arXiv subjects

H. Tyagi

Publications and source records attributed to H. Tyagi.

3 recordsLinked to original sources

arXiv2025

Improving Accretion Diagnostics for Young Stellar Objects with Mid-infrared Hydrogen lines from JWST/MIRI

We present a comprehensive study of mid-infrared neutral hydrogen (H~\textsc{i}) emission lines in 79 nearby (d $<$ 200 $pc$) young stars using JWST/MIRI. We aim to identify mid-infrared H~\textsc{i} transitions that can serve as reliable accretion diagnostics in young stars, and evaluate their utility in deriving physical conditions of the accreting gas. We identify and measure 22 H~\textsc{i} transitions in the MIRI wavelength regime (5-28 $\mu m$) and perform LTE slab modelling to remove the H\textsubscript{2}O contribution from selected H~\textsc{i} transitions. We find that mid-IR H~\textsc{i} line emission is spatially compact, even for sources with spatially extended [Ne~\textsc{ii}] and [Fe~\textsc{ii}] jets, suggesting minimal contamination from extended jet. Although Pfund~$\alpha$ (H~\textsc{i}~6--5) and Humphreys~$\alpha$ (H~\textsc{i}~7--6) are the strongest lines, they are blended with H$_2$O transitions. This blending necessitates additional processing to remove molecular contamination, thereby limiting their use as accretion diagnostics. Instead, we identify the H~\textsc{i}~(8--6) at 7.502 $\mu m$ and H~\textsc{i}~(10--7) at 8.760 $\mu m$ transitions as better alternatives, as they are largely unaffected by molecular contamination and offer a more reliable means of measuring accretion rates from MIRI spectra. We provide updated empirical relations for converting mid-IR H~\textsc{i} line luminosities into accretion luminosity for 6 different H~\textsc{i} lines in the MIRI wavelength range. Moreover, comparison of observed line ratios with theoretical models shows that MIR H~\textsc{i} lines offer robust constraints on the hydrogen gas density in accretion columns, $n_\mathrm{H} = $10$^{10.6}$ to 10$^{11.2}$ cm$^{-3}$ in most stars, with some stars exhibiting lower densities ($<10^{10}$~cm$^{-3}$), approaching the optically thin regime.

astro-ph.SR↗

arXiv2025

JWST observations of segregated $^{12}$CO$_2$ and $^{13}$CO$_2$ ices in protostellar envelopes

The evolution of interstellar ices can be studied with thermal tracers such as the vibrational modes of CO$_2$ ice that show great diversity depending on their local chemical and thermal environment. In this work we present JWST observations of the 15.2 $\mu$m bending mode, the 4.39 $\mu$m stretching mode and the 2.70 $\mu$m combination mode of $^{12}$CO$_2$ and $^{13}$CO$_2$ ice in the high-mass protostar IRAS 20126 and the low-mass protostar Per-emb 35. The 15.2 $\mu$m bending mode of both protostars shows the characteristic double peak profile that is associated with pure CO$_2$ ice and a sharp short-wavelength peak is observed at 4.38 $\mu$m in the $^{13}$CO$_2$ bands of the two sources. Furthermore, a narrow short-wavelength feature is detected at 2.69 $\mu$m in the $^{12}$CO$_2$ combination mode of Per-emb 35. We perform a consistent profile decomposition on all three vibrational modes and show that the profiles of all three bands can be reproduced with the same linear combination of CO$_2$ ice in mixtures with mostly CH$_3$OH and H$_2$O ices when the ices undergo segregation due to heating. The findings show that upon heating, CO$_2$ ice is likely segregating from mostly the water-rich ice layer and the CO$_2$-CH$_3$OH component becomes dominant in all three vibrational modes. Additionally, we find that the contribution of the different CO$_2$ components to the total absorption band is similar for both $^{12}$CO$_2$ and $^{13}$CO$_2$. This indicates that fractionation processes must not play a significant role during the different formation epochs, H$_2$O-dominated and CO-dominated. We quantify the $^{12}$CO$_2$ and $^{13}$CO$_2$ ice column densities and derive $^{12}$C/$^{13}$C$_{ice}$ = 90 $\pm$ 9 in IRAS 20126. Finally, we report the detection of the $^{13}$CO$_2$ bending mode of pure CO$_2$ ice at 15.64 $\mu$m in both IRAS 20126 and Per-emb 35.

astro-ph.SR↗

arXiv2024

Hunt for complex cyanides in protostellar ices with JWST: Tentative detection of CH$_3$CN and C$_2$H$_5$CN

Nitrogen-bearing complex organic molecules have been commonly detected in the gas phase but not yet in interstellar ices. This has led to the long-standing question of whether these molecules form in the gas phase or in ices. $\textit{James Webb}$ Space Telescope ($\textit{JWST}$) offers the sensitivity, spectral resolution, and wavelength coverage needed to detect them in ices and investigate whether their abundance ratios are similar in gas and ice. We report the first tentative detection of CH$_3$CN, C$_2$H$_5$CN, and the simple molecule, N$_2$O, based on the CN-stretch band in interstellar ices toward three (HOPS 153, HOPS 370, and IRAS 20126+4104) out of the five protostellar systems observed as part of the Investigating Protostellar Accretion (IPA) GO program with $\textit{JWST}$-NIRSpec. We also provide upper limits for the two other sources with smaller luminosities in the sample. We detect OCN$^-$ in the ices of all sources with typical CH$_3$CN/OCN$^-$ ratios of around 1. Ice and gas column density ratios of the nitrogen-bearing species with respect to each other are better matched than those with respect to methanol, which are a factor of ${\sim}5$ larger in the ices than the gas. We attribute the elevated ice column densities with respect to methanol to the difference in snowline locations of nitrogen-bearing molecules and of methanol, biasing the gas-phase observations toward fewer nitrogen-bearing molecules. Moreover, we find tentative evidence for enhancement of OCN$^-$, CH$_3$CN, and C$_2$H$_5$CN in warmer ices, although formation of these molecules likely starts along with methanol in the cold prestellar phase. Future surveys combining NIRSpec and MIRI, and additional laboratory spectroscopic measurements of C$_2$H$_5$CN ice, are necessary for robust detection and conclusions on the formation history of complex cyanides.

astro-ph.GA↗