I. Pérez-Fournon’s research while affiliated with University of La Laguna and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (141)


LensWatch. II. Improved Photometry and Time-delay Constraints on the Strongly Lensed Type Ia Supernova 2022qmx (“SN Zwicky”) with Hubble Space Telescope Template Observations
  • Article

February 2025

·

1 Citation

The Astrophysical Journal

C. Larison

·

J. D. R. Pierel

·

M. J. B. Newman

·

[...]

·

Y. Zenati

Strongly lensed supernovae (SNe) are a rare class of transient that can offer tight cosmological constraints that are complementary to methods from other astronomical events. We present a follow-up study of one recently discovered strongly lensed SN, the quadruply imaged type Ia SN 2022qmx (aka “SN Zwicky”), at z = 0.3544. We measure updated, template-subtracted photometry for SN Zwicky and derive improved time delays and magnifications. This is possible because SNe are transient, fading away after reaching their peak brightness. Specifically, we measure point-spread-function photometry for all four images of SN Zwicky in three Hubble Space Telescope WFC3/UVIS passbands (F475W, F625W, and F814W) and one WFC3/IR passband (F160W), with template images taken ∼11 months after the epoch in which the SN images appear. We find consistency to within 2 σ between lens-model-predicted time delays (≲1 day) and measured time delays with HST colors (≲2 days), including the uncertainty from chromatic microlensing that may arise from stars in the lensing galaxy. The standardizable nature of SNe Ia allows us to estimate absolute magnifications for the four images, with images A and C being elevated in magnification compared to lens model predictions by about 6 σ and 3 σ , respectively, confirming previous work. We show that millilensing or differential dust extinction is unable to explain these discrepancies, and we find evidence for the existence of microlensing in images A, C, and potentially D that may contribute to the anomalous magnification.


Fig. 1. Images showing the FIR dust continuum emission, the H-or K s -band continuum emission, the CO(3-2) or CO(4-3) emission, and the related spectra (if CO is detected) of our 12 extreme starburst galaxies ordered by increasing redshift from top to bottom. Left panels: 23 × 23 ALMA band 6 1.3 mm (240 GHz) FIR dust continuum images of our targeted galaxies. Contour levels start at ±4σ and are in steps of 1σ up to 10σ and in larger steps above. The respective synthesised beam size and orientation are indicated by the red filled ellipse in the bottom-left corner. The cross in each panel corresponds to the coordinates of the HAWK-I continuum emission peak (except for J0850+1549 and J0121+0025 for which we consider, respectively, the CFHT MegaCam and Subaru continuum emission peak) and is ±3 in size. Middle-left panels: 10 × 10 VLT HAWK-I seeing-limited H-band or AO K s -band images of our starburst galaxies in greyscale with the ALMA band 6 FIR dust continuum contours overlaid in red. For J0850+1549 and J0121+0025, we show, respectively, the CFHT MegaCam and Subaru seeing-limited R-band images. Contour levels start at ±4σ and are in steps of 2σ, except for J0146-0220, J1249+1550, and J0850+1549 where contour levels are the same as in the left panels. The PSF is shown by the black filled circle in bottom-left corner, and the ALMA synthesised beam by the red filled ellipse in the bottom-right corner. The cross is the same as in the left panels. Middle-right panels: 10 × 10 ALMA CO(3-2) or CO(4-3) velocity-integrated intensity moment-0 maps of our galaxies. The maps were integrated over the cyan-shaded spectral channels shown in the right panels. Contour levels start at ±4σ and are in steps of 1σ. The respective synthesised beam size and orientation are indicated by the red filled ellipse in the bottomright corner. The cross is the same as in the other panels. Right panels: ALMA CO(3-2) or CO(4-3) emission line spectra of our galaxies, plotted when detected, in steps of ∼45 km s −1 and with the zero velocity centred on the redshifts derived from optical nebular emission lines (Table 1). The cyan-shaded regions correspond to the velocity channels optimising the CO detections, as described in Sect. 3.1. The dashed orange lines correspond to the RMS noise level of spectra. The solid red lines are the multi-component Gaussian best-fits to the observed CO line profiles. The vertical bars mark the positions of the fitted Gaussian components. The rest of the figure is available in Appendix A.
Fig. 3. Infrared excess as a function of the UV spectral slope of our galaxies, colour-coded by redshift. Our galaxies are all characterised by very blue β UV < −1.8 and low IRX < +0.5. Most of them deviate from the canonical IRX-β UV relation (solid line; Meurer et al. 1999), and are better reproduced with the bluer intrinsic UV continuum slope β 0 = −2.62 as computed by Reddy et al. (2018) for the SMC (dashed line) and Calzetti et al. (2000) (dotted line) extinction curves.
Fig. 6. Dust mass as a function of the stellar mass of our extreme starburst galaxies, colour-coded by redshift. Our galaxies agree with the M dust -M stars relation derived by Magnelli et al. (2020) as shown by the solid black line, but are well below the relations of Liu et al. (2019) and Kokorev et al. (2021) shown by the dotted and dashed black lines, respectively. The grey shaded zone defines the SN dust production as predicted by Gall & Hjorth (2019), which is barely sufficient to reproduce M dust of most of our galaxies. The thick dashed-dotted green line defines the start of the AGB star contribution to the dust production (Witstok et al. 2023).
CO emission line observations (ALMA band 3).
Unveiling dust, molecular gas, and high star-formation efficiency in extremely UV bright star-forming galaxies at z ~ 2.1-3.6
  • Article
  • Full-text available

November 2024

·

10 Reads

Astronomy and Astrophysics

We analysed the Atacama Large Millimetre/submillimetre Array (ALMA) far-infrared (FIR), 1.3 mm, dust continuum and CO emission of 12 starburst galaxies at z2.13.6z 2.1-3.6 selected for their extreme brightness in the rest-frame UV, with absolute magnitudes of 23.4-23.4 to 24.7-24.7. We also analysed their Very Large Telescope (VLT) High Acuity Wide field K-band Imager (HAWK-I) H- and s bandimages.ThetargetedgalaxiesarecharacterisedbynegligibledustattenuationswithblueUVspectralslopes(-band images. The targeted galaxies are characterised by negligible dust attenuations with blue UV spectral slopes (-2.62 to -1.84),veryyoungstellarpopulationsof), very young stellar populations of 10Myr,andpowerfulstarburstswithahighmeanspecificstarformationrateof Myr, and powerful starbursts with a high mean specific star-formation rate of ,placingthem, placing them 1.5dexabovethemainsequenceatsimilarredshiftsandstellarmassesstarsodot dex above the main sequence at similar redshifts and stellar masses stars odot ). The FIR dust continuum emission revealed in nine galaxies gives IR luminosities of (5.928.3)Lodot(5.9-28.3) L_ odot , with six galaxies remaining dominated by unobscured UV star-formation rates, and high dust masses barely produced by supernovae within the 10 Myr timescale. The CO emission detected in eight galaxies leads to molecular gas masses higher than stellar masses, with the mean molecular gas mass fraction as high as 82 . The corresponding star-formation efficiencies reach 40 , with amazingly short molecular gas depletion timescales between less than 13 Myr and 71 Myr. These unique properties never reported in previously studied galaxies highlight that these galaxies are likely caught at the very beginning of their stellar mass build-up and undergo a very efficient and fast conversion of gas into stars that can only result from the gas collapse within a very short free-fall time. We find that the feedback-free starburst model seems to be able to explain the formation of these galaxies. To reconcile the co-spatial FIR dust emission with the UV-bright unattenuated emission, we speculate about the presence of radiation-driven outflows that can temporarily remove dust at the location of the starburst and expel it at large distances in line with the measured high FIR effective radii (1.7 kpc to 5 kpc) in comparison to the very compact stellar radii that are a few hundreds of parsecs).

Download

Spectroscopic analysis of the strongly lensed SN Encore: constraints on cosmic evolution of Type Ia supernovae

October 2024

·

3 Reads

·

2 Citations

Monthly Notices of the Royal Astronomical Society

Strong gravitational lensing magnifies the light from a background source, allowing us to study these sources in detail. Here, we study the spectra of a z=1.95z = 1.95 lensed Type Ia supernova (SN Ia) SN Encore for its brightest image A, taken 39 d apart. We infer the spectral age with template matching using the supernova identification (snid ) software and find the spectra to be at 29.0±5.029.0 \pm 5.0 and 37.4±2.837.4 \pm 2.8 rest-frame days post-maximum, respectively, consistent with separation in the observer frame after accounting for time dilation. Since SNe Ia measure dark energy properties by providing relative distances between low- and high-z SNe, it is important to test for the evolution of spectroscopic properties. Comparing the spectra to composite low-z SN Ia spectra, we find strong evidence of the similarity between the local sample and SN Encore. The line velocities of common SN Ia spectral lines, Si ii 6355 A˚\mathring{\rm A} and Ca ii near-infrared triplet, are consistent with the distribution for the low-z sample as well as other lensed SNe Ia, e.g. iPTF16geu (z=0.409z = 0.409) and SN H0pe (z=1.78z = 1.78). The consistency between the low-z sample and lensed SNe at high-z suggests no obvious cosmic evolution demonstrating their use as high-z distance indicators, though this needs to be confirmed/refuted via a larger sample. We also find that the spectra of SN Encore match the predictions for explosion models very well. With future large samples of lensed SNe Ia, e.g. with the Vera C. Rubin Observatory, spectra at such late phases will be important to distinguish between different explosion scenarios.


Unveiling dust, molecular gas, and high star formation efficiency in extremely UV-bright star-forming galaxies at $z\sim 2.1-3.6

October 2024

·

2 Reads

We analysed ALMA FIR (1.3 mm) dust continuum and CO emission of 12 starburst galaxies at z2.13.6z\sim 2.1-3.6, selected for their extreme brightness in the rest-UV with MUV=23.4M_{\rm UV} = -23.4 to 24.7-24.7. We also analysed VLT HAWK-I H- and KsK_{\rm s}-band images. The galaxies are characterised by negligible dust attenuations with blue UV spectral slopes (2.62-2.62 to 1.84-1.84), very young stellar populations of 10\sim 10 Myr, and powerful starbursts with a high mean specific star formation rate of 112 Gyr1\rm 112~Gyr^{-1}, placing them 1.5\sim 1.5~dex above the main sequence at similar redshifts and stellar masses (Mstars(1.54.6)×109 MM_{\rm stars} \sim (1.5-4.6)\times 10^9~M_{\odot}). The FIR dust continuum emission revealed in 9 galaxies yields IR luminosities of (5.928.3)×1011 L(5.9-28.3)\times 10^{11}~L_{\odot} and large dust masses barely produced by SNe within the 10~Myr timescale. The CO emission detected in 8 galaxies evidence large molecular gas masses with a mean molecular gas fraction of 82%. The corresponding star formation efficiencies reach 40\gtrsim 40\%, with amazingly short molecular gas depletion timescales between <13 Myr and 71 Myr. These unique properties, never reported in previously studied galaxies, highlight that these galaxies are likely caught at the very beginning of their stellar mass build-up and undergo a very efficient and fast conversion of gas into stars that can only result from the gas collapse within very short free-fall times. We find that the feedback-free starburst model seems to be able to explain the formation of these galaxies. To reconcile the co-spatial FIR dust emission with the UV-bright unattenuated emission, we speculate about radiation-driven outflows which can temporarily remove dust at the location of the starburst and expel dust at large distances in line with the measured large FIR effective radii (1.7 kpc5 kpc\rm 1.7~kpc - 5~kpc) in comparison to very compact stellar radii.


Eruptive mass-loss less than a year before the explosion of superluminous supernovae: I. The cases of SN 2020xga and SN 2022xgc

September 2024

·

12 Reads

We present photometric and spectroscopic observations of SN2020xga and SN2022xgc, two hydrogen-poor superluminous supernovae (SLSNe-I) at z=0.4296z = 0.4296 and z=0.3103z = 0.3103 respectively, that show an additional set of broad Mg II absorption lines, blueshifted by a few thousand km s1^{-1} with respect to the host galaxy absorption system. Previous work interpreted this as due to resonance line scattering of the SLSN continuum by rapidly expanding CSM expelled shortly before the explosion. The peak rest-frame g-band magnitude of SN2020xga is 22.30±0.04-22.30 \pm 0.04 mag and of SN2022xgc is 21.97±0.05-21.97 \pm 0.05 mag, placing them among the brightest SLSNe-I. We use high-quality spectra from ultraviolet to near-infrared wavelengths to model the Mg II line profiles and infer the properties of the CSM shells. We find that the CSM shell of SN2020xga resides at 1.3×1016cm\sim 1.3 \times 10^{16} \rm cm moving with a maximum velocity of 4275 km s14275~\rm km~s^{-1}, and the shell of SN2022xgc is located at 0.8×1016cm\sim 0.8 \times 10^{16} \rm cm reaching up to 4400 km s14400~\rm km~s^{-1}. These shells were expelled 11\sim 11 and 5\sim 5 months before explosion for SN2020xga and SN2022xgc respectively, possibly as a result of Luminous Blue Variable-like eruptions or pulsational pair instability (PPI) mass loss. We also analyze optical photometric data and model the light curves considering powering from the magnetar spin-down mechanism. The results support very energetic magnetars, approaching the mass-shedding limit, powering these SNe with ejecta masses of 79 M\sim 7-9 \rm~M_\odot. The ejecta masses inferred from the magnetar modeling are not consistent with the PPI scenario pointing towards stars >50 M> 50~\rm M_\odot He-core, hence alternative scenarios such as fallback accretion are discussed.


The Nature of 500 micron Risers III: a small complete sample

August 2024

Monthly Notices of the Royal Astronomical Society

Herschel surveys have found large numbers of sources with red far-IR colours, and spectral energy distributions (SEDs) rising from 250 to 500 µm: 500 risers. The nature and role of these sources is not fully understood. We here present Submillimeter Array (SMA) interferometric imaging at 200 GHz of a complete sample of five 500 risers with F500 >44 mJy selected within a 4.5 deg2 region of the XMMLSS field. These observations can resolve the separate components of multiple sources and allow cross identification at other wavelengths using the extensive optical-to-IR data in this field. Of our five targets, we find that two are likely gravitationally lensed, two are multiple sources, and one an isolated single source. Photometric redshifts, using optical-to-IR data and far-IR/submm data, suggest they lie at redshifts z2.5 ⁣ ⁣3.5z \sim 2.5\!-\!3.5. Star formation rates and stellar masses estimated from the SEDs show that the majority of our sources lie on the star-formation rate-stellar mass ‘main sequence’, though with outliers both above and below this relation. Of particular interest is our most multiple source, which consists of three submm emitters and one submm-undetected optical companion within a 7 arcsec region, all with photometric redshifts ∼3. One of the submm emitters in this group lies above the ‘main sequence’, while the optical companion lies well below the relation, and has an estimated stellar mass of 3.3±1.3×10113.3 \pm 1.3 \times 10^{11} M_{\odot }. We suggest this object is a forming brightest cluster galaxy (BCG) in the process of accreting actively star forming companions.


Figure 1. SMA Images of SERVS-XMM 500 Risers. Images are 1 arcminiute on a side. Contours are shown in red and are in increments of 1í µí¼Ž starting at 3í µí¼Ž and rising from there. The synthesised beam size is just over 3 arcseconds. The beam is shown as a white ellipse in the bottom left of each image.
Figure 6. Location of our sources on the star-formation rate -stellar mass correlation. The red line indicates the position of this correlation for a redshift of 3 (Speagle et al. 2014), while the data points show the position of our sources on this diagram. Different coloured points represent different subsamples. Green points represent the sources identified as lens candidates. Orange points indicate the sources associated with the putative galaxy cluster core associated with source J022448. The rest of the sources are shown as blue points. Stellar masses and star formation rates come from the SED fits in Zou et al. (2022) or from our own fits for J021856_2 and J022610.
The Nature of 500 micron Risers III: A Small Complete Sample

July 2024

·

4 Reads

Herschel surveys have found large numbers of sources with red far-IR colours, and spectral energy distributions (SEDs) rising from 250 to 500μ\mum: 500 risers. The nature and role of these sources is not fully understood. We here present Submillimeter Array (SMA) interferometric imaging at 200 GHz of a complete sample of five 500 risers with F500 >> 44 mJy selected within a 4.5 square degree region of the XMMLSS field. These observations can resolve the separate components of multiple sources and allow cross identification at other wavelengths using the extensive optical-to-IR data in this field. Of our five targets we find that two are likely gravitationally lensed, two are multiple sources, and one an isolated single source. Photometric redshifts, using optical-to-IR data and far-IR/submm data, suggest they lie at redshifts z2.53.5z \sim 2.5 - 3.5. Star formation rates and stellar masses estimated from the SEDs show that the majority of our sources lie on the star-formation rate-stellar mass `main sequence', though with outliers both above and below this relation. Of particular interest is our most multiple source which consists of three submm emitters and one submm-undetected optical companion within a 7 arcsecond region, all with photometric redshifts \sim 3. One of the submm emitters in this group lies above the `main sequence', while the optical companion lies well below the relation, and has an estimated stellar mass of 3.3±1.3×\pm 1.3 \times1011^{11} M_{\odot}. We suggest this object is a forming brightest cluster galaxy (BCG) in the process of accreting actively star forming companions.


Spectroscopic analysis of the strongly lensed SN~Encore: Constraints on cosmic evolution of Type Ia supernovae

July 2024

·

6 Reads

Strong gravitational lensing magnifies the light from a background source, allowing us to study these sources in detail. Here, we study the spectra of a z=1.95z = 1.95 lensed Type Ia supernova SN~Encore for its brightest Image A, taken 39 days apart. We infer the spectral age with template matching using the supernova identification (SNID) software and find the spectra to be at 29.0 ±5.0\pm 5.0 and 37.4 ±2.8\pm 2.8 rest-frame days post maximum respectively, consistent with separation in the observer frame after accounting for time-dilation. Since SNe~Ia measure dark energy properties by providing relative distances between low- and high-z SNe, it is important to test for evolution of spectroscopic properties. Comparing the spectra to composite low-z SN~Ia spectra, we find strong evidence for similarity between the local sample of SN~Encore. The line velocities of common SN~Ia spectral lines, Si II 6355 and Ca II NIR triplet are consistent with the distribution for the low-z sample as well as other lensed SNe~Ia, e.g. iPTF16geu (z=0.409z = 0.409) and SN~H0pe (z=1.78z = 1.78). The consistency in SN~Ia spectra across cosmic time demonstrates the utility of using SNe~Ia in the very high-z universe for dark energy inference. We also find that the spectra of SN~Encore match the predictions for explosion models very well. With future large samples of lensed SNe~Ia, spectra at such late phases will be important to distinguish between different explosion scenarios.


Figure 1. Left: HST WFC3/IR two-color image in the region of MACS J0138.0−2155 from 2016, using F105W (blue) and F160W (orange). SN Requiem is marked in its three visible image positions by white circles, notably absent in 2023. Right: combined JWST/NIRCam and HST/WFC3 color image from programs 6549 and 16264 (Table 1). The filters used are F105W+F115W+F125W (blue), F150W+F160W+F200W (green), and F277W+F356W+F444W (red). The images were drizzled to 0 02 pix −1 , and the image scale and orientation are as shown. The three detected image positions of SN Encore are circled, but it is not visible at this scale, and all five images of the host galaxy are labeled (A-E). For a zoom-in of each of the detected image positions, see Section 2 (Image Credit: STScI, A. Koekemoer, T. Li).
Figure 2. The observed light curve in the JWST/NIRCam short-wavelength filters for image A, the brightest and last to arrive (see Figure 3). The longwavelength filters (F277W, F356W, and F444W) were observed, but a more in-depth host-galaxy modeling effort (or a template image) will be required to measure accurate photometry.
Figure 3. JWST/NIRCam color cutouts with F115W (blue), F150W (green) and F200W (red) centered on image A (top), B (middle), and C (bottom) of SN Encore. Note the discovery program only detected SN Encore in F150W, so the first column is a grayscale image in F150W, while the remainder are three-color images. The images were drizzled to 0 02 pix −1 , with the image scale, orientation, and MJD (relative to discovery) shown. SN Encore is brightest in the discovery epoch and is on the decline in the subsequent epochs, but the evolution is relatively small at this redshift and is therefore difficult to see by eye (see Figure 2). Image C was first to arrive followed by image B, and although image C is not clearly visible by eye, it was detected at ∼5σ (see Section 2.1.1).
Figure 4. The (normalized) extracted G235M spectrum of SN Encore with 1σ uncertainty (faint red), with the binned spectrum superimposed (thick red line). The best-match spectrum from SNID (SN 2004eo; black line) is shown for comparison, with characteristic SN Ia features labeled in green text, confirming that SN Encore is of Type Ia.
Lensed Type Ia Supernova “Encore” at z = 2: The First Instance of Two Multiply Imaged Supernovae in the Same Host Galaxy

May 2024

·

51 Reads

·

24 Citations

The Astrophysical Journal Letters

A bright ( m F150W,AB = 24 mag), z = 1.95 supernova (SN) candidate was discovered in JWST/NIRCam imaging acquired on 2023 November 17. The SN is quintuply imaged as a result of strong gravitational lensing by a foreground galaxy cluster, detected in three locations, and remarkably is the second lensed SN found in the same host galaxy. The previous lensed SN was called “Requiem,” and therefore the new SN is named “Encore.” This makes the MACS J0138.0−2155 cluster the first known system to produce more than one multiply imaged SN. Moreover, both SN Requiem and SN Encore are Type Ia SNe (SNe Ia), making this the most distant case of a galaxy hosting two SNe Ia. Using parametric host fitting, we determine the probability of detecting two SNe Ia in this host galaxy over a ∼10 yr window to be ≈3%. These observations have the potential to yield a Hubble constant ( H 0 ) measurement with ∼10% precision, only the third lensed SN capable of such a result, using the three visible images of the SN. Both SN Requiem and SN Encore have a fourth image that is expected to appear within a few years of ∼2030, providing an unprecedented baseline for time-delay cosmography.


JWST Photometric Time-delay and Magnification Measurements for the Triply Imaged Type Ia “SN H0pe” at z = 1.78

May 2024

·

25 Reads

·

21 Citations

The Astrophysical Journal

Supernova (SN) SN H0pe is a gravitationally lensed, triply imaged, Type Ia SN (SN Ia) discovered in James Webb Space Telescope imaging of the PLCK G165.7+67.0 cluster of galaxies. Well-observed multiply imaged SNe provide a rare opportunity to constrain the Hubble constant ( H 0 ), by measuring the relative time delay between the images and modeling the foreground mass distribution. SN H0pe is located at z = 1.783 and is the first SN Ia with sufficient light-curve sampling and long enough time delays for an H 0 inference. Here we present photometric time-delay measurements and SN properties of SN H0pe. Using JWST/NIRCam photometry, we measure time delays of Δ t ab = − 116.6 − 9.3 + 10.8 observer-frame days and Δ t cb = − 48.6 − 4.0 + 3.6 observer-frame days relative to the last image to arrive (image 2b; all uncertainties are 1 σ ), which corresponds to a ∼5.6% uncertainty contribution for H 0 assuming 70 km s ⁻¹ Mpc ⁻¹ . We also constrain the absolute magnification of each image to μ a = 4.3 − 1.8 + 1.6 , μ b = 7.6 − 2.6 + 3.6 , μ c = 6.4 − 1.5 + 1.6 by comparing the observed peak near-IR magnitude of SN H0pe to the nonlensed population of SNe Ia.


Citations (49)


... 23,24]. To remedy this issue, we develop a new tidal stripping model based on galacticus, and implement it in the open-source software pyHalo 2 , a code which has already been used extensively for substructure lensing analyses in a variety of dark matter models [25][26][27], as well as milli-lensing of multiply-imaged supernova [28,29]. In a similar way to how a SAM, such as galacticus, incorporates a layer of abstraction to speed up calculations relative to N-body simulations, codes like pyHalo circumvent some of the more expensive calculations performed with SAMs by generating substructure populations"in place", meaning they do not explicitly model subhalo orbits and other processes occurring over time. ...

Reference:

Faster than SAM: An empirical model for the tidal evolution of dark matter substructure around strong gravitational lenses
LensWatch. II. Improved Photometry and Time-delay Constraints on the Strongly Lensed Type Ia Supernova 2022qmx (“SN Zwicky”) with Hubble Space Telescope Template Observations
  • Citing Article
  • February 2025

The Astrophysical Journal

... Combined with a model for the gravitational potential of the lens galaxy and line-of-sight structures, this constrains the presentday expansion rate of the Universe, the Hubble constant (Refsdal 1964;Treu & Marshall 2016;Suyu et al. 2024;Birrer et al. 2024). Additionally, lensed SNe enable detailed studies of lensing galaxies and high-redshift SNe (Cano et al. 2018;Johansson et al. 2021;Dhawan et al. 2024). ...

Spectroscopic analysis of the strongly lensed SN Encore: constraints on cosmic evolution of Type Ia supernovae
  • Citing Article
  • October 2024

Monthly Notices of the Royal Astronomical Society

... At the center of 30 Dor is a large open cluster, NGC 2070, with a central condensation that is the star cluster R 136. R 136 has an estimated stellar mass of 2 × 10 4 M ⊙ (contained within the innermost 5 pc; Hunter et al. 1995;Domínguez et al. 2023) and hosts very massive stars with masses over 100 M ⊙ (Crowther et al. 2010;Bestenlehner et al. 2011;Hainich et al. 2014;Crowther et al. 2016;Bestenlehner et al. 2020;Upadhyaya et al. 2024). Its most massive star was recently reported to have a mass of at least 200 M ⊙ (Kalari et al. 2022;Shenar et al. 2023). ...

Evidence for very massive stars in extremely UV-bright star-forming galaxies at z ∼ 2.2 − 3.6

... In the same host galaxy as SN Requiem, a second SN, "SN Encore," was discovered, marking the first occurrence of a lensed galaxy producing multiple observed SNe (J. D. R. Pierel et al. 2024). Across all of these SNe, SN Refsdal is the only one to provide precision H 0 constraints to date. ...

Lensed Type Ia Supernova “Encore” at z = 2: The First Instance of Two Multiply Imaged Supernovae in the Same Host Galaxy

The Astrophysical Journal Letters

... For lensed supernovae, immediate follow-up is required, with space telescopes. Time delays can be estimated with time series of photometric filters [26,27], as well as with spectroscopy in the case of a type Ia SN [28]. The transient nature and regularity of the SNe allow a measurement of the time delay with fewer, but well-timed observations. ...

JWST Photometric Time-delay and Magnification Measurements for the Triply Imaged Type Ia “SN H0pe” at z = 1.78

The Astrophysical Journal

... This alternative approach to the "AGN signpost" has already had a number of successes (e.g. Arribas et al., 2023, Bakx et al., 2024b, Calvi et al., 2023, Cheng et al., 2019, Lammers et al., 2022, Lewis et al., 2018, Polletta et al., 2021, Wang et al., 2021a, Zhou et al., 2024a. ...

A dusty protocluster surrounding the binary galaxy HerBS-70 at z = 2.3
  • Citing Article
  • April 2024

Monthly Notices of the Royal Astronomical Society

... The high ionization conditions in this galaxy are also confirmed by the detection of N iv] 1,488 Å and He ii 1,640 Å in the NIRSpec spectrum 11 , which require ionizing photons with energies above around 54 eV. This might point towards the presence of X-ray binaries or very massive stars [41][42][43] , which contribute to the hard ionizing radiation. [71][72][73][74][75][76][77][78], along with the ξ ion redshift evolution from ref. 57 for two different stellar masses (solid and dashed lines). ...

Evidence for very massive stars in extremely UV-bright star-forming galaxies at z ~ 2.2 - 3.6

Astronomy and Astrophysics

... Thus, our model calculates the UV luminosity and the FIR flux self-consistently. It is worth noting here that the FIR dust continuum radiation from > 10 UV-bright galaxies has not been detected yet (e.g., Fudamoto et al. 2024;Carniani et al. 2024a;Zavala et al. 2024;Schouws et al. 2024), even though their observed half-light radii are so small that the optical depth can be extremely high, ≳ 10 (e.g., Ziparo et al. 2023;Ferrara et al. 2024). This observational fact provides an important indication of the dust content and its spatial distribution in such super-early galaxies. ...

The NOEMA observations of GN-z11: Constraining the neutral interstellar medium and dust formation in the heart of cosmic reionization at z = 10.6
  • Citing Article
  • February 2024

Monthly Notices of the Royal Astronomical Society

... To date, the most distant spectroscopically confirmed lenses are at z ∼ 1.6 (Wong et al. 2014;Cañameras et al. 2017;Ciesla et al. 2020). Among these spectacular systems, strongly magnified dusty starforming galaxies (DSFGs) have opened a window into dustobscured and moderate star-formation activities at high redshifts (Vieira et al. 2013;Rizzo et al. 2020Rizzo et al. , 2021Berta et al. 2021;Hamed et al. 2021;Cox et al. 2023) and provided us with unprecedented deep insights into their ISM, kinematics, and dark matter properties (e.g. Cañameras et al. 2017;Yang et al. 2017;Cava et al. 2018;Ciesla et al. 2020;Rizzo et al. 2020Rizzo et al. , 2021Smail et al. 2023;Liu et al. 2024). ...

z-GAL: A NOEMA spectroscopic redshift survey of bright Herschel galaxies. I. Overview

Astronomy and Astrophysics

... SPICA's powerful detectors provide two orders of magnitude greater sensitivity compared to the previousgeneration Herschel and SOFIA instruments, in part because the SPICA instruments are not limited by radiation coming from the telescope itself. This increased sensitivity would have enabled the SAFARI, POL, and SMI instruments to investigate the spectroscopic details of both close-by and far away galaxies in unprecedented detail [2][3][4][5][6]. ...

Probing the high-redshift universe with SPICA: Toward the epoch of reionisation and beyond
  • Citing Article
  • December 2018

Publications of the Astronomical Society of Australia