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Spatially resolved comparison of SFRs from UV and H$\alpha$ in GASP gas-stripped galaxies
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abstract
Star-formation rates (SFR) in galaxies offer a view of various physical processes across them and are measured using various tracers, such as H$\alpha$ and UV. Different physical mechanisms can affect H$\alpha$ and UV emission, resulting in a discrepancy in the corresponding SFR estimates ($\Delta SFR$). We investigate the effects of ram pressure on the SFR measurements and $\Delta SFR$ across 5 galaxies from the GASP survey caught in the late stages of gas stripping due to ram pressure. We probe spatially resolved $\Delta SFR$ at pixel scales of 0.5 kpc, and compare disks to tails, and regions dominated by the dense gas to diffuse ionized gas (DIG) regions. The regions dominated by dense gas show similar SFR values for UV and H$\alpha$ tracers, while the regions dominated by the DIG show up to 0.5 dex higher SFR(UV). There is a large galaxy-by-galaxy variation in $\Delta SFR$, with no difference between the disks and the tails. We discuss the potential causes of variations in $\Delta SFR$ between the dense gas and DIG areas. We conclude that the dominant cause of discrepancy is recent variations in star formation histories, where star formation recently dropped in the DIG-dominated regions leading to changes in $\Delta SFR$. The areal coverage of the tracers shows areas with H$\alpha$ and no UV emission; these areas have LINER-like emission (excess in $[OI\lambda\,6300]/H\alpha$ line ratio), indicating that they are ionized by processes other than star-formation.
Forward citations
Cited by 2 Pith papers
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Star formation at different stages of ram-pressure stripping as observed through far-ultraviolet imaging of 13 GASP galaxies
FUV imaging of 13 GASP jellyfish galaxies shows star-forming tails in strong stripping cases and suggests unresolved H-alpha tails without FUV are powered by non-star-formation processes.
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JWST PRIMER: strong evidence for the environmental quenching of low-mass galaxies out to $\mathbf{\textit{z} \simeq 2}$
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