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B. Rodríguez del Pino

Publications and source records attributed to B. Rodríguez del Pino.

3 recordsLinked to original sources

Unveiling the correlation between the UV 2175 Å dust attenuation bump, PAH emission, and gas-phase metallicity at cosmic noon

The UV 2175 Å attenuation bump is one of the most prominent yet poorly understood features of galaxy attenuation curves. Its main candidate carrier is polycyclic aromatic hydrocarbon (PAH) molecules, which are more prevalent in high-metallicity environments. We present the first systematic study of the relationship between PAH abundance and the UV bump in 49 galaxies at cosmic noon (1.5 < z < 2.7), examining its dependence on stellar mass, star formation rate (SFR), and V-band optical depth. For 19 galaxies, we also investigate gas-phase metallicity using oxygen abundances. We measure the bump amplitude from VLT/MUSE spectroscopy and derive galaxy properties, including the PAH-to-dust mass fraction $q_{\rm PAH}$, through spectral energy distribution fitting with Prospector, combining JWST/NIRCam and JWST/MIRI photometry. Oxygen abundances are derived from strong-line diagnostics using Keck/MOSFIRE and JWST/NIRSpec data. We find a positive correlation between bump amplitude $E_{\rm bump}$ and $q_{\rm PAH}$ (Spearman $ρ= 0.60$). UV bumps are rarely detected at low $q_{\rm PAH}$, supporting PAHs as their primary carriers. Both $E_{\rm bump}$ and $q_{\rm PAH}$ correlate with stellar mass, oxygen abundance, and optical depth, and anticorrelate with specific SFR, suggesting that PAHs and the UV bump are suppressed in low-metallicity, dust-poor, and/or intensely star-forming environments. This is consistent with PAH destruction in environments with limited dust shielding and/or strong radiation fields. A principal component analysis of $E_{\rm bump}$, $q_{\rm PAH}$, optical depth, specific SFR, and oxygen abundance explains 97% of the variance, suggesting that previously reported correlations with stellar mass reflect an underlying dependence on metallicity. Finally, variations in dust geometry may explain the wide range of bump amplitudes (0-0.5 mag) at high $q_{\rm PAH}$.

astro-ph.GA↗

In-orbit Performance of the Near-Infrared Spectrograph NIRSpec on the James Webb Space Telescope

The Near-Infrared Spectrograph (NIRSpec) is one of the four focal plane instruments on the James Webb Space Telescope. In this paper, we summarize the in-orbit performance of NIRSpec, as derived from data collected during its commissioning campaign and the first few months of nominal science operations. More specifically, we discuss the performance of some critical hardware components such as the two NIRSpec Hawaii-2RG (H2RG) detectors, wheel mechanisms, and the micro-shutter array. We also summarize the accuracy of the two target acquisition procedures used to accurately place science targets into the slit apertures, discuss the current status of the spectro-photometric and wavelength calibration of NIRSpec spectra, and provide the as measured sensitivity in all NIRSpec science modes. Finally, we point out a few important considerations for the preparation of NIRSpec science programs.

astro-ph.IM↗

The host galaxies of luminous type 2 AGN at $z \sim$0.3-0.4

We study the morphological and structural properties of the host galaxies associated with 57 optically-selected luminous type 2 AGN at $z\sim$0.3-0.4: 16 high-luminosity Seyfert 2 (HLSy2, 8.0$\le$log($L_{\rm [OIII]}/L_{\odot})<$8.3) and 41 obscured quasars (QSO2, log($L_{\rm [OIII]}/L_{\odot})\ge$8.3). With this work, the total number of QSO2 at $z<1$ with parametrized galaxies increases from $\sim$35 to 76. Our analysis is based on HST WFPC2 and ACS images that we fit with {\sc GALFIT}. HLSy2 and QSO2 show a wide diversity of galaxy hosts. The main difference lies in the higher incidence of highly-disturbed systems among QSO2. This is consistent with a scenario in which galaxy interactions are the dominant mechanism triggering nuclear activity at the highest AGN power. There is a strong dependence of galaxy properties with AGN power (assuming $L_ {\rm [OIII]}$ is an adequate proxy). The relative contribution of the spheroidal component to the total galaxy light (B/T) increases with $L_ {\rm [OIII]}$. While systems dominated by the spheoridal component spread across the total range of $L_ {\rm [OIII]}$, most disk-dominated galaxies concentrate at log($L_{\rm [OIII]}/L_{\odot})<$8.6. This is expected if more powerful AGN are powered by more massive black holes which are hosted by more massive bulges or spheroids. The average galaxy sizes ($\langle r_{\rm e} \rangle$) are 5.0$\pm$1.5 kpc for HLSy2 and 3.9$\pm$0.6 kpc for HLSy2 and QSO2 respectively. These are significantly smaller than those found for QSO1 and narrow line radio galaxies at similar $z$. We put the results of our work in context of related studies of AGN with quasar-like luminosities.

astro-ph.GA↗