V. Bozza’s research while affiliated with University of Salerno and other places

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Publications (318)


VBMicroLensing: three algorithms for multiple lensing with contour integration
  • Preprint

October 2024

V. Bozza

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V. Saggese

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G. Covone

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[...]

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J. Zhang

Modeling of microlensing events poses computational challenges for the resolution of the lens equation and the high dimensionality of the parameter space. In particular, numerical noise represents a severe limitation to fast and efficient calculations of microlensing by multiple systems, which are of particular interest in exoplanetary searches. We present a new public code built on our previous experience on binary lenses that introduces three new algorithms for the computation of magnification and astrometry in multiple microlensing. Besides the classical polynomial resolution, we introduce a multi-polynomial approach in which each root is calculated in a frame centered on the closest lens. In addition, we propose a new algorithm based on a modified Newton-Raphson method applied to the original lens equation without any numerical manipulation. These new algorithms are more accurate and robust compared to traditional single-polynomial approaches at a modest computational cost, opening the way to massive studies of multiple lenses. The new algorithms can be used in a complementary way to optimize efficiency and robustness.


Euclid. I. Overview of the Euclid mission

September 2024

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115 Reads

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34 Citations

Astronomy and Astrophysics

The current standard model of cosmology successfully describes a variety of measurements, but the nature of its main ingredients, dark matter and dark energy, remains unknown. is a medium-class mission in the Cosmic Vision 2015--2025 programme of the European Space Agency (ESA) that will provide high-resolution optical imaging, as well as near-infrared imaging and spectroscopy, over about 14\,000\,deg2^2 of extragalactic sky. In addition to accurate weak lensing and clustering measurements that probe structure formation over half of the age of the Universe, its primary probes for cosmology, these exquisite data will enable a wide range of science. This paper provides a high-level overview of the mission, summarising the survey characteristics, the various data-processing steps, and data products. We also highlight the main science objectives and expected performance.


Strong deflection limit analysis of black hole lensing in inhomogeneous plasma

September 2024

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8 Reads

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3 Citations

Physical Review D

This paper investigates gravitational lensing effects in the presence of plasma in the strong deflection limit, which corresponds to light rays circling around a compact object and forming higher-order images. While previous studies of this case have predominantly focused on the deflection of light in a vacuum or in the presence of a homogeneous plasma, this work introduces an analytical treatment for the influence of a nonuniform plasma. After recalling the exact expression for the deflection angle of photons in a static, asymptotically flat and spherically symmetric spacetime filled with cold nonmagnetized plasma, a strong deflection limit analysis is presented. Particular attention is then given to the case of a Schwarzschild spacetime, where the deflection angle of photons for different density profiles of plasma is obtained. Moreover, perturbative results for an arbitrary power-law radial density profile are also presented. These formulas are then applied to the calculation of the positions and magnifications of higher-order images, concluding that the presence of a nonuniform plasma reduces both their angular size and their magnifications, at least within the range of the power-law indices considered. These findings contribute to the understanding of gravitational lensing in the presence of plasma, offering a versatile framework applicable to various asymptotically flat and spherically symmetric spacetimes.


Fig. 1: Histogram of observations obtained after the stacking in the field of the GC Terzan 5. The colors represent the images obtained for each year: black (group 1) is 2014, blue (group 2) is 2015, green (group 3) is 2016, olive (group 4) is 2017, purple (group 5) is 2019, and pink (group 6) is 2021.
Frequencies found in the analysis of the stars classified as semiregular variables
Digging deeper into the dense Galactic globular cluster Terzan 5 with electron-multiplying CCDs. Variable star detection and new discoveries
  • Article
  • Full-text available

July 2024

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22 Reads

Astronomy and Astrophysics

Context . High frame-rate imaging was employed to mitigate the effects of atmospheric turbulence (seeing) in observations of globular cluster Terzan 5. Aims . High-precision time-series photometry with the highest angular resolution so far has been obtained for the crowded central region of Terzan 5. Observations were carried out using ground-based telescopes, implementing ways to avoid saturation of the brightest stars in the field observed. Methods . The Electron-Multiplying Charge Coupled Device (EMCCD) camera installed at the Danish 1.54 m telescope at the ESO La Silla Observatory was used to produce thousands of short-exposure time images (ten images per second), which were stacked to produce the normal-exposure-time images (minutes). We employed difference image analysis in the stacked images to produce high-precision photometry using the DanDIA pipeline. Results . We analyzed the light curves of 1670 stars with 242 epochs in the crowded central region of Terzan 5 in order to statistically detect variable stars in the field observed. We present a possible visual counterpart outburst at the position of the pulsar J1748-2446N, and the visual counterpart light curve of the low-mass X-ray binary CX 3. Additionally, we present the discovery of four semiregular variables. We also present updated ephemerides and properties of the only RR Lyrae star previously known in the field covered by our observations in Terzan 5. Finally, we report a significant displacement of two sources by ~0.62 and 0.59 arcsec with respect to their positions in previous images available in the literature.

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Analytical perturbations of relativistic images in Kerr space-time

July 2024

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9 Reads

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2 Citations

Light rays passing very close to black holes may wind several times before escaping. For any given electromagnetic source around the black hole, a distant observer would thus observe two infinite sequences of images on either side of the black hole. These images are generated by light rays performing an increasing numbers of loops. The strong deflection limit provides a simple analytic formalism to describe such higher order images for spherically symmetric metrics, while for axially symmetric black holes one typically resorts to numerical approaches. Here we present the leading order perturbation to higher order images when the black hole spin is turned on. We show that the images slide around the black hole shadow as an effect of space-time dragging. We derive analytical formulae for their shifts and the perturbation of their time delays. We also discuss how such simple analytical formulae for images by Kerr black holes can be of great help in many applications.


Figure 1. Gaia22dkv's light curve and the best-fit planetary microlensing model (black solid line) considering microlens parallax and orbital motion effects. Data points observed by various sites are shown as open circles in different colors, respectively. The magnitudes are transformed into the ¢ i band using the magnifications from the best-fit model. The inset panel presents the zoomed-in view of the region in the neighborhood of the planetary anomaly. The gray line represents the best-fit binary-source (1L2S) model, which fails to match the anomaly.
Figure 2. Two degenerate microlens parallax solutions from PSPL analysis of the light curve with the region in the neighborhood of the planet anomaly removed. The upper and the lower panels display the u 0 + and u 0 − grid-search results, respectively. The solutions with Δχ 2 < 1, 4, 9, 16, 25, and >25 of the best fit are color coded with red, yellow, green, blue, cyan, and gray. The insets display zoomed-in views.
Figure 3. Δχ 2 map of the binary-lens point-source grid-search results on the ( ) s q log , log and ( ) a q , log planes. The upper and lower panels show u 0 + and u 0 − grid searches, respectively. The solutions with Δχ 2 < 50, 200, 450, 800, 1250, and >1250 compared with the best fits (c » 868 min 2 for u 0 + and c » 690 min 2 for u 0 −) are color coded with red, yellow, green, blue, gray, and light gray, respectively.
Figure 4. (For u 0 + cases) The source trajectories and light curves in the neighborhood of the planet anomaly for several u 0 + solutions. Left: The upper and middle panels show the caustics and source trajectories for solutions UPS−3.8, UPS−3.3 (the global best-fit solution), and LFS−2.6, respectively. The trajectories with arrows indicating the direction of motion are plotted with respect to the binary-lens axis. The insets of each subpanel on the left display the caustics (blue) and source position (red) at t 0,kep −1 day, t 0,kep and t 0,kep + 1 day with increasing opacities. The radii of the red circles indicate the best-fit source sizes (upper limits) for the FS (PS) solutions. Right: The light curves and best-fit models of the four solutions (UPS−3.8: dotted line, UPS−3.3: solid lines, LFS−2.6: dashed lines) are shown in the upper panel. The residuals are displayed in the lower panel.
Figure 15. Posteriors of astrometric lensing model parameters from MCMC sampling. The red, yellow, green, and blue areas represent Δχ 2 within 1, 4, 9, and 16 of the best fit. The model parameters with light-curve priors, i.e., (t 0 , u 0 , t E , f B /f S ), are not shown.
Gaia22dkvLb: A Microlensing Planet Potentially Accessible to Radial-velocity Characterization

July 2024

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70 Reads

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2 Citations

The Astronomical Journal

We report discovering an exoplanet from following up a microlensing event alerted by Gaia. The event Gaia22dkv is toward a disk source rather than the traditional bulge microlensing fields. Our primary analysis yields a Jovian planet with M p = 0.59 − 0.05 + 0.15 M J at a projected orbital separation r ⊥ = 1.4 − 0.3 + 0.8 au, and the host is a ∼1.1 M ⊙ turnoff star at ∼1.3 kpc. At r ′ ≈ 14 , the host is far brighter than any previously discovered microlensing planet host, opening up the opportunity to test the microlensing model with radial velocity (RV) observations. RV data can be used to measure the planet’s orbital period and eccentricity, and they also enable searching for inner planets of the microlensing cold Jupiter, as expected from the “inner–outer correlation” inferred from Kepler and RV discoveries. Furthermore, we show that Gaia astrometric microlensing will not only allow precise measurements of its angular Einstein radius θ E but also directly measure the microlens parallax vector and unambiguously break a geometric light-curve degeneracy, leading to the definitive characterization of the lens system.


Digging deeper into the dense Galactic globular cluster Terzan 5 with Electron-Multiplying CCDs. Variable star detection and new discoveries

June 2024

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13 Reads

Context. High frame-rate imaging was employed to mitigate the effects of atmospheric turbulence (seeing) in observations of globular cluster Terzan 5. Aims. High-precision time-series photometry has been obtained with the highest angular resolution so far taken in the crowded central region of Terzan 5, with ground-based telescopes, and ways to avoid saturation of the brightest stars in the field observed. Methods. The Electron-Multiplying Charge Coupled Device (EMCCD) camera installed at the Danish 1.54-m telescope at the ESO La Silla Observatory was employed to produce thousands of short-exposure time images (ten images per second) that were stacked to produce the normal-exposure-time images (minutes). We employed difference image analysis in the stacked images to produce high-precision photometry using the DanDIA pipeline. Results. Light curves of 1670 stars with 242 epochs were analyzed in the crowded central region of Terzan 5 to statistically detect variable stars in the field observed. We present a possible visual counterpart outburst at the position of the pulsar J1748-2446N, and the visual counterpart light curve of the low-mass X-ray binary CX 3. Additionally, we present the discovery of 4 semiregular variables. We also present updated ephemerides and properties of the only RR Lyrae star previously known in the field covered by our observations in Terzan 5. Finally, we report a significant displacement of two sources by ~0.62 and 0.59 arcseconds with respect to their positions in previous images available in the literature.


Four microlensing giant planets detected through signals produced by minor-image perturbations

June 2024

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7 Reads

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1 Citation

Astronomy and Astrophysics

Aims. We investigated the nature of the anomalies appearing in four microlensing events KMT-2020-BLG-0757, KMT-2022-BLG-0732, KMT-2022-BLG-1787, and KMT-2022-BLG-1852. The light curves of these events commonly exhibit initial bumps followed by subsequent troughs that extend across a substantial portion of the light curves. Methods. We performed thorough modeling of the anomalies to elucidate their characteristics. Despite their prolonged durations, which differ from the usual brief anomalies observed in typical planetary events, our analysis revealed that each anomaly in these events originated from a planetary companion located within the Einstein ring of the primary star. It was found that the initial bump arouse when the source star crossed one of the planetary caustics, while the subsequent trough feature occurred as the source traversed the region of minor image perturbations lying between the pair of planetary caustics. Results. The estimated masses of the host and planet, their mass ratios, and the distance to the discovered planetary systems are ( M host / M ⊙ , M planet /M J , q /10 ⁻³ , D L /kpc) = (0.58 −0.30 +0.33 , 10.71 −5.61 +6.17 , 17.61 ± 2.25, 6.67 −1.30 +0.93 ) for KMT-2020-BLG-0757, (0.53 −0.31 +0.31 , 1.12 −0.65 +0.65 , 2.01 ± 0.07, 6.66 −1.84 +1.19 ) for KMT-2022-BLG-0732, (0.42 −0.23 +0.32 , 6.64 −3.64 +4.98 , 15.07 ± 0.86, 7.55 −1.30 +0.89 ) for KMT-2022-BLG-1787, and (0.32 −0.19 +0.34 , 4.98 −2.94 +5.42 , 8.74 ± 0.49, 6.27 −1.15 +0.90 ) for KMT-2022-BLG-1852. These parameters indicate that all the planets are giants with masses exceeding the mass of Jupiter in our solar system and the hosts are low-mass stars with masses substantially less massive than the Sun.


Four microlensing giant planets detected through signals produced by minor-image perturbations

June 2024

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17 Reads

We investigated the nature of the anomalies appearing in four microlensing events KMT-2020-BLG-0757, KMT-2022-BLG-0732, KMT-2022-BLG-1787, and KMT-2022-BLG-1852. The light curves of these events commonly exhibit initial bumps followed by subsequent troughs that extend across a substantial portion of the light curves. We performed thorough modeling of the anomalies to elucidate their characteristics. Despite their prolonged durations, which differ from the usual brief anomalies observed in typical planetary events, our analysis revealed that each anomaly in these events originated from a planetary companion located within the Einstein ring of the primary star. It was found that the initial bump arouse when the source star crossed one of the planetary caustics, while the subsequent trough feature occurred as the source traversed the region of minor image perturbations lying between the pair of planetary caustics. The estimated masses of the host and planet, their mass ratios, and the distance to the discovered planetary systems are (M_{\rm host}/M_\odot, M_{\rm planet}/M_{\rm J}, q/10^{-3}, \dl/{\rm kpc}) = (0.58^{+0.33}_{-0.30}, 10.71^{+6.17}_{-5.61}, 17.61\pm 2.25,6.67^{+0.93}_{-1.30}) for KMT-2020-BLG-0757, (0.530.31+0.31,1.120.65+0.65,2.01±0.07,6.661.84+1.19)(0.53^{+0.31}_{-0.31}, 1.12^{+0.65}_{-0.65}, 2.01 \pm 0.07, 6.66^{+1.19}_{-1.84}) for KMT-2022-BLG-0732, (0.420.23+0.32,6.643.64+4.98,15.07±0.86,7.551.30+0.89)(0.42^{+0.32}_{-0.23}, 6.64^{+4.98}_{-3.64}, 15.07\pm 0.86, 7.55^{+0.89}_{-1.30}) for KMT-2022-BLG-1787, and (0.320.19+0.34,4.982.94+5.42,8.74±0.49,6.271.15+0.90)(0.32^{+0.34}_{-0.19}, 4.98^{+5.42}_{-2.94}, 8.74\pm 0.49, 6.27^{+0.90}_{-1.15}) for KMT-2022-BLG-1852. These parameters indicate that all the planets are giants with masses exceeding the mass of Jupiter in our solar system and the hosts are low-mass stars with masses substantially less massive than the Sun.


Strong deflection limit analysis of black hole lensing in inhomogeneous plasma

June 2024

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4 Reads

This paper investigates gravitational lensing effects in the presence of plasma in the strong deflection limit, which corresponds to light rays circling around a compact object and forming higher-order images. While previous studies of this case have predominantly focused on the deflection of light in a vacuum or in the presence of a homogeneous plasma, this work introduces an analytical treatment for the influence of a non-uniform plasma. After recalling the exact expression for the deflection angle of photons in a static, asymptotically flat and spherically symmetric spacetime filled with cold non-magnetized plasma, a strong deflection limit analysis is presented. Particular attention is then given to the case of a Schwarzschild spacetime, where the deflection angle of photons for different density profiles of plasma is obtained. Moreover, perturbative results for an arbitrary power-law radial density profile are also presented. These formulae are then applied to the calculation of the positions and magnifications of higher-order images, concluding that the presence of a non-uniform plasma reduces both their angular size and their magnifications, at least within the range of the power-law indices considered. These findings contribute to the understanding of gravitational lensing in the presence of plasma, offering a versatile framework applicable to various asymptotically flat and spherically symmetric spacetimes.


Citations (44)


... We generate two distinct sets of galactic mock catalogues that differ in their covered redshift ranges, as well as in their evolution and magnification biases. The first set of mock catalogues mimics the expected distribution of galaxies that the Euclid mission [33] will measure, while the second set is based on the 21cm neutral hydrogen galaxy population targeted by the extension of the Square Kilometre Array Observatory [SKAO2,90]. In our analysis, we assume that these catalogues cover the entire sky, although we demonstrate that the FOTO signal remains measurable even for partial sky coverage. ...

Reference:

Measuring our peculiar velocity from spectroscopic redshift surveys
Euclid. I. Overview of the Euclid mission
  • Citing Article
  • September 2024

Astronomy and Astrophysics

... Notable examples include the Van der Waals black hole [75], Kerr black hole [76], Simpson-Visser black hole [77], acoustic charged black hole [74,78], hairy Kerr black hole [40], Kerr-Taub-NUT-Quintessence black hole [79], Kerr-Taub-NUT spacetime [80], Bardeen black hole [81], Reissner-Nordström (RN) black hole [82], and black holes from the Horndeski theory of gravity [83], among others. Gravitational lensing effects induced by various black holes have been studied both numerically and an-alytically in the strong-field limit [84][85][86]. Kumar et al. [60] analyzed the strong gravitational lensing effects of a hairy black hole in Horndeski theory of gravity. They discussed the astrophysical consequences of various supermassive black holes due to the presence of hair in this theory and compared the results with those for the standard Schwarzschild black hole in general relativity. ...

Strong deflection limit analysis of black hole lensing in inhomogeneous plasma
  • Citing Article
  • September 2024

Physical Review D

... Their findings revealed a profusion of images distributed symmetrically around the optic axis, a consequence of the profound gravitational influence experienced by light rays. Some further studies of images arising due to lensing by a black hole, explicitly, the Kerr one, can be found also in [31]. ...

Analytical perturbations of relativistic images in Kerr space-time

... As described in Section 6.2, there are a number of difficulties to comparing directly with observed data in an SBI framework. In future work we will overcome a number of these limitations, at which point the method will be directly applicable to a number of future surveys, such as Euclid (Euclid-Collaboration et al. 2024) and LSST (Ivezić et al. 2019), containing billions of sources. and dust attenuated emission. ...

Euclid. I. Overview of the Euclid mission

... The article is concerned the demonstration of possibilities of MASTER global robotic telescopes network of Lomonosov Moscow State University images archive, that is collected almost 20 years in identical photometry system, can provide unique data in many fields of astronomy: not only in studying optical counterparts of high energy phenomena but also in exoplanet research, variable stars investigations, progenitors of Supernova and other events search, asteroids parameters calculations, and other actual astronomical problems [33][34][35][36][37][38][39][40][41][42][43][44][45]. MASTER archive can provide unique light curves of exoplanet transit events, obtained by MASTER Robotic Net long before other ground-based and space observations (TESS in current article). ...

Identification of the Top TESS Objects of Interest for Atmospheric Characterization of Transiting Exoplanets with JWST

The Astronomical Journal

... As a result, the observed T eff of the post-subtraction stellar spectrum rapidly increases and then slowly decays during a flare and follows a fast-rise, exponential decay (FRED) temporal profile. Conversely, variations in the residual spectrum resulting from a spot-crossing event occur more slowly and with a symmetrical temporal profile well-described by a Gaussian (e.g., Béky et al. 2014;Schutte et al. 2023;Biagiotti et al. 2024). Furthermore, a flare spectrum is brightest at near-UV and blue optical wavelengths (0.2-0.5 µm), placing the NIRISS/SOSS wavelength range in the Rayleigh-Jeans tail during the flare peak. ...

Star-spot activity, orbital obliquity, transmission spectrum, physical properties, and transit time variations of the HATS-2 planetary system

Astronomy and Astrophysics

... Other applications of machine learning used to find comets and future developments Machine learning methods are becoming increasingly used in the detection and discovery of comets that have come out after the development of CNN-based methods like Tails (e.g., Rożek et al., 2023;Sedaghat et al., 2024). Future developments and improvements to CCN-based methods like Tails include the use of multiple-input CNNs, such as the BTSBot, implemented for identifying supernovae in ZTF images (Rehemtulla et al., 2023). ...

Optical Monitoring of the Didymos–Dimorphos Asteroid System with the Danish Telescope around the DART Mission Impact

The Planetary Science Journal

... influence from systematics. Indeed, for many microlensing events of interest, models with Xallarap may compete with models with Parallax and cannot be excluded easily (e.g., see N. Miyake et al. 2012;N. Koshimoto et al. 2017; P. Rota et al. 2021;Y. K. Satoh et al. 2023). The Xallarap+Parallax model could be ruled out if the source has a mass incompatible with the observed flux in follow-up imaging (A. Bhattacharya et al. 2017Bhattacharya et al. , 2020J. W. Blackman et al. 2021). Furthermore, during lightcurve fitting, if a Xallarap+Parallax model returns an orbital period of 1 yr, there is a high chan ...

OGLE-2019-BLG-0825: Constraints on the Source System and Effect on Binary-lens Parameters Arising from a Five-day Xallarap Effect in a Candidate Planetary Microlensing Event

The Astronomical Journal

... This has enabled microlensing to detect the first Jupiter-like planet in a Jupiter-like orbit around a white dwarf (Blackman et al. 2021). It has also enabled the discovery of planets with no evidence for any host star (Mróz et al. 2018(Mróz et al. , 2019(Mróz et al. , 2020aRyu et al. 2021;Kim et al. 2021;Koshimoto et al. 2023), implying that they are likely to be unbound from any host star, although some could certainly be in wide orbits about host stars. Two of these candidate free-floating planets are likely to have masses slightly lower than an Earth-mass (Mróz et al. 2020b;Koshimoto et al. 2023), and a statistical analysis implies that these planets are likely to be 6 +6 −4 times more common than the known populations of bound planets ). ...

Terrestrial- and Neptune-mass Free-Floating Planet Candidates from the MOA-II 9 yr Galactic Bulge Survey

The Astronomical Journal

... A traditional assumption is (m, r) = (0, 0), and it has been implicitly or explicitly assumed in many studies to date (e.g., Bennett et al. 2014;Shvartzvald et al. 2014;Shin et al. 2023). Some studies consider other possibilities for m like m = 1 (Koshimoto et al. 2017;Ishitani Silva et al. 2022;Olmschenk et al. 2023 . Relative likelihood distribution of (m, r) calculated by Equation (6) for the S16 sample of 22 planetary events. ...

MOA-2020-BLG-208Lb: Cool Sub-Saturn-mass Planet within Predicted Desert

The Astronomical Journal