astronomy received a great boost following the discovery of kilonova (KN) AT2017gfo, the optical counterpart of the gravitational wave source GW170817 associated with the short gamma-ray burst GRB 170817A. AT2017gfo was the first KN that could be extensively monitored in time using both photometry and spectroscopy. Previously, only few candidates have been observed against the glare of short GRB afterglows. In this work, we aim to search the fingerprints of AT2017gfo-like KN emissions in the optical/NIR light curves of 39 short GRBs with known redshift. For the first time, our results allow us to study separately the range of luminosity of the blue and red components of AT2017gfo-like kilonovae in short GRBs. In particular, the red component is similar in luminosity to AT2017gfo, while the blue KN can be more than 10 times brighter. Finally, we exclude a KN as luminous as AT2017gfo in GRBs 050509B and 061201.103 22 - Some of the metrics are blocked by yourconsent settings
Product Metadata only A numerical simulation study of an astrometry case for MORFEO at the ELTWe report results from numerical simulations assessing astrometry measurements with the Multiconjugate Adaptive Optics Relay for ELT Observations (MORFEO) instrument on the Extremely Large Telescope (ELT). Using the Advanced Exposure Time Calculator (AETC), we evaluate MORFEO astrometric accuracy in moderately crowded fields. Our simulations account for spatially variable Point Spread Function (PSF), geometric distortion, and rotation-dependent variations. We computed focal plane coordinates using observed stellar distribution and computed population synthesis with the SPISEA tool, generating stellar magnitude distributions for MICADO filters at selected metallicities and stellar ages. Our analysis shows that MORFEO can achieve high-precision astrometry in the galaxy neighborhood (within μ<24 mag) by minimizing PSF enlargement and optimizing calibration strategies. These results inform future observational campaigns and contribute to the development of astrometric science cases for the ELT. - Some of the metrics are blocked by yourconsent settings
Publication Open Access The Aarhus red giants challenge. I. Stellar structures in the red giant branch phase(2020) ;Silva Aguirre, V. ;Christensen-Dalsgaard, J.; ;Miller Bertolami, M. ;Serenelli, A. ;Stello, D. ;Weiss, A. ;Angelou, G. ;Jiang, C. ;Lebreton, Y. ;Spada, F. ;Bellinger, E. P. ;Deheuvels, S. ;Ouazzani, R. M.; ;Mosumgaard, J. R. ;Townsend, R. H. D. ;Battich, T. ;Bossini, D. ;Constantino, T. ;Eggenberger, P. ;Hekker, S. ;Mazumdar, A. ;Miglio, A. ;Nielsen, K. B.Salaris, M.Context. With the advent of space-based asteroseismology, determining accurate properties of red-giant stars using their observed oscillations has become the focus of many investigations due to their implications in a variety of fields in astrophysics. Stellar models are fundamental in predicting quantities such as stellar age, and their reliability critically depends on the numerical implementation of the physics at play in this evolutionary phase.
Aims: We introduce the Aarhus red giants challenge, a series of detailed comparisons between widely used stellar evolution and oscillation codes that aim to establish the minimum level of uncertainties in properties of red giants arising solely from numerical implementations. We present the first set of results focusing on stellar evolution tracks and structures in the red-giant-branch (RGB) phase.
Methods: Using nine state-of-the-art stellar evolution codes, we defined a set of input physics and physical constants for our calculations and calibrated the convective efficiency to a specific point on the main sequence. We produced evolutionary tracks and stellar structure models at a fixed radius along the red-giant branch for masses of 1.0 M⊙, 1.5 M⊙, 2.0 M⊙, and 2.5 M⊙, and compared the predicted stellar properties.
Results: Once models have been calibrated on the main sequence, we find a residual spread in the predicted effective temperatures across all codes of ∼20 K at solar radius and ∼30-40 K in the RGB regardless of the considered stellar mass. The predicted ages show variations of 2-5% (increasing with stellar mass), which we attribute to differences in the numerical implementation of energy generation. The luminosity of the RGB-bump shows a spread of about 10% for the considered codes, which translates into magnitude differences of ∼0.1 mag in the optical V-band. We also compare the predicted [C/N] abundance ratio and find a spread of 0.1 dex or more for all considered masses.
Conclusions: Our comparisons show that differences at the level of a few percent still remain in evolutionary calculations of red giants branch stars despite the use of the same input physics. These are mostly due to differences in the energy generation routines and interpolation across opacities, and they call for further investigation on these matters in the context of using properties of red giants as benchmarks for astrophysical studies.All our evolutionary calculations and models are available at https://github.com/vsilvagui/aarhus_RG_challenge
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Publication Open Access The Aarhus red giants challenge. II. Stellar oscillations in the red giant branch phase(2020) ;Christensen-Dalsgaard, J. ;Silva Aguirre, V.; ;Miller Bertolami, M. ;Serenelli, A. ;Stello, D. ;Weiss, A. ;Angelou, G. ;Jiang, C. ;Lebreton, Y. ;Spada, F. ;Bellinger, E. P. ;Deheuvels, S. ;Ouazzani, R. M.; ;Mosumgaard, J. R. ;Townsend, R. H. D. ;Battich, T. ;Bossini, D. ;Constantino, T. ;Eggenberger, P. ;Hekker, S. ;Mazumdar, A. ;Miglio, A. ;Nielsen, K. B.Salaris, M.Contact. The large quantity of high-quality asteroseismic data that have been obtained from space-based photometric missions and the accuracy of the resulting frequencies motivate a careful consideration of the accuracy of computed oscillation frequencies of stellar models, when applied as diagnostics of the model properties.
Aims: Based on models of red-giant stars that have been independently calculated using different stellar evolution codes, we investigate the extent to which the differences in the model calculation affect the model oscillation frequencies and other asteroseismic diagnostics.
Methods: For each of the models, which cover four different masses and different evolution stages on the red-giant branch, we computed full sets of low-degree oscillation frequencies using a single pulsation code and, from these frequencies, typical asteroseismic diagnostics. In addition, we carried out preliminary analyses to relate differences in the oscillation properties to the corresponding model differences.
Results: In general, the differences in asteroseismic properties between the different models greatly exceed the observational precision of these properties. This is particularly true for the nonradial modes whose mixed acoustic and gravity-wave character makes them sensitive to the structure of the deep stellar interior and, hence, to details of their evolution. In some cases, identifying these differences led to improvements in the final models presented here and in Paper I; here we illustrate particular examples of this.
Conclusions: Further improvements in stellar modelling are required in order fully to utilise the observational accuracy to probe intrinsic limitations in the modelling and improve our understanding of stellar internal physics. However, our analysis of the frequency differences and their relation to stellar internal properties provides a striking illustration of the potential, in particular, of the mixed modes of red-giant stars for the diagnostics of stellar interiors.85 16 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The Abundance of S-Process Elements: Temporal and Spatial Trends from Open Cluster Observations(2022); ;Viscasillas Vázquez, Carlos; ;BARATELLA, MARTINA; ; ;Randich, Sofia; Spectroscopic observations of stars belonging to open clusters, with well-determined ages and distances, are a unique tool for constraining stellar evolution, nucleosynthesis, mixing processes, and, ultimately, Galactic chemical evolution. Abundances of slow (s) process neutron capture elements in stars that retain their initial surface composition open a window into the processes that generated them. In particular, they give us information on their main site of production, i.e., the low-and intermediate-mass Asymptotic Giant Branch (AGB) stars. In the present work, we review some observational results obtained during the last decade that contributed to a better understanding of the AGB phase: the growth of s-process abundances at recent epochs, i.e., in the youngest stellar populations; the different relations between age and [s/Fe] in distinct regions of the disc; and finally the use of s-process abundances combined with those of α elements, [s/α], to estimate stellar ages. We revise some implications that these observations had both on stellar and Galactic evolution, and on our ability to infer stellar ages.57 18 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Abundance ratios and IMF slopes in the dwarf elliptical galaxy NGC 1396 with MUSE(2016) ;Mentz, J. J.; ;Peletier, R. F. ;Falcón-Barroso, J. ;Lisker, T. ;van de Ven, G. ;Loubser, S. I. ;Hilker, M. ;Sánchez-Janssen, R.; ; ;Capaccioli, M. ;Norris, M.; ;Smith, R. ;Beasley, M. A. ;Lyubenova, M. ;Munoz, R.Puzia, T.Deep observations of the dwarf elliptical (dE) galaxy NGC 1396 (MV = -16.60, Mass ∼4 × 108 M☉), located in the Fornax cluster, have been performed with the Very Large Telescope/Multi Unit Spectroscopic Explorer spectrograph in the wavelength region from 4750 to 9350 Å. In this paper, we present a stellar population analysis studying chemical abundances, the star formation history (SFH) and the stellar initial mass function (IMF) as a function of galactocentric distance. Different, independent ways to analyse the stellar populations result in a luminosity-weighted age of ∼6 Gyr and a metallicity [Fe/H]∼ -0.4, similar to other dEs of similar mass. We find unusually overabundant values of [Ca/Fe] ∼+ 0.1, and underabundant Sodium, with [Na/Fe] values around -0.1, while [Mg/Fe] is overabundant at all radii, increasing from ∼+ 0.1 in the centre to ∼+ 0.2 dex. We notice a significant metallicity and age gradient within this dwarf galaxy. To constrain the stellar IMF of NGC 1396, we find that the IMF of NGC 1396 is consistent with either a Kroupa-like or a top-heavy distribution, while a bottom-heavy IMF is firmly ruled out. An analysis of the abundance ratios, and a comparison with galaxies in the Local Group, shows that the chemical enrichment history of NGC 1396 is similar to the Galactic disc, with an extended SFH. This would be the case if the galaxy originated from a Large Magellanic Cloud-sized dwarf galaxy progenitor, which would lose its gas while falling into the Fornax cluster.78 26 - Some of the metrics are blocked by yourconsent settings
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Publication Open Access The ACS LCID Project. XI. On the Early Time Resolution of SFHs of Local Group Dwarf Galaxies: Comparing the Effects of Reionization in Models with Observations(2016) ;Aparicio, Antonio ;Hidalgo, Sebastian L. ;Skillman, Evan; ;Mayer, Lucio ;Navarro, Julio ;Cole, Andrew ;Gallart, Carme ;Monelli, Matteo ;Weisz, Daniel ;Bernard, Edouard ;Dolphin, AndrewStetson, PeterThe analysis of the early star formation history (SFH) of nearby galaxies, obtained from their resolved stellar populations, is relevant as a test for cosmological models. However, the early time resolution of observationally derived SFHs is limited by several factors. Thus, direct comparison of observationally derived SFHs with those derived from theoretical models of galaxy formation is potentially biased. Here we investigate and quantify this effect. For this purpose, we analyze the duration of the early star formation activity in a sample of four Local Group dwarf galaxies and test whether they are consistent with being true fossils of the pre-reionization era; I.e., if the quenching of their star formation occurred before cosmic reionization by UV photons was completed. Two classical dSph (Cetus and Tucana) and two dTrans (LGS-3 and Phoenix) isolated galaxies with total stellar masses between 1.3× {10}6 and 7.2× {10}6 {M}☉ have been studied. Accounting for time resolution effects, the SFHs peak as much as 1.25 Gyr earlier than the optimal solutions. Thus, this effect is important for a proper comparison of model and observed SFHs. It is also shown that none of the analyzed galaxies can be considered a true fossil of the pre-reionization era, although it is possible that the outer regions of Cetus and Tucana are consistent with quenching by reionization.Based on observations made with the NASA/ESA Hubble Space Telescope, obtained at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS 5-26555. These observations are associated with program #10505.
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Publication Open Access The ACS LCID Project: On the Origin of Dwarf Galaxy Types—A Manifestation of the Halo Assembly Bias?(2015) ;Gallart, Carme ;Monelli, Matteo ;Mayer, Lucio ;Aparicio, Antonio ;Battaglia, Giuseppina ;Bernard, Edouard J.; ;Cole, Andrew A. ;Dolphin, Andrew E. ;Drozdovsky, Igor ;Hidalgo, Sebastian L. ;Navarro, Julio F.; ;Skillman, Evan D. ;Stetson, Peter B.Weisz, Daniel R.We discuss how knowledge of the whole evolutionary history of dwarf galaxies, including details on the early star formation events, can provide insight on the origin of the different dwarf galaxy types. We suggest that these types may be imprinted by the early conditions of formation rather than only being the result of a recent morphological transformation driven by environmental effects. We present precise star formation histories of a sample of Local Group dwarf galaxies, derived from color-magnitude diagrams reaching the oldest main-sequence turnoffs. We argue that these galaxies can be assigned to two basic types: fast dwarfs that started their evolution with a dominant and short star formation event and slow dwarfs that formed a small fraction of their stars early and have continued forming stars until the present time (or almost). These two different evolutionary paths do not map directly onto the present-day morphology (dwarf spheroidal versus dwarf irregular). Slow and fast dwarfs also differ in their inferred past location relative to the Milky Way and/or M31, which hints that slow dwarfs were generally assembled in lower-density environments than fast dwarfs. We propose that the distinction between a fast and slow dwarf galaxy primarily reflects the characteristic density of the environment where they form. At a later stage, interaction with a large host galaxy may play a role in the final gas removal and ultimate termination of star formation.Based on observations made with the NASA/ESA HST, which is operated by the AURA, under NASA contract NAS5-26555. Observations associated with programs #8706, #10505, and #10590.
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Publication Open Access Addendum al Documento Valutazione dei Rischi dedicato al rischio biologico derivante da Sars-CoV-2, protocollo di sicurezza anti-contagio misure di prevenzione e protezione formazione e informazione(IASF Palermo, 2020); ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; Number: 59Documento da allegare al Documento di Valutazione dei Rischi di ogni Struttura di Ricerca INAF - Istituto Nazionale di Astrofisica. Documento approvato con nota Circolare del 15 maggio 2020, numero 2482.205 127 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Additional fluorine abundance determinations in evolved stars(2019) ;Abia, C.; ;Cunha, K. ;de Laverny, P.Smith, V. V.We present new fluorine abundance measurements for a sample of carbon-rich asymptotic giant branch (AGB) stars and two other metal-poor evolved stars of Ba/CH types. The abundances are derived from IR, K-band, high-resolution spectra obtained using GEMINI-S/Phoenix and TNG/Giano-b. Our sample includes an extragalactic AGB carbon star belonging to the Sagittarius dSph galaxy. The metallicity of our stars ranges from [Fe/H] = 0.0 down to - 1.4 dex. The new measurements, together with those previously derived in similar stars, show that normal (N-type) and SC-type AGB carbon stars of near solar metallicity present similar F enhancements, discarding previous hints that suggested that SC-type stars have larger enhancements. These mild F enhancements are compatible with current chemical-evolution models pointing out that AGB stars, although relevant, are not the main sources of this element in the solar neighbourhood. Larger [F/Fe] ratios are found for lower-metallicity stars. This is confirmed by theory. We highlight a tight relation between the [F/⟨s⟩] ratio and the average s-element enhancement [⟨s⟩/Fe] for stars with [Fe/H] > -0.5, which can be explained by the current state-of-the-art low-mass AGB models assuming an extended 13C pocket. For stars with [Fe/H] < -0.5, discrepancies between observations and model predictions still exist. We conclude that the mechanism of F production in AGB stars needs further scrutiny and that simultaneous F and s-element measurements in a larger number of metal-poor AGB stars are needed to better constrain the models.56 17 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Advances and new ideas for neutron-capture astrophysics experiments at CERN n_TOF(2023) ;Domingo-Pardo, C. ;Babiano-Suarez, V. ;Balibrea-Correa, J. ;Caballero, L. ;Ladarescu, I. ;Lerendegui-Marco, J. ;Tain, J. L. ;Tarifeño-Saldivia, A. ;Aberle, O. ;Alcayne, V. ;Altieri, S. ;Pirovano, E. ;Plaza, J. ;Pomp, S. ;Porras, I. ;Praena, J. ;Quesada, J. M. ;Reifarth, R. ;Rochman, D. ;Romanets, Y. ;Rubbia, C. ;Amaducci, S. ;Sánchez, A. ;Sabaté-Gilarte, M. ;Schillebeeckx, P. ;Schumann, D. ;Sekhar, A. ;Smith, A. G. ;Sosnin, N. V. ;Stamati, M. ;Sturniolo, A. ;Tagliente, G. ;Andrzejewski, J. ;Tarrío, D. ;Torres-Sánchez, P. ;Turko, J. ;Urlass, S. ;Vagena, E. ;Valenta, S. ;Variale, V. ;Vaz, P. ;Vecchio, G.; ;Bacak, M. ;Vlachoudis, V. ;Vlastou, R. ;Wallner, T. ;Woods, P. J. ;Wright, T. ;Zarrella, R. ;Žugec, P. ;n TOF Collaboration ;Beltrami, C. ;Bennett, S. ;Bernardes, A. P. ;Berthoumieux, E. ;Boromiza, M. ;Bosnar, D. ;Caamaño, M. ;Calviño, F. ;Calviani, M. ;Cano-Ott, D. ;Casanovas, A. ;Cerutti, F.; ;Chasapoglou, S. ;Chiaveri, E. ;Chiera, N. M. ;Colombetti, P. ;Colonna, N. ;Console Camprini, P. ;Cortés, G. ;A. Cortés-Giraldo, M. ;Cosentino, L.; ;Dellmann, S. ;Di Castro, M. ;Di Maria, S. ;Diakaki, M. ;Dietz, M. ;Dressler, R. ;Dupont, E. ;Durán, I. ;Eleme, Z. ;Fargier, S. ;Fernández, B. ;Fernández-Domínguez, B. ;Finocchiaro, P. ;Fiore, S. ;García-Infantes, F. ;Gawlik-Ramiega, A. ;Gervino, G. ;Gilardoni, S. ;González-Romero, E. ;Guerrero, C. ;Gunsing, F. ;Gustavino, C. ;Heyse, J. ;Hillman, W. ;Jenkins, D. G. ;Jericha, E. ;Junghans, A. ;Kadi, Y. ;Kaperoni, K. ;Käppeler, F. ;Kaur, G. ;Kimura, A. ;Knapová, I. ;Köster, U. ;Kokkoris, M. ;Krtička, M. ;Kyritsis, N. ;Lederer-Woods, C. ;Lerner, G. ;Manna, A. ;Martínez, T. ;Masi, A. ;Massimi, C. ;Mastinu, P. ;Mastromarco, M. ;Maugeri, E. A. ;Mazzone, A. ;Mendoza, E. ;Mengoni, A. ;Milazzo, P. M. ;Mönch, I. ;Mucciola, R. ;Murtas, F. ;Musacchio-Gonzalez, E. ;Musumarra, A. ;Negret, A. ;Pérez de Rada, A. ;Pérez-Maroto, P. ;Patronis, N. ;Pavón-Rodríguez, J. A. ;Pellegriti, M. G. ;Perkowski, J.Petrone, C.This article presents a few selected developments and future ideas related to the measurement of (n ,γ ) data of astrophysical interest at CERN n_TOF. The MC-aided analysis methodology for the use of low-efficiency radiation detectors in time-of-flight neutron-capture measurements is discussed, with particular emphasis on the systematic accuracy. Several recent instrumental advances are also presented, such as the development of total-energy detectors with γ -ray imaging capability for background suppression, and the development of an array of small-volume organic scintillators aimed at exploiting the high instantaneous neutron-flux of EAR2. Finally, astrophysics prospects related to the intermediate i neutron-capture process of nucleosynthesis are discussed in the context of the new NEAR activation area.29 16 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Agb stars and their circumstellar envelopes. I. the vulcan code(2021); ; ;Gobrecht, David; The interplay between AGB interiors and their outermost layers, where molecules and dust form, is a problem of high complexity. As a consequence, physical processes like mass loss, which depend on the chemistry of the circumstellar envelope, are often oversimplified. The best candidates to drive mass-loss in AGB stars are dust grains, which trap the outgoing radiation and drag the surrounding gas. Grains build up, however, is far from being completely understood. Our aim is to model both the physics and the chemistry of the cool expanding layers around AGB stars in order to characterize the on-going chemistry, from atoms to dust grains. This has been our rationale to develop ab initio VULCAN, a FORTRAN hydro code able to follow the propagation of shocks in the circumstellar envelopes of AGB stars. The version presented in this paper adopts a perfect gas law and a very simplified treatment of the radiative transfer effects and dust nucleation. In this paper, we present preliminary results obtained with our code.38 16 - Some of the metrics are blocked by yourconsent settings
Publication Restricted Age dating of an extensive thrust system on Mercury: implications for the planet's thermal evolution(2015); ;Massironi, M. ;Marchi, S. ;Fassett, C. I.; 138 6 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Ages of the Bulge Globular Clusters NGC 6522 and NGC 6626 (M28) from HST Proper-motion-cleaned Color-Magnitude Diagrams(2018) ;Kerber, L. O. ;Nardiello, D. ;Ortolani, S. ;Barbuy, B. ;Bica, E.; ;Libralato, M.Vieira, R. G.Bulge globular clusters (GCs) with metallicities [Fe/H] ≲ -1.0 and blue horizontal branches are candidates to harbor the oldest populations in the Galaxy. Based on the analysis of HST proper-motion-cleaned color-magnitude diagrams in filters F435W and F625W, we determine physical parameters for the old bulge GCs NGC 6522 and NGC 6626 (M28), both with well-defined blue horizontal branches. We compare these results with similar data for the inner halo cluster NGC 6362. These clusters have similar metallicities (-1.3 ≤ [Fe/H] ≤ -1.0) obtained from high-resolution spectroscopy. We derive ages, distance moduli, and reddening values by means of statistical comparisons between observed and synthetic fiducial lines employing likelihood statistics and the Markov chain Monte Carlo method. The synthetic fiducial lines were generated using α-enhanced BaSTI and Dartmouth stellar evolutionary models, adopting both canonical (Y ∼ 0.25) and enhanced (Y ∼ 0.30-0.33) helium abundances. RR Lyrae stars were employed to determine the HB magnitude level, providing an independent indicator to constrain the apparent distance modulus and the helium enhancement. The shape of the observed fiducial line could be compatible with some helium enhancement for NGC 6522 and NGC 6626, but the average magnitudes of RR Lyrae stars tend to rule out this hypothesis. Assuming canonical helium abundances, BaSTI and Dartmouth models indicate that all three clusters are coeval, with ages between ∼12.5 and 13.0 Gyr. The present study also reveals that NGC 6522 has at least two stellar populations, since its CMD shows a significantly wide subgiant branch compatible with 14% ± 2% and 86% ± 5% for first and second generations, respectively. Based on observations with the NASA/ESA Hubble Space Telescope, obtained at the Space Telescope Science Institute.82 28 - Some of the metrics are blocked by yourconsent settings
Publication Open Access AGILE detection of a rapid γ-ray flare from the blazar PKS 1510-089 during the GASP-WEBT monitoring(2009); ;Pucella, G.; ; ; ; ;Donnarumma, I. ;Longo, F.; ; ;Barbiellini, G. ;Boffelli, F.; ; ;Cattaneo, P.W. ;Chen, A.W. ;Cocco, V.; ; ; ;Di Cocco, G.; ; ;Ferrari, A.; ;Froysland, T.; ;Galli, M.; ; ; ;Lapshov, I.; ;Lipari, P.; ; ;Morselli, A.; ; ;Perotti, F.; ;Picozza, P.; ;Prest, M. ;Rapisarda, M. ;Rappoldi, A. ;Sabatini, S.; ; ; ;Vallazza, E. ;Zambra, A. ;Zanello, D. ;Agudo, I. ;Aller, M.F. ;Aller, H.D. ;Arkharov, A.A. ;Bach, U. ;Benitez, E. ;Berdyugin, A. ;Blinov, D.A.; ;Chen, W.P.; ; ;Dultzin, D. ;Fuhrmann, L. ;Gómez, J.L. ;Gurwell, M.A. ;Jorstad, S.G. ;Heidt, J. ;Hiriart, D. ;Hsiao, H.Y. ;Kimeridze, G. ;Konstantinova, T.S. ;Kopatskaya, E.N. ;Koptelova, E. ;Kurtanidze, O. ;Larionov, V.M.; ;Lindfors, E. ;Lopez, J.M. ;Marscher, A.P. ;McHardy, I.M. ;Melnichuk, D.A. ;Mommert, M. ;Mujica, R. ;Nilsson, K. ;Pasanen, M. ;Roca-Sogorb, M. ;Sorcia, M. ;Takalo, L.O. ;Taylor, B.; ;Troitsky, I.S.; ; ;Colafrancesco, S. ;Cutini, S. ;Gasparrini, D.; ;Preger, B. ;Santolamazza, P.; ;Giommi, P.Salotti, L.We report the detection by the AGILE satellite of a rapid gamma-ray flare from the powerful gamma-ray quasar PKS 1510-089, during a pointing centered on the Galactic Center region from 1 March to 30 March 2008. This source has been continuosly monitored in the radio-to-optical bands by the GLAST-AGILE Support Program (GASP) of the Whole Earth Blazar Telescope (WEBT). Moreover, the gamma-ray flaring episode triggered three ToO observations by the Swift satellite in three consecutive days, starting from 20 March 2008. In the period 1-16 March 2008, AGILE detected gamma-ray emission from PKS 1510-089 at a significance level of 6.2-sigma with an average flux over the entire period of (84 +/- 17) x 10^{-8} photons cm^{-2} s^{-1} for photon energies above 100 MeV. After a predefined satellite re-pointing, between 17 and 21 March 2008, AGILE detected the source at a significance level of 7.3-sigma, with an average flux (E > 100 MeV) of (134 +/- 29) x 10^{-8} photons cm^{-2} s^{-1} and a peak level of (281 +/- 68) x 10^{-8} photons cm^{-2} s^{-1} with daily integration. During the observing period January-April 2008, the source also showed an intense and variable optical activity, with several flaring episodes and a significant increase of the flux was observed at millimetric frequencies. Moreover, in the X-ray band the Swift/XRT observations seem to show an harder-when-brighter behaviour of the source spectrum. The spectral energy distribution of mid-March 2008 is modelled with a homogeneous one-zone synchrotron self Compton emission plus contributions from inverse Compton scattering of external photons from both the accretion disc and the broad line region. Indeed, some features in the optical-UV spectrum seem to indicate the presence of Seyfert-like components, such as the little blue bump and the big blue bump.36 14 - Some of the metrics are blocked by yourconsent settings
Publication Open Access AGILE detection of extreme γ -ray activity from the blazar PKS 1510-089 during March 2009: Multifrequency analysis(2011); ; ; ; ;Pucella, G. ;Krimm, H.A.; ; ; ; ; ;Donnarumma, I.; ; ; ;Barbiellini, G. ;Boffelli, F.; ; ;Cattaneo, P.W. ;Chen, A.W. ;Cocco, V.; ; ; ;Di Cocco, G.; ; ;Ferrari, A.; ;Froysland, T. ;Frutti, M.; ;Galli, M.; ; ; ;Lapshov, I.; ;Lipari, P. ;Longo, F.; ; ;Morselli, A.; ; ;Perotti, F.; ;Picozza, P.; ;Porrovecchio, G. ;Prest, M. ;Rapisarda, M. ;Rappoldi, A. ;Rubini, A. ;Sabatini, S.; ;Striani, E.; ; ;Vallazza, E. ;Zambra, A. ;Zanello, D. ;Agudo, I. ;Aller, H.D. ;Aller, M.F. ;Arkharov, A.A. ;Bach, U. ;Benitez, E. ;Berdyugin, A. ;Blinov, D.A.; ;Chen, W.P.; ; ;Forné, E. ;Fuhrmann, L. ;Gómez, J.L. ;Gurwell, M.A. ;Jordan, B. ;Jorstad, S.G. ;Heidt, J. ;Hiriart, D. ;Hovatta, T. ;Hsiao, H.Y. ;Kimeridze, G. ;Konstantinova, T.S. ;Kopatskaya, E.N. ;Koptelova, E. ;Kurtanidze, O.M. ;Kurtanidze, S.O. ;Larionov, V.M. ;Lähteenmäki, A.; ;Lindfors, E. ;Marscher, A.P. ;McBreen, B. ;McHardy, I.M. ;Morozova, D.A. ;Nilsson, K. ;Pasanen, M. ;Roca-Sogorb, M. ;Sillanpää, A. ;Takalo, L.O. ;Tornikoski, M.; ;Troitsky, I.S.; ; ;Colafrancesco, S.; ;Santolamazza, P.; ;Giommi, P.Salotti, L.We report on the extreme gamma-ray activity from the FSRQ PKS 1510-089 observed by AGILE in March 2009. In the same period a radio-to-optical monitoring of the source was provided by the GASP-WEBT and REM. Moreover, several Swift ToO observations were triggered, adding important information on the source behaviour from optical/UV to hard X-rays. We paid particular attention to the calibration of the Swift/UVOT data to make it suitable to the blazars spectra. Simultaneous observations from radio to gamma rays allowed us to study in detail the correlation among the emission variability at different frequencies and to investigate the mechanisms at work. In the period 9-30 March 2009, AGILE detected an average gamma-ray flux of (311+/-21)x10^-8 ph cm^-2 s^-1 for E>100 MeV, and a peak level of (702+/-131)x10^-8 ph cm^-2 s^-1 on daily integration. The gamma-ray activity occurred during a period of increasing activity from near-IR to UV, with a flaring episode detected on 26-27 March 2009, suggesting that a single mechanism is responsible for the flux enhancement observed from near-IR to UV. By contrast, Swift/XRT observations seem to show no clear correlation of the X-ray fluxes with the optical and gamma-ray ones. However, the X-ray observations show a harder photon index (1.3-1.6) with respect to most FSRQs and a hint of harder-when-brighter behaviour, indicating the possible presence of a second emission component at soft X-ray energies. Moreover, the broad band spectrum from radio-to-UV confirmed the evidence of thermal features in the optical/UV spectrum of PKS 1510-089 also during high gamma-ray state. On the other hand, during 25-26 March 2009 a flat spectrum in the optical/UV energy band was observed, suggesting an important contribution of the synchrotron emission in this part of the spectrum during the brightest gamma-ray flare, therefore a significant shift of the synchrotron peak.35 11 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The AIV concept of SHARK-NIR, a new coronagraph for the Large Binocular TelescopeSHARK-NIR is one of the forthcoming instruments of the Large Binocular Telescope second generation instruments. Due to its coronagraphic nature, coupled with low resolution spectroscopy capabilities, it will be mainly devoted to exoplanetary science, but its FoV of 18 x 18 arcsec and very high contrast imaging capabilities will allow to exploit also other intriguing scientific cases. The instrument has been conceived and designed to fully exploit the exquisite adaptive optics correction delivered by the FLAO module, which will be improved with the SOUL upgrade, and will implement different coronagraphic techniques, with contrast as high as 10-6 up to 65 mas from the star. Despite the wavelength range of SHARK-NIR is 0.96-1.7 um, the instrument is designed to work in synergy with SHARK-VIS and with LMIRcam, on board of LBTI. The contemporary acquisition from these instruments will extend the wavelength coverage from M band down to the visible radiation. The physical location of the instrument, at the entrance of LBTI, imposes dimensional constraints to the instrument, which had been kept very compact. The folded optical design includes more than 50 optical elements, among which 4 Off-Axis Parabolas, 1 Deformable Mirror for the compensation of the Non Common Path Aberrations from the FLAO Wavefront Sensor, 2 detectors and 3 different kinds of coronagraph: Gaussian Lyot, Shaped Pupil and Four Quadrant Pupil Mask. Most of these optics are located onto an optical bench 500 x 400 mm, which makes SHARK-NIR an extremely dense instrument. This, together with the presence of 4 off-axis parabolas and of coronagraphs, such as the Four Quadrant, poorly tolerant to misalignments, requires a careful alignment and test phase, which needs the fine adjustement of many hundreds of degrees of freedom. We will give here an overview of the opto-mechanical layout of SHARK-NIR and of the identified alignment procedure, mostly optical, planned to take place in 2018.77 25