M. Pérez-Torres’s research while affiliated with University of Zaragoza and other places

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Publications (37)


Fig. 1. Stokes I radio maps centred on V1298 Tau (the location of the target is indicated by a cross) that we obtained with JVLA at each epoch of observation (upper image: L-band; lower image: C-band). The observing date is indicated in the upper left corner of each panel. The beam sizes are sketched in the bottom left corner. Contours are −3, −2, 3, 4 5, 7, 10, 15, 20, 25, 40 times the RMS of each map. The background colour scale ranges from −43 to 200 µJy/beam for L-band and from −14 to 200 µJy/beam for C-band.
Fig. 2. Upper panel: peak flux values (dots) and 3σ upper limits (triangles) of the JVLA observations in L-and C-bands (black and orange data points), and GMRT in band 4 (red data points), as a function of the observing epoch. Middle panel: ASAS-SN g-band magnitudes and JVLA radio fluxes phase-folded to the stellar rotation period P∼2.9 days. Phase zero corresponds to the first epoch of the JVLA C-band observations. Optical and radio observations were carried out within the same time span. Lower panel: GLS periodogram of the ASAS-SN optical light curve collected over the time span covered by JVLA observations (28 July-28 Sept. 2024). The stellar rotation period of ∼2.9 days is indicated by a red dashed line.
Fig. 3. Variation of Stokes I fluxes during the two JVLA C-Band epochs with the brightest emission, (blue) for 28 August 2024 and (orange) for 31 August 2024, where t = 0 marks the beginning of the first on-source scan for each epoch, and the data of the second epoch have been shifted by 0.5 min on the x-axis for better visualisation. The horizontal bars indicate the intervals of source scans. The horizontal lines correspond to the average and 1σ confidence level.
Fig. 4. SRT 6.6 GHz total intensity light curve for 27 June 2024. The flux density reported in the plot (<Flux> = 3.7±4.3 mJy) represents the mean of N = 20 measurements, and the error bar has been determined as σ/ √ N, from which a 3σ upper limit of <13 mJy is derived. We removed from the flux density light curve the contribution of the nearby confusion source NVSS J040522+200958, which is 0.15 mJy at 6.6 GHz based on our calculation.
First detection of variable radio emission originating from the infant planetary system V1298 Tau
  • Article
  • Full-text available

March 2025

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9 Reads

Astronomy and Astrophysics

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O. Morata

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[...]

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J.M. Girart

Context. V1298 Tau is a very young and magnetically active K1V star that hosts a benchmark multi-planetary system to study planet formation and evolutionary history at the earliest stages. Thanks to the high interest, it has been the target of a multi-wavelength follow-up. Aims. We selected V1298 Tau for a first targeted follow-up at radio frequencies with the Karl G. Jansky Very Large Telescope (JVLA), the upgraded Giant Metrewave Radio Telescope (uGMRT), and the Sardinia Radio Telescope (SRT) to search for emission in the overall frequency range 0.55–7.2 GHz. Detecting radio emission from such a very active star is key to characterising its magnetosphere, allowing us in principle to probe the strength of the coronal magnetic field and plasma density. Methods. Observations were carried out between October 2023 and September 2024: three epochs (total of ∼180 min on-source) with uGMRT band-4 (0.55–0.75 GHz), 12 epochs (total of ∼427 min on-source) with the JVLA using L (1–2 GHz) and C (4.5–6.5 GHz) bands, and three epochs (total of ∼56 min on-source) with SRT using C -high band (6–7.2 GHz). Results. We report the first detection of radio emission from V1298 Tau at different epochs using the JVLA. The emission has maximum peak flux densities of 91±10 and 177±6 µJy/beam in the L - and C -band, respectively. From a comparison with contemporary optical photometry, we found that the detected emission with the highest fluxes are located around a phase of minimum of the photospheric light curve. Although the uGMRT and SRT observations could not detect the source, we measured 3σ flux density upper limits in the range ∼41–56 µJy/beam using uGMRT, while with SRT we reached upper limits down to 13 mJy. The lack of a significant fraction of circular polarisation indicates that the observed flux is not due to electron cyclotron maser emission from star-planet interaction, and it is likely produced by gyrosynchroton and/or cyclotron emission from the corona triggered by stellar magnetic activity, although we cannot exclude thermal emission, due to a lack of constraints on the brightness temperature.

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Fig. 1. Stokes I radio maps centered on V1298 Tau (the location of the target is indicated by a cross) that we obtained with JVLA at each epoch of observation (upper image: L-band; lower image: C-band). The observing date is indicated in the upper left corner of each panel. The beam sizes are sketched at the bottom left corner. Contours are −3, −2, 3, 4 5, 7, 10, 15, 20, 25, 40 times the RMS of each map. The background color scale ranges from −43 to 200 µJy/beam for L-band and from −14 to 200 µJy/beam for C-band.
First detection of variable radio emission originating from the infant planetary system V1298 Tau

March 2025

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4 Reads

V1298 Tau is a very young and magnetically active star which hosts a benchmark multi-planetary system to study planet formation and evolutionary history at the earliest stages. We selected V1298 Tau for a first targeted follow-up at radio frequencies with the Karl G. Jansky Very Large Telescope (JVLA), the upgraded Giant Metrewave Radio Telescope (uGMRT), and the Sardinia Radio Telescope (SRT), to search for emission in the overall frequency range 0.55-7.2 GHz. Detecting radio emission from such a very active star is key to characterise its magnetosphere, allowing in principle to probe the strength of the coronal magnetic field and plasma density. Observations were carried out between Oct 2023 and Sept 2024: three epochs with uGMRT band-4 (0.55-0.75 GHz), 12 epochs with the JVLA using L (1-2 GHz) and C (4.5-6.5 GHz) bands, and three epochs with SRT using C-high band (6-7.2 GHz). We report the first detection of radio emission from V1298 Tau at different epochs using the JVLA. The emission has maximum peak flux densities of 91±\pm10 and 177±\pm6 μ\muJy/beam in the L- and C-band, respectively. From a comparison with contemporary optical photometry, we found that the detected emission with the highest fluxes are located around a phase of minimum of the photospheric light curve. Although the uGMRT and SRT observations could not detect the source, we measured 3σ\sigma flux density upper limits in the range ~41-56 μ\muJy/beam using uGMRT, while with SRT we reached upper limits down to 13 mJy. The lack of a significant fraction of circular polarisation indicates that the observed flux is not due to electron cyclotron maser emission from star-planet interaction, and it is likely produced by gyrosynchroton/cyclotron emission from the corona triggered by stellar magnetic activity, although we cannot exclude thermal emission due to a lack of constraints on the brightness temperature.


Jetted subgalactic-size radio sources in merging galaxies -- A jet redirection scenario

February 2025

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19 Reads

Context: The long-standing question concerning jetted subgalactic-size (JSS) radio sources is whether they will evolve into large radio galaxies, die before escaping the host galaxy, or remain indefinitely confined to their compact size. Aims: Our main goal is to propose a scenario that explains the relative number of JSS radio sources and their general properties. Methods: We studied the parsec-scale radio morphology of a complete sample of 21 objects using Very Long Baseline Array (VLBA) observations at various frequencies and analyzed the morphological characteristics of their optical hosts. Results: Many of these radio sources exhibit radio morphologies consistent with transverse motions of their bright edges and are found in dynamically disturbed galaxies. VLBA images suggest the possible presence of large-angle, short-period precessing jets, and an orbital motion of the radio-loud active galactic nucleus (AGN) in a dual or binary system. The majority of JSS radio sources appear to be in systems in different stages of their merging evolution. Conclusions: We propose a scenario where rapid jet redirection, through precession or orbital motion, prevents the jet from penetrating the interstellar medium (ISM) sufficiently to escape the host galaxy. Most JSS radio sources remain compact due to their occurrence in merging galaxies.


Fig. 1. Coverage of our uGMRT observations of the GJ 486 system folded to the orbital period of GJ 486b of 1.47 d. Each epoch is shown with a different color. Each point corresponds to the central time of each observing epoch, with the horizontal side of the surrounding rectangle being the time span of the epoch. The vertical axis has no real meaning, and the epochs are simply offset so they do not overlap.
Fig. 2. Stokes I wide-field image centered on GJ 486 from band 4 (central frequency of 648 MHz) uGMRT observations on 30 October 2021. The image covers a region of ∼8 ′ × 8 ′ , centered at the position of GJ 486 (green cross). The synthesized beam is shown as a green solid ellipse in the bottom left. The green square corresponds to a region of 60 × 60 arcsec squared, which we have used to estimate the local rms.
Fig. 3. Dynamic spectrum of the Stokes I and V (upper and lower panels, respectively) emission from the GJ 486-GJ 486b system for our 30 October 2021 uGMRT observations in band 4, averaged in frequency (∆ ν = 0.4 MHz). The time interval used is 10.7 s (which is the integration time). There is no apparent detection of radio emission above the noise. Blank regions correspond to times when we observed the phase calibrator. The spectra at the top and right of the dynamic spectrum result from collapsing all channels (top) and times (right). For a box located on a time range from 2:00 to 2:20 and a frequency range from 0.68 to 0.72 GHz. The rms values are 13.5 and 8.4 mJy for the Stokes I and V spectra, respectively.
Fig. 6. Predicted flux density arising at a nominal frequency of 670 MHz from SPI. The yellow (cross-hatched) areas correspond to the expected radio flux density, including (neglecting) free-free absorption from the thermal electrons in the stellar wind. The rows correspond to the expected emission for two different values of the coronal temperature, T c = 4.7 MK (the nominal value; top row) and T c = 2.5 MK (3σ lower limit; bottom row). The left and middle panels show the predicted flux density as a function of the stellar wind mass-loss rate for an unmagnetized planet (left) and a magnetized one with B pl = 0.85 G (middle), with a vertical dashed line showing the nominal value, ˙ M ⋆ = 1.4 ˙ M ⊙ (see text for details). The right panels show the predicted flux density as a function of the planetary magnetic field for the aforementioned nominal value of ˙ M ⋆ , and a vertical dashed line corresponds to the nominal value of the magnetic field, B pl = 0.85 G. Red areas correspond to values M A ≥ 1, that is, where the planet is in the super-Alfvénic regime; therefore model predictions are not valid. The horizontal dash-dotted lines correspond to the 3σ detection threshold of our observations (where σ = 30 µJy b −1 ).
Parameters of the GJ 486-GJ 486b system.
Searching for star-planet interactions in GJ 486 at radio wavelengths with the uGMRT

December 2024

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9 Reads

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1 Citation

Astronomy and Astrophysics

Aims. We search for radio emission from star–planet interactions in the M dwarf system GJ 486, which hosts an Earth-like planet. Methods. We observed the GJ 486 system with the upgraded Giant Metrewave Radio Telescope (uGMRT) from 550 to 750 MHz in nine different epochs between October 2021 and February 2022, covering almost all orbital phases of GJ 486b from different orbital cycles. We obtained radio images and dynamic spectra of the total and circularly polarized intensity for each individual epoch. Results. We did not detect any quiescent radio emission in any epoch above 3 σ . Similarly, we did not detect any bursty emission in our dynamic spectra. Conclusions. While we cannot completely rule out that the absence of a radio detection is due to time variability of the radio emission or to the maximum electron-cyclotron maser emission being below our observing range, these cases seem unlikely. We discuss two possible scenarios: an intrinsic dim radio signal and, alternatively, a situation where the anisotropic beamed emission is pointed away from the observer. If the non-detection of radio emission from the star-planet interaction in GJ 486 is due to an intrinsically dim signal, this implies that independent of whether the planet is magnetized or not, the mass-loss rate is small ( Ṁ ⋆ ≲ 0.3 Ṁ ⊙ ) and that, concomitantly, the efficiency of the conversion of the Poynting flux into radio emission must be low ( β ≲ 10 ⁻³ ). Free-free absorption effects are negligible, given the high value of the coronal temperature. Finally, if the anisotropic beaming pointed away from the observer, this would imply that GJ 486 has very low values of magnetic obliquity and inclination.


Fig. 1: Coverage of our uGMRT observations of the GJ 486 system, folded to the orbital period of GJ 486b of 1.47 d. Each epoch is shown with a different color. Each point corresponds to the central time of each observing epoch, with the horizontal side of the surrounding rectangle being the time span of the epoch. The vertical axis has no real meaning and the epochs are simply offset so they do not overlap.
Fig. 4: Fraction of transmitted SPI flux due to the effect of free-free absorption for T c values of 1 (dot-dashed black line), 1.5 (blue dashed line), 2.5 (orange dotted line) and 4.7 (green solid line) MK.
Fig. 6: Predicted flux density arising at a nominal frequency of 670 MHz from star planet interaction. The yellow (cross-hatched) areas correspond to the expected radio flux density, including (neglecting) free-free absorption from the thermal electrons in the stellar wind. The rows correspond to the expected emission for two different values of the coronal temperature, T c = 4.7 MK (the nominal value; top row) and T c = 2.5 MK (3-σ lower limit; bottom row). The left and middle panels show the predicted flux density as a function of the stellar wind mass-loss rate for an unmagnetized planet (left) and a magnetized one with B pl = 0.85 G (middle), with a vertical dashed line showing the nominal value, 9 M ‹ = 1.4 9 M d (see text for details). The right panels show the predicted flux density as a function of the planetary magnetic field, for the aforementioned nominal value of 9 M ‹ , and a vertical dashed line corresponding to the nominal value of the magnetic field, B pl = 0.85 G. Red areas correspond to values M A ě 1, i.e., where the planet is in the Super-Alfvénic regime, therefore model predictions are not valid. The horizontal dash-dotted lines correspond to the 3σ detection threshold of our observations (where σ " 30 µJy b ´1 ).
Fig. C.2: Same as in Fig. C.1, but for our system viewed pole-on and with a magnetic obliquity close to 90 0 (geometry # 3).
Searching for star-planet interactions in GJ 486 at radio wavelengths with the uGMRT

November 2024

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10 Reads

We search for radio emission from star-planet interactions in the M-dwarf system GJ~486, which hosts an Earth-like planet. We observed the GJ~486 system with the upgraded Giant Metrewave Radio Telescope (uGMRT) from 550 to 750 MHz in nine different epochs, between October 2021 and February 2022, covering almost all orbital phases of GJ~486 b from different orbital cycles. We obtained radio images and dynamic spectra of the total and circularly polarized intensity for each individual epoch We do not detect any quiescent radio emission in any epoch above 3σ\sigma. Similarly, we do not detect any bursty emission in our dynamic spectra. While we cannot completely rule out that the absence of a radio detection is due to time variability of the radio emission, or to the maximum electron-cyclotron maser emission being below our observing range, this seems unlikely. We discuss two possible scenarios: an intrinsic dim radio signal, or alternatively, that the anisotropic beamed emission pointed away from the observer. If the non-detection of radio emission from star-planet interaction in GJ~486 is due to an intrinsically dim signal, this implies that, independently of whether the planet is magnetized or not, the mass-loss rate is small (\dot{M}_\star \lesssim 0.3 \dot{M}_\sun) and that, concomitantly, the efficiency of the conversion of Poynting flux into radio emission must be low (β103\beta \lesssim 10^{-3}). Free-free absorption effects are negligible, given the high value of the coronal temperature. Finally, if the anisotropic beaming pointed away from us, this would imply that GJ~486 has very low values of its magnetic obliquity and inclination.



Fig. 1. Deep X-band image of the Arches cluster (see Table A.1 for details). Sources are labelled with the NIR stellar ID from Clark et al. (2018a) with the exception of the AR19 and AR20 sources (see Sect. 3.2).
Fig. 2. Flux versus frequency plot in logarithmic space in the case of the C-band observations from 10 June 2018.
Fig. A.1. All images of the Arches cluster.
Variability parameters.
Hardness ratios of the sources detected by Chandra.
A multi-frequency multi-epoch radio continuum study of the Arches cluster with the Very Large Array

November 2024

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3 Reads

Astronomy and Astrophysics

Context. The Arches cluster, one of the most massive clusters in the Milky Way, is located about 30 pc in projection from the central massive black hole Sagittarius A* at a distance of ≈8 kpc from Earth. With its high mass, young age, and location in the Galaxy’s most extreme star forming environment, the Arches is an extraordinary laboratory for studying massive stars and clusters. Aims. Our objective is to improve our knowledge of the properties of massive stars and the Arches cluster through high-angular-resolution radio continuum studies. Methods. We observed the Arches cluster with the Karl G. Jansky Very Large Array in the C - and X -bands (central frequencies of 6 and 10 GHz respectively) in two epochs at C -band and five epochs at X -band throughout 2016, 2018, and 2022, covering time spans ranging from 22 days to 6 years. We used the A-configuration to achieve the highest possible angular resolution and cross-matched the detected point-sources with stars detected in the infrared, using proper motion catalogues to ensure cluster membership. Results. We report the most extensive radio point-source catalogue of the cluster to date, with a total of 25 radio detections (7 more than the most recent study). We also created the deepest (2.5 μ Jy in X -band) images of the cluster so far in the 4 to 12 GHz frequency range. Most of our stellar radio sources (12 out of 18) show a positive spectral index, indicating that the dominant emission process is free-free thermal radiation, which probably originates from stellar winds. We find that radio variability is more frequent than what was inferred from previous observations, and affects up to 60% of the sources associated with bright stellar counterparts, with two of them, F18 and F26, showing extreme flux variability. We propose four of our detections (F6, F18, F19, and F26) as primary candidates for colliding-wind binaries (CWBs) based on their consistent flat-to-negative spectral index. We classify F7, F9, F12, F14, and F55 as CWB binary candidates based on their high flux and/or spectral index variability, and X-ray counterparts. Thus, we infer a 14/23 ≈ 61% multiplicity fraction for the radio stars of the Arches cluster when combining our findings with recent infrared radial velocity studies.


Prospects for a survey of the galactic plane with the Cherenkov Telescope Array

October 2024

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103 Reads

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8 Citations

Approximately one hundred sources of very-high-energy (VHE) gamma rays are known in the Milky Way, detected with a combination of targeted observations and surveys. A survey of the entire Galactic Plane in the energy range from a few tens of GeV to a few hundred TeV has been proposed as a Key Science Project for the upcoming Cherenkov Telescope Array Observatory (CTAO). This article presents the status of the studies towards the Galactic Plane Survey (GPS). We build and make publicly available a sky model that combines data from recent observations of known gamma-ray emitters with state-of-the-art physically-driven models of synthetic populations of the three main classes of established Galactic VHE sources (pulsar wind nebulae, young and interacting supernova remnants, and compact binary systems), as well as of interstellar emission from cosmic-ray interactions in the Milky Way. We also perform an optimisation of the observation strategy (pointing pattern and scheduling) based on recent estimations of the instrument performance. We use the improved sky model and observation strategy to simulate GPS data corresponding to a total observation time of 1620 hours spread over ten years. Data are then analysed using the methods and software tools under development for real data. Under our model assumptions and for the realisation considered, we show that the GPS has the potential to increase the number of known Galactic VHE emitters by almost a factor of five. This corresponds to the detection of more than two hundred pulsar wind nebulae and a few tens of supernova remnants at average integral fluxes one order of magnitude lower than in the existing sample above 1 TeV, therefore opening the possibility to perform unprecedented population studies. The GPS also has the potential to provide new VHE detections of binary systems and pulsars, to confirm the existence of a hypothetical population of gamma-ray pulsars with an additional TeV emission component, and to detect bright sources capable of accelerating particles to PeV energies (PeVatrons). Furthermore, the GPS will constitute a pathfinder for deeper follow-up observations of these source classes. Finally, we show that we can extract from GPS data an estimate of the contribution to diffuse emission from unresolved sources, and that there are good prospects of detecting interstellar emission and statistically distinguishing different scenarios. Thus, a survey of the entire Galactic plane carried out from both hemispheres with CTAO will ensure a transformational advance in our knowledge of Galactic VHE source populations and interstellar emission.


Fig. 3 Sketch illustrating the two putative sources of electron cyclotron maser (ECM) emission in exoplanetary systems. Left Panel: Emission induced on a star by a close-in planet. If the planet orbits inside the Alfvén surface of the star, it can perturb the star's magnetic field, producing Alfvén waves which propagate back towards the star. These waves interact with electrons, accelerating them towards the stellar surface. Electrons with sufficiently large pitch angles undergo a magnetic mirroring effect and are reflected, producing ECM emission which propagates in a hollow cone. Right Panel: Auroral emission induced on a planet by the interaction of its magnetosphere with the incident wind of its host star. The magnetic field carried by the stellar wind causes the planet's magnetosphere to open up on the dayside (left). These field lines are pushed towards the nightside (right), where they subsequently reconnect. The energy released in the magnetic reconnection accelerates electrons back towards the poles along the field line highlighted in red, where they reflect and power ECM emission in a similar manner to that described for the left panel. For clarity, the emission cone is only shown for the Northern hemisphere in both cases.
Radio Signatures of Star-Planet Interactions, Exoplanets, and Space Weather

September 2024

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93 Reads

Radio detections of stellar systems provide a window onto stellar magnetic activity and the space weather conditions of extrasolar planets, information that is difficult to attain at other wavelengths. There have been recent advances observing auroral emissions from radio-bright low-mass stars and exoplanets largely due to the maturation of low-frequency radio instruments and the plethora of wide-field radio surveys. To guide us in placing these recent results in context, we introduce the foremost local analogues for the field: Solar bursts and the aurorae found on Jupiter. We detail how radio bursts associated with stellar flares are foundational to the study of stellar coronae, and time-resolved radio dynamic spectra offers one of the best prospects of detecting and characterising coronal mass ejections from other stars. We highlight the prospects of directly detecting coherent radio emission from exoplanetary magnetospheres, and early tentative results. We bridge this discussion to the field of brown dwarf radio emission, in which their larger and stronger magnetospheres are amenable to detailed study with current instruments. Bright, coherent radio emission is also predicted from magnetic interactions between stars and close-in planets. We discuss the underlying physics of these interactions and implications of recent provisional detections for exoplanet characterisation. We conclude with an overview of outstanding questions in theory of stellar, star-planet interaction, and exoplanet radio emission, and the prospects of future facilities in answering them.


Fig. 2. Size evolution considering only observations from a single array (upper panel: EVN; lower panel: VLBA). Each panel is similar to Figure 1, except that the epochs not considered in the fit are shown with light grey shading for clarity.
Fig. C2. Flux density (left panel) and size (right panel) of GRB 221009A and J1905+1943 in the EVN observations. The average flux density of J1905+1943 (left panel) and the 1:1 correlation (right panel) are shown as grey dashed lines for the sake of comparison.
Fig. D1. Constraint on the viewing angle from the absence of an observed source apparent displacement in our VLBA observations. In each panel, filled contours show the displacement of the centre of the fitted Gaussian expected between 44 d and 262 d, color coded as shown in the colorbar on the right, as a function of the E/A ratio and of the off-edge viewing angle θ v − θ j . The red contour shows ∆(262 d) − ∆(44 d) = 0.6 mas, which represents the largest displacement compatible at 1 σ with our observations. The red contour hence contains the excluded parameter region. The upper panel row refers to a wind-like external medium, while the lower row refers to a homogeneous external medium. Each column assumes a different jet half-opening angle, given at the top of the column.
The expansion of the GRB 221009A afterglow

July 2024

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7 Reads

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3 Citations

Astronomy and Astrophysics

We observed upgamma -ray burst (GRB) 221009A using very long baseline interferomety (VLBI) with the European VLBI Network (EVN) and the Very Long Baseline Array (VLBA), over a period spanning from 40 to 262 days after the initial GRB. The high angular resolution (mas) of our observations allowed us, for the second time ever, after GRB\,030329, to measure the projected size, s, of the relativistic shock caused by the expansion of the GRB ejecta into the surrounding medium. Our observations support the expansion of the shock with a >4significance,andconfirmitsrelativisticnaturebyrevealinganapparentlysuperluminalexpansionrate.Fittingapowerlawexpansionmodel,>4 significance, and confirm its relativistic nature by revealing an apparently superluminal expansion rate. Fitting a power law expansion model, s t^a,totheobservedsizeevolution,wefindaslope, to the observed size evolution, we find a slope . Fitting the data at each frequency separately, we find different expansion rates, pointing to a frequency-dependent behaviour. We show that the observed size evolution can be reconciled with a reverse shock plus forward shock, provided that the two shocks dominate the emission at different frequencies and, possibly, at different times.


Citations (12)


... Two main methods for discovery are being explored: one through radio emission due to electron-cyclotron maser instability (ECMI) emission from the travel of the particle along the magnetic field of the planetary body, and the other through molecular emission due to the interaction between the electron and the planetary atmosphere (see review by Callingham et al. 2024). There have been a few suggestions of auroral interactions observed in the radio with LOFAR (Turner et al. 2021; try@lowell.edu ...

Reference:

Stringent Limits on H$_3^+$ Emission from the Hot Jupiters WASP-80b and WASP-69b
Radio signatures of star–planet interactions, exoplanets and space weather
  • Citing Article
  • November 2024

Nature Astronomy

... , as follows. The first method is to convert the 12 CO(J = 1-0) integrated intensity to N(H 2 ), assuming the X-factor of ( ) =´---X 2 10 cm K km s CO 20 2 1 1 . This factor has 10%-40% uncertainty at the Galactocentric radius of 8.5-12 kpc, which is derived for the position of the molecular clouds (N. Arimoto et al. 1996;A. D. Bolatto et al. 2013;S. Abe et al. 2024). The second one is to calculate the column density assuming local thermodynamic equilibrium (LTE). On the assumption that the 12 CO(J = 1-0) line is optically thick, the excitation temperature (T ex ) is derived from the 12 CO(J = 1-0) data. With T ex and the 12 CO(J = 1-0) intensity, the 13 CO optical depth and column density, N( 13 CO ...

Prospects for a survey of the galactic plane with the Cherenkov Telescope Array

... High-resolution Very Long Baseline Interferometry (VLBI) provides a plausible pathway to direct kinematic measurements of these objects. Two events have associated "expansion speed" measurements: GRB 030329A and 221009A, (Taylor et al. 2004;Giarratana et al. 2024), while two further studies obtain upper limits using similar techniques (GRB 201015A, Giarratana et al. 2022;GRB 190289A, Salafia et al. 2022). Moreover, the proximity of GRB170817a (Abbott et al. 2017b), associated with the seminal gravitational wave event GW170817 (Abbott et al. 2017a), enabled a measurement of jet proper motion at both radio (Mooley et al. 2018) and optical (Mooley et al. 2022) wavelengths. ...

The expansion of the GRB 221009A afterglow

Astronomy and Astrophysics

... This value places the range typically associated with mild stellar activity for M stars. This conclusion is based on the log 10 L X L bol distribution for M stars, derived from the data in Shan et al. (2024), as shown in the Figure 6. We separate the stars into two spectral type groups: M0 to M4 (in blue) and M4 to M8 (in red). ...

CARMENES input catalog of M dwarfs. VII. New rotation periods for the survey stars and their correlations with stellar activity

Astronomy and Astrophysics

... Usually, the theoretical power levels corresponding to well-defined false alarm probability values (e.g., 10 %, 5 %, 1 %, 0.1 %) are computed and are used to establish the significance of the highest peak only (e.g., [3,7,11,12]). However, sometimes such threshold values are used to evaluate the significance of two or more peaks (see e.g., [12][13][14][15][16][17]). In fact, this reflects the need to obtain information regarding the significance of peaks other than the highest one. ...

Wolf 327b: A new member of the pack of ultra-short-period super-Earths around M dwarfs

Astronomy and Astrophysics

... This approach justifies Jupiter non-Io DAM auroras and is thought to be at work in UCDs. Based on the physics described above, we followed the geometric model proposed in Bloot et al. (2024) to reproduce the total and polarized lightcurves of WISE J1122. According to the references above, the auroral emission originates in circumpolar rings (which may remind the main oval in Jupiter) around the magnetic poles, where the electrons supplied by the field-aligned currents bounce back to the equatorial plasma disk. ...

Phenomenology and periodicity of radio emission from the stellar system AU Microscopii

Astronomy and Astrophysics

... Recently, Moore et al. (2023)and Chen et al. (2024b) presented the first evidence of a modulation in the radioactive decay tail for SN 2022jli. In one of the proposed scenarios, the authors suggest that the modulation arises from mass transfer from a companion star onto the newly formed neutron star (NS). ...

SN 2022jli: A Type Ic Supernova with Periodic Modulation of Its Light Curve and an Unusually Long Rise

The Astrophysical Journal Letters

... In addition to the above-mentioned radio interferometers, the high brightness temperature of the radio emission measured in a number of UCDs (see references below) enables the use of the very-long-baseline interferometry (VLBI) technique. The high spatial resolution that VLBI provides is a suitable tool to constrain both the magnetic and kinematic properties of the UCDs; actually, VLBI observations have contributed to remarkable results, namely, the establishment of direct limits on the radio emission brightness temperature (TVLM 513−46546;Forbrich & Berger 2009), the measurement of precise dynamical mass in a binary system (2MASS J0746+2000AB; Zhang et al. 2020), the discovery of the first planetary companion from radio astrometry (TVLM 513−46546;Curiel et al. 2020), and the discovery of the first extrasolar radiation belts (LSR J1835+3259; Kao et al. 2023, Climent et al. 2023. ...

Evidence for a radiation belt around a brown dwarf
  • Citing Article
  • August 2023

Science

... Prominent features of intermediate-mass elements such as oxygen, magnesium, and calcium are seen both in Type Ib and Ic SN spectra (see Gal-Yam 2017, for a general introduction). Although SNe Ib/c lack obvious H features in their early-time spectra, few studies have focused on the existence of H in some of SNe Ib at later time (e.g." Branch et al. 2002;Elmhamdi et al. 2006;Kuncarayakti et al. 2023;Agudo et al. 2023). ...

Panning for gold, but finding helium: Discovery of the ultra-stripped supernova SN2019wxt from gravitational-wave follow-up observations

Astronomy and Astrophysics

... Table 4 does not show Barnard's Star "b", the planet candidate proposed by Ribas et al. (2018) that was afterwards challenged by Lubin et al. (2021) and Artigau et al. (2022). However, the list of others' exoplanets challenged by CARMENES is much longer, such as GJ 1151 "b" (proposed by Mahadevan et al. 2021 and ruled out by Perger et al. 2021 andBlanco-Pozo et al. 2023), TZ Ari "b" (proposed by Feng et al. 2020 and ruled out by Quirrenbach et al. 2022), or CN Leo "b" (proposed by Tuomi et al. 2019 and ruled out by Lafarga et al. 2021). See a full list of exoplanet candidates that turned to be a spurious signal, stellar rotation or alias, and their references, in Table 4 of Ribas et al. (2023). ...

The CARMENES search for exoplanets around M dwarfs. A long-period planet around GJ 1151 measured with CARMENES and HARPS-N data

Astronomy and Astrophysics