Browsing by Department "O.A. Palermo"
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Publication Open Access A 1.9 Earth Radius Rocky Planet and the Discovery of a Non-transiting Planet in the Kepler-20 System(2016) ;Buchhave, Lars A. ;Dressing, Courtney D. ;Dumusque, Xavier ;Rice, Ken ;Vanderburg, Andrew ;Mortier, Annelies ;Lopez-Morales, Mercedes ;Lopez, Eric ;Lundkvist, Mia S. ;Kjeldsen, Hans; ; ;Charbonneau, David ;Collier Cameron, Andrew; ;Figueira, Pedro ;Fiorenzano, Aldo F. M.; ;Haywood, Raphaëlle D. ;Johnson, John Asher ;Latham, David W. ;Lovis, Christophe; ;Mayor, Michel; ; ;Motalebi, Fatemeh; ;Pepe, Francesco ;Phillips, David F. ;Piotto, Giampaolo ;Pollacco, Don ;Queloz, Didier ;Sasselov, Dimitar ;Ségransan, Damien; ;Udry, StéphaneWatson, ChrisKepler-20 is a solar-type star (V = 12.5) hosting a compact system of five transiting planets, all packed within the orbital distance of Mercury in our own solar system. A transition from rocky to gaseous planets with a planetary transition radius of ∼1.6 R_E has recently been proposed by several articles in the literature. Kepler-20b (R_p ∼ 1.9 R_E) has a size beyond this transition radius; however, previous mass measurements were not sufficiently precise to allow definite conclusions to be drawn regarding its composition. We present new mass measurements of three of the planets in the Kepler-20 system that are facilitated by 104 radial velocity measurements from the HARPS-N spectrograph and 30 archival Keck/HIRES observations, as well as an updated photometric analysis of the Kepler data and an asteroseismic analysis of the host star (M_star = 0.948+/- 0.051 M☉ and R_star = 0.964+/- 0.018 R☉). Kepler-20b is a 1.868_(-0.034)^(+0.066) R_E planet in a 3.7 day period with a mass of 9.70_(-1.44)^(+1.41) M_E, resulting in a mean density of 8.2_(-1.3)^(+1.5) g/cm^3, indicating a rocky composition with an iron-to-silicate ratio consistent with that of the Earth. This makes Kepler-20b the most massive planet with a rocky composition found to date. Furthermore, we report the discovery of an additional non-transiting planet with a minimum mass of 19.96_(-3.61)^(+3.08) M_E and an orbital period of ∼34 days in the gap between Kepler-20f (P ∼ 11 days) and Kepler-20d (P ∼ 78 days). -- Based on observations made with the Italian Telescopio Nazionale Galileo (TNG) operated on the island of La Palma by the Fundación Galileo Galilei of the INAF (Istituto Nazionale di Astrofísica) at the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astrofísica de Canarias.152 68 - Some of the metrics are blocked by yourconsent settings
Publication Open Access An 11 Earth-mass, Long-period Sub-Neptune Orbiting a Sun-like Star(2019) ;Mayo, Andrew W. ;Rajpaul, Vinesh M. ;Buchhave, Lars A. ;Dressing, Courtney D. ;Mortier, Annelies ;Zeng, Li ;Fortenbach, Charles D. ;Aigrain, Suzanne; ;Collier Cameron, Andrew ;Charbonneau, David ;Coffinet, Adrien; ; ;Dumusque, Xavier ;Martinez Fiorenzano, A. F. ;Haywood, Raphaëlle D. ;Latham, David W. ;López-Morales, Mercedes; ; ; ;Pearce, Logan ;Pepe, Francesco ;Phillips, David ;Piotto, Giampaolo; ;Rice, Ken; Udry, StephaneAlthough several thousands of exoplanets have now been detected and characterized, observational biases have led to a paucity of long-period, low-mass exoplanets with measured masses and a corresponding lag in our understanding of such planets. In this paper we report the mass estimation and characterization of the long-period exoplanet Kepler-538b. This planet orbits a Sun-like star (V = 11.27) with {M}* ={0.892}-0.035+0.051 M ☉ and {R}* ={0.8717}-0.0061+0.0064 R ☉. Kepler-538b is a {2.215}-0.034+0.040 R ⊕ sub-Neptune with a period of P = 81.73778 ± 0.00013 days. It is the only known planet in the system. We collected radial velocity (RV) observations with the High Resolution Echelle Spectrometer (HIRES) on Keck I and High Accuracy Radial velocity Planet Searcher in North hemisphere (HARPS-N) on the Telescopio Nazionale Galileo (TNG). We characterized stellar activity by a Gaussian process with a quasi-periodic kernel applied to our RV and cross-correlation function FWHM observations. By simultaneously modeling Kepler photometry, RV, and FWHM observations, we found a semi-amplitude of K={1.68}-0.38+0.39 m s-1 and a planet mass of {M}p={10.6}-2.4+2.5 M ⊕. Kepler-538b is the smallest planet beyond P = 50 days with an RV mass measurement. The planet likely consists of a significant fraction of ices (dominated by water ice), in addition to rocks/metals, and a small amount of gas. Sophisticated modeling techniques such as those used in this paper, combined with future spectrographs with ultra high-precision and stability will be vital for yielding more mass measurements in this poorly understood exoplanet regime. This in turn will improve our understanding of the relationship between planet composition and insolation flux and how the rocky to gaseous transition depends on planetary equilibrium temperature.112 34 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 3D Hydrodynamic Modeling of SN 1987A from the SN explosion till the Athena EraThe proximity of SN 1987A and the wealth of observations collected at all wavelength bands since its outburst allow us to study in detail the transition of a supernova (SN) in a supernova remnant(SNR) and the link between the morphological properties of a SNRand the complex phases in the SN explosion. Here we investigate theinteraction between the remnant of SN 1987A and the surroundingcircumstellar medium (CSM) through three-dimensional hydrodynamic modeling. The aim is to identify the imprint of SN 1987A on the X-ray emission of its remnant and to determine the contribution of shocked ejecta and shocked CSM to the detected X-ray flux, thusproviding clues on both the ejecta and the density structure of theinhomogeneous CSM. Our model describes the evolution of the blast wave from the breakout of the shock wave at the stellar surface till its transition from SN to SNR, making predictions on the future observations of SN 1987A with the instruments on board Athena. Our model is able to reproduce alltogether the main observables of both the progenitor supernova (e.g. the bolometric lightcurve during the first 250 days) and of its remnant (X-ray lightcurves and spectra during the following 26 years of evolution), providing for the first time an accurate description of the structure of ejecta and of the CSM around the progenitor.112 19 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 3D MHD modeling of the expanding remnant of SN 1987A. Role of magnetic field and non-thermal radio emission(2019); ; ;Petruk, O. ;Ono, M. ;Nagataki, S. ;Aloy, M. A. ;Mimica, P. ;Lee, S. -H.; ; Guarrasi, M.
Aims: We investigate the role played by a pre-supernova (SN) ambient magnetic field in the dynamics of the expanding remnant of SN 1987A, and the origin and evolution of the radio emission from the remnant, in particular during the interaction of the blast wave with the nebula surrounding the SN.
Methods: We modeled the evolution of SN 1987A from the breakout of the shock wave at the stellar surface to the expansion of its remnant through the surrounding nebula using three-dimensional magnetohydrodynamic simulations. The model considers the radiative cooling, the deviations from equilibrium of ionization, the deviation from temperature-equilibration between electrons and ions, and a plausible configuration of the pre-SN ambient magnetic field. We explore the strengths of the pre-SN magnetic field ranging between 1 and 100 μG at the inner edge of the nebula and we assume an average field strength at the stellar surface B0 ≈ 3 kG. From the simulations, we synthesize the thermal X-ray and the non-thermal radio emission and compare the model results with observations.
Results: The presence of an ambient magnetic field with strength in the range considered does not change significantly the overall evolution of the remnant. Nevertheless, the magnetic field reduces the erosion and fragmentation of the dense equatorial ring after the impact of the SN blast wave. As a result, the ring survives the passage of the blast, at least during the time covered by the simulations (40 yr). Our model is able to reproduce the morphology and lightcurves of SN 1987A in both X-ray and radio bands. The model reproduces the observed radio emission if the flux originating from the reverse shock is heavily suppressed. In this case, the radio emission originates mostly from the forward shock traveling through the H II region and this may explain why the radio emission seems to be insensitive to the interaction of the blast with the ring. Possible mechanisms for the suppression of emission from the reverse shock are investigated. We find that synchrotron self-absorption and free-free absorption have negligible effects on the emission during the interaction with the nebula. We suggest that the emission from the reverse shock at radio frequencies might be limited by highly magnetized ejecta.Movies associated to Figs. 2 and 4 are available at http://www.aanda.org
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Publication Open Access 3D MHD modeling of twisted coronal loops(2016); ; ;Guarrasi, M. ;Mignone, A.; ;Hood, A. W.Priest, E. R.We perform MHD modeling of a single bright coronal loop to include the interaction with a non-uniform magnetic field. The field is stressed by random footpoint rotation in the central region and its energy is dissipated into heating by growing currents through anomalous magnetic diffusivity that switches on in the corona above a current density threshold. We model an entire single magnetic flux tube in the solar atmosphere extending from the high-β chromosphere to the low-β corona through the steep transition region. The magnetic field expands from the chromosphere to the corona. The maximum resolution is ∼30 km. We obtain an overall evolution typical of loop models and realistic loop emission in the EUV and X-ray bands. The plasma confined in the flux tube is heated to active region temperatures (∼3 MK) after ∼2/3 hr. Upflows from the chromosphere up to ∼100 km s-1 fill the core of the flux tube to densities above 109 cm-3. More heating is released in the low corona than the high corona and is finely structured both in space and time.497 19 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 3DMAP-VR, A Project to Visualize Three-dimensional Models of Astrophysical Phenomena in Virtual RealityIn this research note, we present 3DMAP-VR,(3-Dimensional Modeling of Astrophysical Phenomena in Virtual Reality), a project aimed at visualizing 3D MHD models of astrophysical simulations, using virtual reality sets of equipment. The models account for all the relevant physical processes in astrophysical phenomena: gravity, magnetic-field-oriented thermal conduction, energy losses due to radiation, gas viscosity, deviations from proton-electron temperature equilibration, deviations from the ionization equilibrium, cosmic rays acceleration, etc.. We realized an excellent synergy between our 3DMAP-VR project and Sketchfab (one of the largest open access platforms to publish and share 3D virtual reality and augmented reality content) to promote a wide dissemination of results for both scientific and public outreach purposes.123 46 - Some of the metrics are blocked by yourconsent settings
Publication Restricted A chemical survey of exoplanets with ARIEL(2018) ;Tinetti, Giovanna ;Drossart, Pierre ;Eccleston, Paul ;Hartogh, Paul ;Heske, Astrid ;Leconte, Jérémy; ;Ollivier, Marc ;Pilbratt, Göran ;Puig, Ludovic; ;Radioti, Aikaterini ;Réess, Jean-Michel ;Rezac, Ladislav ;Rocchetto, Marco ;Rosich, Albert; ; ;Santerne, Alexandre; ; ;Duong, Bastien ;Savini, Giorgio; ;Sicardy, Bruno ;Sierra, Carles; ;Skup, Konrad ;Snellen, Ignas ;Sobiecki, Mateusz; ;Soret, Lauriane ;Eales, Stephen ;Charnay, Bejamin; ;Min, Michiel ;Stiepen, A. ;Strugarek, Antoine ;Taylor, Jake ;Taylor, William; ;Tessenyi, Marcell; ;Edwards, Billy ;Brun, Allan Sacha ;Miguel, Yamila ;Tucker, C. ;Valencia, Diana ;Vasisht, Gautam ;Nørgaard-Nielsen, Hans Ulrik ;Vazan, Allona ;Vilardell, Francesc ;Vinatier, Sabrine; ; ;Waters, Rens ;Wawer, Piotr ;Pinfield, David ;Bryson, Ian ;Wawrzaszek, Anna ;Whitworth, Anthony ;Yung, Yuk L. ;Yurchenko, Sergey N. ;Rataj, Mirek ;Osorio, María Rosa Zapatero; ;Zellem, Robert; ;Zwart, Frans ;Sarkar, Subhajit ;Ray, Tom ;Bujwan, Waldemar ;Ribas, Ignasi ;Swain, Mark ;Szabo, Robert ;Werner, Stephanie ;Fletcher, Leigh ;Barstow, Joanna ;Burleigh, Matt ;Cho, James ;du Foresto, Vincent Coudé ;Selsis, Franck ;Coustenis, Athena ;Decin, Leen ;Casewell, Sarah ;Encrenaz, Therese ;Tennyson, Jonathan ;Beaulieu, Jean-Philippe ;Triaud, Amaury ;Venot, Olivia ;Waldmann, Ingo ;Waltham, David ;Wright, Gillian ;Amiaux, Jerome ;Minier, Vincent; ;Auguères, Jean-Louis ;Berthé, Michel ;Forget, François ;Bezawada, Naidu ;Bishop, Georgia ;Bowles, Neil ;Coffey, Deirdre ;Colomé, Josep ;Crook, Martin ;Crouzet, Pierre-Elie ;Morello, Giuseppe ;Da Peppo, Vania ;Vandenbussche, Bart ;Fossey, Steve ;Sanz, Isabel Escudero; ;Frericks, Martin ;Hunt, Tom ;Kohley, Ralf ;Middleton, Kevin; ;Ottensamer, Roland; ; ; ;Pearson, Chris ;Chen, Guo ;Stamper, Richard ;Symonds, Kate ;Rengel, Miriam ;Renotte, Etienne ;Ade, Peter; ;Alard, Christophe ;Narita, Norio ;Galand, Marina ;Allard, Nicole; ;André, Yves; ; ;Argyriou, Ioannis ;Aylward, Alan; ;Bakos, Gaspar ;Banaszkiewicz, Marek ;Fränz, Markus; ;Barlow, Mike ;Batista, Virginie; ; ; ;Bernardi, Pernelle ;Bézard, Bruno ;Blecka, Maria ;Bolmont, Emeline ;Fujii, Yuka ;Clédassou, Rodolphe ;Nguyen Tong, N.; ; ; ;Deroo, Pieter; ;Dominik, Carsten; ;Doublier, Vanessa ;García-Piquer, Álvaro ;Doyle, Simon ;Doyon, René; ;Drummond, Benjamin ;Gear, Walter ;Geoffray, Hervé ;Gérard, Jean Claude ;Gesa, Lluis ;Gomez, H. ;Buchave, Lars A. ;Graczyk, Rafał ;Gillon, Michael ;Lagage, Pierre-Olivier ;Griffith, Caitlin ;Grodent, Denis; ;Gustin, Jacques ;Hamano, Keiko ;Hargrave, Peter ;Hello, Yann ;Heng, Kevin ;Herrero, Enrique ;Helled, Ravit ;Ferus, Martin ;Bonfond, Bertrand ;Hornstrup, Allan ;Hubert, Benoit ;Ida, Shigeru ;Ikoma, Masahiro ;Iro, Nicolas ;Irwin, Patrick ;Jarchow, Christopher ;Jaubert, Jean ;Morales, Juan Carlos ;Jones, Hugh ;Julien, Queyrel ;Palle, Enric ;Griffin, Matt ;Kameda, Shingo ;Kerschbaum, Franz ;Kervella, Pierre ;Koskinen, Tommi ;Krijger, Matthijs ;Krupp, Norbert ;Muñoz, Antonio García ;Lafarga, Marina; ;Lellouch, Emanuel ;Palmer, Paul; ;Guedel, Manuel ;Luntzer, A. ;Rank-Lüftinger, Theresa; ;Maldonado, Jesus ;Moneti, Andrea ;Maillard, Jean-Pierre ;Mall, Urs ;Marquette, Jean-Baptiste ;Mathis, Stephane; ;Maxted, Pierre ;Matsuo, Taro ;Justtanont, Kay ;Medvedev, Alexander ;Papageorgiou, Andreas; ;Parmentier, Vivien ;Perger, Manuel; ; ;Pierrehumbert, Ray; ; ;Machado, Pedro ;Piotto, Giampaolo ;Pisano, Giampaolo ;Pascale, EnzoThousands of exoplanets have now been discovered with a huge range of masses, sizes and orbits: from rocky Earth-like planets to large gas giants grazing the surface of their host star. However, the essential nature of these exoplanets remains largely mysterious: there is no known, discernible pattern linking the presence, size, or orbital parameters of a planet to the nature of its parent star. We have little idea whether the chemistry of a planet is linked to its formation environment, or whether the type of host star drives the physics and chemistry of the planet's birth, and evolution. ARIEL was conceived to observe a large number ( 1000) of transiting planets for statistical understanding, including gas giants, Neptunes, super-Earths and Earth-size planets around a range of host star types using transit spectroscopy in the 1.25-7.8 μm spectral range and multiple narrow-band photometry in the optical. ARIEL will focus on warm and hot planets to take advantage of their well-mixed atmospheres which should show minimal condensation and sequestration of high-Z materials compared to their colder Solar System siblings. Said warm and hot atmospheres are expected to be more representative of the planetary bulk composition. Observations of these warm/hot exoplanets, and in particular of their elemental composition (especially C, O, N, S, Si), will allow the understanding of the early stages of planetary and atmospheric formation during the nebular phase and the following few million years. ARIEL will thus provide a representative picture of the chemical nature of the exoplanets and relate this directly to the type and chemical environment of the host star. ARIEL is designed as a dedicated survey mission for combined-light spectroscopy, capable of observing a large and well-defined planet sample within its 4-year mission lifetime. Transit, eclipse and phase-curve spectroscopy methods, whereby the signal from the star and planet are differentiated using knowledge of the planetary ephemerides, allow us to measure atmospheric signals from the planet at levels of 10-100 part per million (ppm) relative to the star and, given the bright nature of targets, also allows more sophisticated techniques, such as eclipse mapping, to give a deeper insight into the nature of the atmosphere. These types of observations require a stable payload and satellite platform with broad, instantaneous wavelength coverage to detect many molecular species, probe the thermal structure, identify clouds and monitor the stellar activity. The wavelength range proposed covers all the expected major atmospheric gases from e.g. H2O, CO2, CH4 NH3, HCN, H2S through to the more exotic metallic compounds, such as TiO, VO, and condensed species. Simulations of ARIEL performance in conducting exoplanet surveys have been performed - using conservative estimates of mission performance and a full model of all significant noise sources in the measurement - using a list of potential ARIEL targets that incorporates the latest available exoplanet statistics. The conclusion at the end of the Phase A study, is that ARIEL - in line with the stated mission objectives - will be able to observe about 1000 exoplanets depending on the details of the adopted survey strategy, thus confirming the feasibility of the main science objectives.176 3 - Some of the metrics are blocked by yourconsent settings
Product Metadata only A Multiwavelength, Multiepoch Monitoring Campaign of Accretion Variability in T Tauri Stars from the ODYSSEUS Survey. III. Optical Spectra(2024) ;Wendeborn, John ;Espaillat, Catherine C. ;Thanathibodee, Thanawuth ;Robinson, Connor E. ;Pittman, Caeley V. ;Calvet, Nuria ;Muzerolle, James ;Walter, Fredrick M. ;Eislöffel, Jochen; ;Manara, Carlo F. ;Kóspál, Ágnes ;Ábrahám, Péter ;Claes, Rik; ; ;Campbell-White, Justyn ;McGinnis, Pauline; ;Mauco, Karina ;Gameiro, Filipe; Guo, ZhenClassical T Tauri Stars (CTTSs) are highly variable stars that possess gas- and dust-rich disks from which planets form. Much of their variability is driven by mass accretion from the surrounding disk, a process that is still not entirely understood. A multiepoch optical spectral monitoring campaign of four CTTSs (TW Hya, RU Lup, BP Tau, and GM Aur) was conducted along with contemporaneous Hubble Space Telescope (HST) UV spectra and ground-based photometry in an effort to determine accretion characteristics and gauge variability in this sample. Using an accretion flow model, we find that the magnetospheric truncation radius varies between 2.5 and 5 R ⋆ across all of our observations. There is also significant variability in all emission lines studied, particularly Hα, Hβ, and Hγ. Using previously established relationships between line luminosity and accretion, we find that, on average, most lines reproduce accretion rates consistent with accretion shock modeling of HST spectra to within 0.5 dex. Looking at individual contemporaneous observations, however, these relationships are less accurate, suggesting that variability trends differ from the trends of the population and that these empirical relationships should be used with caution in studies of variability. * Based on observations collected at the European Southern Observatory under ESO program 106.20Z8. - Some of the metrics are blocked by yourconsent settings
Product Metadata only A Multiwavelength, Multiepoch Monitoring Campaign of Accretion Variability in T Tauri Stars from the ODYSSEUS Survey. III. Optical Spectra(2024) ;Wendeborn, John ;Espaillat, Catherine C. ;Thanathibodee, Thanawuth ;Robinson, Connor E. ;Pittman, Caeley V. ;Calvet, Nuria ;Muzerolle, James ;Walter, Fredrick M. ;Eislöffel, Jochen; ;Manara, Carlo F. ;Kóspál, Ágnes ;Ábrahám, Péter ;Claes, Rik; ; ;Campbell-White, Justyn ;McGinnis, Pauline; ;Mauco, Karina ;Gameiro, Filipe; Guo, ZhenClassical T Tauri Stars (CTTSs) are highly variable stars that possess gas- and dust-rich disks from which planets form. Much of their variability is driven by mass accretion from the surrounding disk, a process that is still not entirely understood. A multiepoch optical spectral monitoring campaign of four CTTSs (TW Hya, RU Lup, BP Tau, and GM Aur) was conducted along with contemporaneous Hubble Space Telescope (HST) UV spectra and ground-based photometry in an effort to determine accretion characteristics and gauge variability in this sample. Using an accretion flow model, we find that the magnetospheric truncation radius varies between 2.5 and 5 R ⋆ across all of our observations. There is also significant variability in all emission lines studied, particularly Hα, Hβ, and Hγ. Using previously established relationships between line luminosity and accretion, we find that, on average, most lines reproduce accretion rates consistent with accretion shock modeling of HST spectra to within 0.5 dex. Looking at individual contemporaneous observations, however, these relationships are less accurate, suggesting that variability trends differ from the trends of the population and that these empirical relationships should be used with caution in studies of variability. * Based on observations collected at the European Southern Observatory under ESO program 106.20Z8. - Some of the metrics are blocked by yourconsent settings
Product Metadata only A Multiwavelength, Multiepoch Monitoring Campaign of Accretion Variability in T Tauri Stars from the ODYSSEUS Survey. III. Optical Spectra(2024) ;Wendeborn, John ;Espaillat, Catherine C. ;Thanathibodee, Thanawuth ;Robinson, Connor E. ;Pittman, Caeley V. ;Calvet, Nuria ;Muzerolle, James ;Walter, Fredrick M. ;Eislöffel, Jochen; ;Manara, Carlo F. ;Kóspál, Ágnes ;Ábrahám, Péter ;Claes, Rik; ; ;Campbell-White, Justyn ;McGinnis, Pauline; ;Mauco, Karina ;Gameiro, Filipe; Guo, ZhenClassical T Tauri Stars (CTTSs) are highly variable stars that possess gas- and dust-rich disks from which planets form. Much of their variability is driven by mass accretion from the surrounding disk, a process that is still not entirely understood. A multiepoch optical spectral monitoring campaign of four CTTSs (TW Hya, RU Lup, BP Tau, and GM Aur) was conducted along with contemporaneous Hubble Space Telescope (HST) UV spectra and ground-based photometry in an effort to determine accretion characteristics and gauge variability in this sample. Using an accretion flow model, we find that the magnetospheric truncation radius varies between 2.5 and 5 R ⋆ across all of our observations. There is also significant variability in all emission lines studied, particularly Hα, Hβ, and Hγ. Using previously established relationships between line luminosity and accretion, we find that, on average, most lines reproduce accretion rates consistent with accretion shock modeling of HST spectra to within 0.5 dex. Looking at individual contemporaneous observations, however, these relationships are less accurate, suggesting that variability trends differ from the trends of the population and that these empirical relationships should be used with caution in studies of variability. * Based on observations collected at the European Southern Observatory under ESO program 106.20Z8. - Some of the metrics are blocked by yourconsent settings
Publication Open Access Accretion disk coronae of Intermediate Polar Cataclysmic Variables - 3D: MagnetoHydro-Dynamic modeling and thermal X-ray emission(2017) ;Barbera, Enrico; IPCVs contain a magnetic, rotating white dwarf surrounded by a magnetically truncated accretion disk. To explain their strong flickering X-ray emission, accretion has been successfully taken into account. Nevertheless, observations suggest that accretion phenomena could not be the only process behind it. An intense flaring activity occurring on the surface of the disk may generate a corona, contribute to the thermal X-ray emission and influence the system stability. Our purposes are: investigating the formation of an extended corona above the accretion disk, due to an intense flaring activity occurring on the disk surface; studying its effects on the disk and stellar magnetosphere; assessing its contribution to the observed X-ray flux. We have developed a 3D MHD model of a IPCV. The model takes into account gravity, disk viscosity, thermal conduction, radiative losses and coronal flare heating. To perform a parameter space exploration, several system conditions have been considered, with different magnetic field intensity and disk density values. From the results of the evolution of the model, we have synthesized the thermal X-ray emission. The simulations show the formation of an extended corona, linking disk and star. The flaring activity is capable of strongly influencing the disk configuration and its stability, effectively deforming the magnetic field lines. Hot plasma evaporation phenomena occur in the layer immediately above the disk. The flaring activity gives rise to a thermal X-ray emission in both the [0.1-2.0] keV and the [2.0-10] keV bands. An intense coronal activity occurring on the disk surface of an IPCV can affect the structure of the disk depending noticeably on the density of the disk and the magnetic field of the central object. Moreover, the synthesis of the thermal X-ray fluxes shows that this flaring activity may contribute to the observed thermal X-ray emission.48 19 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Accretion in young stars: measure of the stream velocity of TW Hya from the X-ray Doppler shiftHigh-resolution X-ray spectra are a unique tool to investigate the accretion process in young stars. In fact X-rays allow to investigate the accretion-shock region, where the infalling material is heated by strong shocks due to the impact with the denser stellar atmosphere. Here we show for the first time that it is possible to constrain the velocity of the accretion stream by measuring the Doppler shift of the emitted X-rays. To this aim we analyzed the deep Chandra/HETGS observation of the accreting young star TW Hya. We selected a sample of emission lines free from significant blends, fitted them with gaussian profiles, computed the radial velocity corresponding to each line, and averaged these velocities to obtain an accurate estimate of the global velocity of the X-ray emitting plasma. After correcting for Earth's motion, we compared this observed velocity with the photospheric radial velocity. In order to check this procedure we applied the same technique to other Chandra/HETGS spectra of single stars, whose X-rays are due only to coronal plasma. While spectra of pure coronal sources provide Doppler shifts in agreement with the known stellar radial velocity, we found that the X-ray spectrum of TW Hya is red-shifted by ~30-40 km/s with respect to the stellar photosphere. This proves that the X-ray emitting plasma on TW Hya is moving with respect to the stellar surface, definitively confirming that it originates in the accretion-shock region. The observed velocity suggests that the base of the accretion region is located at low latitudes of the stellar surface.73 14 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Accretion, Disks, and Magnetic Activity in the TW Hya Association(2016); ; We present new photometric and spectroscopic data for the M-type members of the TW Hya association with the aim of a comprehensive study of accretion, disks and magnetic activity at the critical age of ~ 10 Myr where circumstellar matter disappears.120 37 - Some of the metrics are blocked by yourconsent settings
Publication Open Access An Accurate Mass Determination for Kepler-1655b, a Moderately Irradiated World with a Significant Volatile Envelope(2018) ;Haywood, Raphaëlle D. ;Vanderburg, Andrew ;Mortier, Annelies ;Giles, Helen A. C. ;López-Morales, Mercedes ;Lopez, Eric D.; ;Charbonneau, David ;Collier Cameron, Andrew ;Coughlin, Jeffrey L. ;Dressing, Courtney D. ;Nava, Chantanelle ;Latham, David W. ;Dumusque, Xavier ;Lovis, Christophe; ;Pepe, Francesco; ;Udry, Stéphane ;Bouchy, François ;Johnson, John A. ;Mayor, Michel; ;Phillips, David ;Piotto, Giampaolo ;Rice, Ken ;Sasselov, Dimitar ;Ségransan, Damien ;Watson, Chris; ; ;Buchhave, Lars A. ;Ciardi, David R. ;Fiorenzano, Aldo F.We present the confirmation of a small, moderately irradiated (F = 155 ± 7 F ⊕) Neptune with a substantial gas envelope in a P = 11.8728787 ± 0.0000085 day orbit about a quiet, Sun-like G0V star Kepler-1655. Based on our analysis of the Kepler light curve, we determined Kepler-1655b’s radius to be 2.213 ± 0.082 R ⊕. We acquired 95 high-resolution spectra with Telescopio Nazionale Galileo/HARPS-N, enabling us to characterize the host star and determine an accurate mass for Kepler-1655b of 5.0{+/- }2.83.1 {M}\oplus via Gaussian-process regression. Our mass determination excludes an Earth-like composition with 98% confidence. Kepler-1655b falls on the upper edge of the evaporation valley, in the relatively sparsely occupied transition region between rocky and gas-rich planets. It is therefore part of a population of planets that we should actively seek to characterize further.64 18 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Active shape correction of a thin glass/plastic x-ray mirror(SPIE, The International Society for Optical Engineering, 2014); ; ; ; ; ;Dell'Agostino, Stefano; ;Lullo, Giuseppe ;Pelliciari, Carlo; ; Optics for future X-ray telescopes will be characterized by very large aperture and focal length, and will be made of lightweight materials like glass or plastic in order to keep the total mass within acceptable limits. Optics based on thin slumped glass foils are currently in use in the NuSTAR telescope and are being developed at various institutes like INAF/OAB, aiming at improving the angular resolution to a few arcsec HEW. Another possibility would be the use of thin plastic foils, being developed at SAO and the Palermo University. Even if relevant progresses in the achieved angular resolution were recently made, a viable possibility to further improve the mirror figure would be the application of piezoelectric actuators onto the non-optical side of the mirrors. In fact, thin mirrors are prone to deform, so they require a careful integration to avoid deformations and even correct forming errors. This however offers the possibility to actively correct the residual deformation. Even if other groups are already at work on this idea, we are pursuing the concept of active integration of thin glass or plastic foils with piezoelectric patches, fed by voltages driven by the feedback provided by X-rays, in intra-focal setup at the XACT facility at INAF/OAPA. In this work, we show the preliminary simulations and the first steps taken in this project.11 4 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Activity and rotation of the X-ray emitting Kepler stars(2017); ;Pizzocaro, D.; ; ;Belfiore, A.; ;Salvetti, D.The relation between magnetic activity and rotation periods in late-type stars provides fundamental information on the stellar dynamo and spin evolution. In spite of its importance for stellar physics, homogeneous samples of stars with accurate and sensitive measurement of both rotation period and magnetic activity have been hard to come by. The Kepler mission represents a significant step forward, providing high-cadence optical light curves for thousands of stars, from which the rotation period can be measured observing the brightness modulation due to star spots. A cross-match of the Kepler Input Catalog with the 3XMM-DR5 Catalog and subsequent careful inspection for likely non-stellar sources yields more than 100 late-type stars. We have developed an algorithm which identifies rotation periods and white-light flares in the Kepler light curves. We have calculated the X-ray luminosity from the 3XMM-DR5 count rates, and searched the light curves provided by the EXTraS (Exploring the X-ray Transient and variable Sky) FP-7 project for X-ray flares. Here we discuss the correlation between various measures for coronal and photometric activity (from the XMM-Newton and the Kepler data, respectively) and the Kepler rotation periods and Rossby number.88 26 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Activity and rotation of the X-ray emitting Kepler stars(2019) ;Pizzocaro, D.; ; ;Raetz, S.; ;Belfiore, A.; ;Salvetti, D.The relation between magnetic activity and rotation in late-type stars provides fundamental information on stellar dynamos and angular momentum evolution. Rotation-activity studies found in the literature suffer from inhomogeneity in the measurement of activity indexes and rotation periods. We overcome this limitation with a study of the X-ray emitting, late-type main-sequence stars observed by XMM-Newton and Kepler. We measured rotation periods from photometric variability in Kepler light curves. As activity indicators, we adopted the X-ray luminosity, the number frequency of white-light flares, the amplitude of the rotational photometric modulation, and the standard deviation in the Kepler light curves. The search for X-ray flares in the light curves provided by the EXTraS (Exploring the X-ray Transient and variable Sky) FP-7 project allows us to identify simultaneous X-ray and white-light flares. A careful selection of the X-ray sources in the Kepler field yields 102 main-sequence stars with spectral types from A to M. We find rotation periods for 74 X-ray emitting main-sequence stars, 20 of which do not have period reported in the previous literature. In the X-ray activity-rotation relation, we see evidence for the traditional distinction of a saturated and a correlated part, the latter presenting a continuous decrease in activity towards slower rotators. For the optical activity indicators the transition is abrupt and located at a period of 10 d but it can be probed only marginally with this sample, which is biased towards fast rotators due to the X-ray selection. We observe seven bona-fide X-ray flares with evidence for a white-light counterpart in simultaneous Kepler data. We derive an X-ray flare frequency of 0.15 d-1, consistent with the optical flare frequency obtained from the much longer Kepler time-series.69 34 - Some of the metrics are blocked by yourconsent settings
Publication Open Access ADAHELI: exploring the fast, dynamic Sun in the x-ray, optical, and near-infrared(2015); ; ; ;Sabatini, Paolo ;Bigazzi, Alberto ;Bellazzini, Ronaldo ;Bellot Rubio, Luis Ramon ;Brez, Alessandro; ; ; ; ;Curti, Fabio; ; ; ; ;Faurobert, Marianne ;Feller, Alex ;Galsgaard, Klaus ;Gburek, Szymon ;Giannattasio, Fabio; ;Hirzberger, Johann ;Jefferies, Stuart M. ;Madjarska, Maria S. ;Manni, Fabio ;Mazzoni, Alessandro; ;Penza, Valentina; ; ;Pieralli, Francesca; ;Martinez Pillet, Valentin ;Pinchera, Michele; ; ;Romoli, Andrea; ; ;Rudawy, Pawel ;Sandri, Paolo ;Scardigli, Stefano ;Spandre, Gloria ;Solanki, Sami K.; ;Vecchio, AntonioAdvanced Astronomy for Heliophysics Plus (ADAHELI) is a project concept for a small solar and space weather mission with a budget compatible with an European Space Agency (ESA) S-class mission, including launch, and a fast development cycle. ADAHELI was submitted to the European Space Agency by a European-wide consortium of solar physics research institutes in response to the "Call for a small mission opportunity for a launch in 2017," of March 9, 2012. The ADAHELI project builds on the heritage of the former ADAHELI mission, which had successfully completed its phase-A study under the Italian Space Agency 2007 Small Mission Programme, thus proving the soundness and feasibility of its innovative low-budget design. ADAHELI is a solar space mission with two main instruments: ISODY: an imager, based on Fabry-Pérot interferometers, whose design is optimized to the acquisition of highest cadence, long-duration, multiline spectropolarimetric images in the visible/near-infrared region of the solar spectrum. XSPO: an x-ray polarimeter for solar flares in x-rays with energies in the 15 to 35 keV range. ADAHELI is capable of performing observations that cannot be addressed by other currently planned solar space missions, due to their limited telemetry, or by ground-based facilities, due to the problematic effect of the terrestrial atmosphere.88 32 - Some of the metrics are blocked by yourconsent settings
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 The Advanced Virgo+ status(Institute of Physics Publishing, 2023) ;Acernese, F. ;Agathos, M. ;Ain, A. ;Albanesi, S. ;Alléné, C. ;Allocca, A. ;Amato, A. ;Andia, M. ;Andrade, T. ;Andres, N. ;Andrés-Carcasona, M. ;Andrić, T. ;Ansoldi, S. ;Antier, S. ;Apostolatos, T. ;Appavuravther, E. Z. ;Arène, M. ;Arnaud, N. ;Assiduo, M. ;Melo, S. Assis de Souza ;Astone, P. ;Aubin, F. ;Babak, S. ;Badaracco, F. ;Bagnasco, S. ;Baird, J. ;Baka, T. ;Ballardin, G. ;Baltus, G. ;Banerjee, B. ;Barneo, P. ;Barone, F. ;Barsuglia, M. ;Barta, D. ;Basti, A. ;Bawaj, M. ;Bazzan, M. ;Beirnaert, F. ;Bejger, M. ;Benedetto, V. ;Berbel, M. ;Bernuzzi, S. ;Bersanetti, D. ;Bertolini, A. ;Bhardwaj, U. ;Bianchi, A. ;Bilicki, M. ;Bini, S. ;Bischi, M. ;Bitossi, M. ;Bizouard, M. -A. ;Bobba, F. ;Boër, M. ;Bogaert, G. ;Boileau, G. ;Boldrini, M. ;Bonavena, L. D. ;Bondarescu, R. ;Bondu, F. ;Bonnand, R. ;Boschi, V. ;Boudart, V. ;Bouffanais, Y. ;Bozzi, A. ;Bradaschia, C. ;Braglia, M. ;Branchesi, M. ;Breschi, M. ;Briant, T. ;Brillet, A. ;Brooks, J.; ;Bucci, F. ;Bulashenko, O. ;Bulik, T. ;Bulten, H. J. ;Buscicchio, R. ;Buskulic, D. ;Buy, C. ;Cabras, G. ;Cabrita, R. ;Cagnoli, G. ;Calloni, E. ;Canepa, M. ;Caneva, G. ;Cannavacciuolo, M. ;Capocasa, E. ;Carapella, G. ;Carbognani, F. ;Carpinelli, M. ;Carullo, G. ;Diaz, J. Casanueva; ;Caudill, S. ;Cavalieri, R. ;Cella, G. ;Cerdá-Durán, P. ;Cesarini, E. ;Chaibi, W. ;Chanial, P. ;Chassande-Mottin, E. ;Chaty, S. ;Chessa, P. ;Chiadini, F. ;Chiarini, G. ;Chierici, R. ;Chincarini, A. ;Chiofalo, M. L. ;Chiummo, A. ;Christensen, N. ;Ciani, G. ;Ciecielag, P. ;Cieślar, M. ;Cifaldi, M.; ;Clesse, S. ;Cleva, F. ;Coccia, E. ;Codazzo, E. ;Cohadon, P. -F. ;Colombo, A. ;Colpi, M. ;Conti, L. ;Cordero-Carrión, I. ;Corezzi, S. ;Cortese, S. ;Coulon, J. -P. ;Coupechoux, J. -F. ;Croquette, M. ;Cudell, J. R. ;Cuoco, E. ;Curyło, M. ;Dabadie, P. ;Canton, T. Dal ;Dall'Osso, S. ;Dálya, G. ;D'Angelo, B. ;Danilishin, S. ;D'Antonio, S. ;Dattilo, V. ;Davier, M. ;Degallaix, J. ;Laurentis, M. De ;Deléglise, S. ;Lillo, F. De ;Dell'Aquila, D. ;Pozzo, W. Del ;Matteis, F. De ;Depasse, A. ;Pietri, R. De ;Rosa, R. De ;Rossi, C. De ;Simone, R. De ;Fiore, L. Di ;Giorgio, C. Di ;Giovanni, F. Di ;Giovanni, M. Di ;Girolamo, T. Di ;Diksha, D. ;Lieto, A. Di ;Michele, A. Di ;Pace, S. Di ;Palma, I. Di ;Renzo, F. Di ;D'Onofrio, L. ;Dooney, T. ;Dorosh, O. ;Drago, M. ;Ducoin, J. -G. ;Dupletsa, U. ;Durante, O. ;D'Urso, D. ;Duverne, P. -A.; ;Estevez, D. ;Fabrizi, F. ;Faedi, F. ;Fafone, V. ;Favaro, G. ;Fays, M. ;Fenyvesi, E. ;Ferrante, I. ;Fidecaro, F. ;Figura, P. ;Fiori, A. ;Fiori, I. ;Fittipaldi, R. ;Fiumara, V. ;Flaminio, R. ;Font, J. A. ;Frasca, S. ;Frasconi, F. ;Freise, A. ;Freitas, O. ;Fronzé, G. G. ;Gadre, B. ;Gamba, R. ;Garaventa, B. ;Garcia-Bellido, J. ;Gargiulo, J. ;Garufi, F. ;Gasbarra, C. ;Gemme, G. ;Gennai, A. ;Ghosh, Archisman ;Giacoppo, L. ;Giri, P. ;Gissi, F. ;Gkaitatzis, S. ;Glotin, F. ;Goncharov, B. ;Gosselin, M. ;Gouaty, R.; ;Granata, M. ;Granata, V. ;Greco, G. ;Grignani, G. ;Grimaldi, A. ;Guerra, D. ;Guetta, D. ;Guidi, G. M. ;Gulminelli, F. ;Guo, Y. ;Gupta, P. ;Gutierrez, N. ;Haegel, L. ;Halim, O. ;Hannuksela, O. ;Harder, T. ;Haris, K. ;Harmark, T. ;Harms, J. ;Haskell, B. ;Heidmann, A. ;Heitmann, H. ;Hello, P. ;Hemming, G. ;Hennes, E. ;Hennig, J. -S. ;Hennig, M. ;Hild, S. ;Hofman, D. ;Holland, N. A. ;Hui, V. ;Iandolo, G. A. ;Idzkowski, B. ;Iess, A. ;Iorio, G. ;Iosif, P. ;Jacqmin, T. ;Jacquet, P. -E. ;Janquart, J. ;Janssens, K. ;Jaraba, S. ;Jaranowski, P. ;Jasal, P. ;Juste, V. ;Kalaghatgi, C. ;Karathanasis, C. ;Katsanevas, S. ;Kéfélian, F. ;Koekoek, G. ;Koley, S. ;Kolstein, M. ;Kranzhoff, S. L. ;Królak, A. ;Kuijer, P. ;Kuroyanagi, S. ;Lagabbe, P. ;Laghi, D. ;Lalleman, M. ;Lamberts, A. ;Rana, A. La ;Rosa, I. La ;Lartaux-Vollard, A. ;Lazzaro, C. ;Leaci, P. ;Lemaître, A. ;Lenti, M. ;Leonova, E. ;Leroy, N. ;Letendre, N. ;Lethuillier, M. ;Leyde, K. ;Linde, F. ;London, L. ;Longo, A. ;Lopez Portilla, M. ;Lorenzini, M. ;Loriette, V. ;Losurdo, G. ;Lumaca, D. ;Macquet, A. ;Magazzù, C. ;Maggiore, R. ;Magnozzi, M. ;Majorana, E. ;Man, N.; ;Mantovani, M. ;Mapelli, M. ;Marchesoni, F. ;Marín Pina, D. ;Marion, F. ;Marquina, A. ;Marsat, S. ;Martelli, F. ;Martinez, M. ;Martinez, V. ;Masserot, A. ;Mastrodicasa, M. ;Mastrogiovanni, S. ;Meijer, Q. ;Menendez-Vazquez, A. ;Mereni, L. ;Merzougui, M. ;Miani, A. ;Michel, C. ;Miller, A. ;Miller, B. ;Milotti, E. ;Minenkov, Y. ;Mir, Ll. M. ;Miravet-Tenés, M. ;Mitchell, A. L. ;Mondal, C. ;Montani, M. ;Morawski, F. ;Morras, G. ;Mours, B. ;Mow-Lowry, C. M. ;Muciaccia, F. ;Mukherjee, Suvodip ;Nagar, A. ;Napolano, V. ;Nardecchia, I. ;Narola, H. ;Naticchioni, L. ;Neilson, J. ;Nesseris, S. ;Nguyen, C. ;Nieradka, G. ;Nissanke, S. ;Nitoglia, E. ;Nocera, F. ;Novak, J. ;Nuño Siles, J. F. ;Oertel, M. ;Oganesyan, G. ;Oliveri, R. ;Orselli, M. ;Palomba, C. ;Pang, P. T. H. ;Pannarale, F. ;Paoletti, F. ;Paoli, A. ;Paolone, A. ;Pappas, G. ;Parisi, A. ;Pascucci, D. ;Pasqualetti, A. ;Passaquieti, R. ;Passuello, D. ;Patricelli, B. ;Pedurand, R. ;Pegna, R. ;Pegoraro, M. ;Perego, A. ;Pereira, A. ;Périgois, C. ;Perreca, A. ;Perriès, S. ;Perry, J. W. ;Pesios, D. ;Petrillo, C. ;Phukon, K. S. ;Piccinni, O. J. ;Pichot, M. ;Piendibene, M. ;Piergiovanni, F. ;Pierini, L. ;Pierra, G. ;Pierro, V. ;Pillant, G. ;Pillas, M. ;Pilo, F. ;Pinard, L. ;Pinto, I. M. ;Pinto, M. ;Piotrzkowski, K. ;Placidi, A. ;Placidi, E. ;Plastino, W. ;Poggiani, R. ;Polini, E. ;Porcelli, E. ;Portell, J. ;Porter, E. K. ;Poulton, R. ;Pracchia, M. ;Pradier, T. ;Principe, M. ;Prodi, G. A. ;Prosposito, P. ;Puecher, A. ;Punturo, M. ;Puosi, F. ;Puppo, P. ;Raaijmakers, G. ;Radulesco, N. ;Rapagnani, P. ;Razzano, M. ;Regimbau, T. ;Rei, L. ;Rettegno, P. ;Revenu, B. ;Reza, A. ;Rezaei, A. S. ;Ricci, F. ;Rinaldi, S. ;Robinet, F. ;Rocchi, A. ;Rolland, L. ;Romanelli, M. ;Romano, R. ;Romero, A. ;Ronchini, S. ;Rosa, L. ;Rosińska, D. ;Roy, S. ;Rozza, D. ;Ruggi, P. ;Ruiz Morales, E. ;Saffarieh, P.; ;Salconi, L.; ;Sallé, M. ;Samajdar, A. ;Sanchis-Gual, N. ;Sanuy, A. ;Sasli, A. ;Sassi, P. ;Sassolas, B. ;Sayah, S. ;Schmidt, S. ;Seglar-Arroyo, M. ;Sentenac, D. ;Sequino, V. ;Servignat, G. ;Setyawati, Y. ;Shcheblanov, N. S. ;Sieniawska, M. ;Silenzi, L. ;Singh, N. ;Singha, A. ;Sipala, V. ;Soldateschi, J. ;Sordini, V. ;Sorrentino, F. ;Sorrentino, N. ;Soulard, R. ;Spagnuolo, V. ;Spera, M. ;Spinicelli, P. ;Stachie, C. ;Steer, D. A. ;Steinlechner, J. ;Steinlechner, S. ;Stergioulas, N.; ;Suchenek, M. ;Sur, A. ;Suresh, J. ;Swinkels, B. L. ;Syx, A. ;Szewczyk, P. ;Tacca, M. ;Tamanini, N. ;Tanasijczuk, A. J. ;Tapia San Martín, E. N. ;Taranto, C. ;Tonelli, M. ;Torres-Forné, A. ;Melo, I. Tosta e. ;Tournefier, E. ;Trapananti, A. ;Travasso, F. ;Trenado, J. ;Tringali, M. C. ;Troiano, L. ;Trovato, A. ;Trozzo, L. ;Tsang, K. W. ;Turbang, K. ;Turconi, M. ;Turski, C. ;Ubach, H. ;Utina, A. ;Valentini, M. ;Vallero, S. ;van Bakel, N. ;van Beuzekom, M. ;van Dael, M. ;van den Brand, J. F. J. ;Van Den Broeck, C. ;van der Sluys, M. ;Van de Walle, A. ;van Dongen, J. ;van Haevermaet, H. ;van Heijningen, J. V. ;van Ranst, Z. ;van Remortel, N. ;Vardaro, M. ;Vasúth, M. ;Vedovato, G. ;Verdier, P. ;Verkindt, D. ;Verma, P. ;Vetrano, F. ;Viceré, A. ;Vinet, J. -Y. ;Viret, S. ;Virtuoso, A. ;Vocca, H. ;Walet, R. C. ;Was, M. ;Yadav, N. ;Zadrożny, A. ;Zelenova, T.Zendri, J. -P.The gravitational wave detector Advanced Virgo+ is currently in the commissioning phase in view of the fourth Observing Run (O4).15 7