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Narendra Nath Patra

Publications and source records attributed to Narendra Nath Patra.

30 records · Page 2Linked to original sources

Molecular scale height in spiral galaxies

Having to have low thermal energy, the molecular gas in galaxies is expected to settle in a thin disc near the midplane. However, contradicting this understanding, recent studies have revealed considerably thick molecular discs in nearby spiral galaxies. To understand this apparent discrepancy, we theoretically model the molecular discs in a sample of eight nearby spiral galaxies and estimate their molecular scale heights (Half Width at Half Maxima (HWHM)). We assume that the baryonic discs are in vertical hydrostatic equilibrium under their mutual gravity in the external force field of the dark matter halo. We set up the joint Poisson's-Boltzman equation of hydrostatic equilibrium and numerically solve it to obtain the three-dimensional molecular gas distribution and determine the scale heights in our sample galaxies. We find that the scale heights follow a universal exponential law with a scale length of $0.46 \pm 0.01 \ r_{25}$. The molecular scale heights in our sample galaxies are found to vary between 50-200 pc depending on the galaxy and radius. Using the density solutions, we build dynamical models of the molecular discs and produce molecular column density maps. These model maps found to match to the observed ones reasonably well. We further incline the dynamical models to an inclination of 90$^o$ to estimate the expected observed thickness of the molecular discs. Interestingly it is found that at edge-on orientation, our sample galaxies under hydrostatic assumption can easily produce a few kpc thick observable molecular disc.

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Gas-dust correlations in nearby galaxies: a case study of NGC 3184 and NGC 7793

The study of gas-dust interactions occurring in the interstellar medium of a galaxy is essential for understanding various physical processes taking place within it. A comparison of such events at different locations corresponding to diverse astrophysical environments provides more insight into the star-formation as well as dust destruction conditions and time-scales. We present a case study for two galaxies: NGC 3184 and NGC 7793, which are typical examples of a `grand design spiral' and a `flocculent spiral', respectively. We investigate the gas-dust correlations at various spatially resolved locations within each galaxy, including spiral arms, using archival data. Moreover, we have segregated the neutral gas into wide (warm) and narrow (cold) velocity components to check the correlations with individual dust emission bands. We find a positive correlation between the gas and the dust, with the total atomic gas emission mainly dominated by its warm component in both the galaxies. We also find the dust population in NGC 7793 to have a greater fraction of emission coming from cold and diffuse, larger-sized dust particles as compared to NGC 3184. This nearby galaxy pilot study could serve as a template for similar studies of larger galaxy samples with analogous morphologies.

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Detection of a slow HI bar in the dwarf irregular galaxy DDO 168

We examine the HI total intensity maps of the VLA LITTLE-THINGS galaxies and identify an HI bar in the dwarf irregular galaxy DDO 168 which has a dense and compact dark matter halo that dominates at all radii. This is only the third galaxy found to host an HI bar. Using the HI kinematic data, we apply the Tremaine-Weinberg method to estimate the pattern speed of the bar. The HI bar is found to have an average pattern speed of $23.3 \pm 5.9$ km/s/kpc. Interestingly, for the first time, we find that the observed pattern speeds of the bar in the two kinematic halves are different. We identify the origin of this difference to be the kinematic asymmetry. This observed offset in the pattern speed serves to put a stringent constraint on the lifetime of the bar set by the winding timescale. The lifetime of the bar is found to be $\sim 5.3 \times 10^8$ years, which is $\sim 2$ times the local dynamical time scale of the disc. We also find the HI bar in DDO 168 to be a weak bar with a strength of $\sim 0.2$. If HI bar being weak can be easily disturbed, this could possibly explain why it is extremely rare to observe HI bars in galaxies. We estimate the bar radius to be $\sim 1$ kpc and the dimensionless ratio, $R_L/R_b$ to be $\geq$ 2.1 indicating a `slow' bar in DDO 168. Our results confirm the proposition that the dynamical friction with the halo slows down a rotating bar in a galaxy dominated by dark matter halo from inner radii.

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A self-consistent hydrostatic mass modelling of pressure supported dwarf galaxy Leo T

Assuming a hydrostatic equilibrium in an HI cloud, the joint Poisson's equation is set up and numerically solved to calculate the expected HI distribution. Unlike previous studies, the cloud is considered to be non-isothermal, and an {\it iterative} method is employed to iteratively estimate the intrinsic velocity dispersion profile using the observed second-moment of the HI data. We apply our {\it iterative} method to a recently discovered dwarf galaxy Leo T and find that its observed HI distribution does not comply with the expected one if one assumes no dark matter in it. To model the mass distribution in Leo T, we solve the Poisson's equation using a large number of trial dark matter halos and compare the model HI surface density ($Σ_{HI}$) profiles to the observed one to identify the best dark matter halo parameters. For Leo T, we find a pseudo-isothermal halo with core density, $ρ_0 \sim 0.67$ $\rm M_{\odot} \thinspace pc^{-3}$ and core radius, $r_s \sim 37$ parsec explains the observation best. The resulting dark matter halo mass within the central 300 pc, $M_{300}$, found to be $\sim 2.7 \times 10^6$ $\rm M_{\odot}$. We also find that a set of dark matter halos with similar $M_{300} \sim 3.7 \times 10^6$ $\rm M_{\odot}$ but very different $ρ_0$ and $r_s$ values, can produce equally good $Σ_{HI}$ profile within the observational uncertainties. This, in turn, indicates a strong degeneracy between the halo parameters and the best fit values are not unique. Interestingly, it also implies that the mass of a dark matter halo, rather than its structure primarily directs the expected HI distribution under hydrostatic equilibrium.

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Molecular scale height in NGC 7331

Combined Poisson's-Boltzman equations of hydrostatic equilibrium were set up and solved numerically for different baryonic components to obtain the molecular scale height as defined by the Half Width at Half Maxima (HWHM) in the spiral galaxy NGC 7331. The scale height of the molecular gas was found to vary between $\sim 100-200$ pc depending on the radius and assumed velocity dispersion. The solutions of the hydrostatic equation and the observed rotation curve were used to produce a dynamical model and consequently a simulated column density map of the molecular disk. The modelled molecular disk found to match with the observed one reasonably well except at the outer disk regions. The molecular disk of NGC 7331 was projected to an inclination of 90$^o$ to estimate its observable edge-on thickness (HWHM), which was found to be $\sim 500$ pc. With an HWHM of $\sim 500$ pc, the observed edge-on extent of the molecular disk was seen to be $\sim$ 1 kpc from the mid-plane. This indicates that in a typical galaxy, hydrostatic equilibrium, in fact, can produce a few kilo-parsec thick observable molecular disk which was thought to be difficult to explain earlier.

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Detection of the Galactic Warm Neutral Medium in HI 21cm absorption

We report a deep Giant Metrewave Radio Telescope (GMRT) search for Galactic H{\sc i} 21cm absorption towards the quasar B0438$-$436, yielding the detection of wide, weak H{\sc i} 21cm absorption, with a velocity-integrated H{\sc i} 21cm optical depth of $0.0188 \pm 0.0036$~km~s$^{-1}$. Comparing this with the H{\sc i} column density measured in the Parkes Galactic All-Sky Survey gives a column density-weighted harmonic mean spin temperature of $3760 \pm 365$~K, one of the highest measured in the Galaxy. This is consistent with most of the H{\sc i} along the sightline arising in the stable warm neutral medium (WNM). The low peak H{\sc i} 21cm optical depth towards B0438$-$436 implies negligible self-absorption, allowing a multi-Gaussian joint decomposition of the H{\sc i} 21cm absorption and emission spectra. This yields a gas kinetic temperature of $\rm T_k \leq (4910 \pm 1900)$~K, and a spin temperature of $\rm T_s = (1000 \pm 345)$~K for the gas that gives rise to the H{\sc i} 21cm absorption. Our data are consistent with the H{\sc i} 21cm absorption arising from either the stable WNM, with $\rm T_s \ll T_k$, $\rm T_k \approx 5000$~K, and little penetration of the background Lyman-$α$ radiation field into the neutral hydrogen, or from the unstable neutral medium, with $\rm T_s \approx T_k \approx 1000\;K$.

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FIGGS2: An HI survey of extremely faint irregular galaxies

We present the observations and first results from the FIGGS2 survey. FIGGS2 is an extension of the earlier Faint Irregular Galaxies GMRT survey (FIGGS) towards faint luminosity end. The sample consists of 20 galaxies of which 15 were detected in HI 21cm line using the Giant Meter-wave Radio Telescope (GMRT). The median blue band magnitude of our sample is ~ -11.6, which is more than one magnitude fainter than earlier FIGGS survey. From our GMRT observations we find that, for many of our sample galaxies, the HI disks are offset from their optical disks. The HI diameters of the FIGGS2 galaxies show a tight correlation with their HI mass. The slope of the correlation is 2.08 +/- 0.20 similar to what is found for FIGGS galaxies. We also find that for almost all galaxies, the HI disks are larger than the optical disks which is a common trend for dwarf or spiral galaxies. The mean value of the ratio of HI to optical diameter is ~ 1.54.

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Cold HI in faint dwarf galaxies

We present the results of a study of the amount and distribution of cold atomic gas, as well its correlation with recent star formation in a sample of extremely faint dwarf irregular galaxies. Our sample is drawn from the Faint Irregular Galaxy GMRT Survey (FIGGS) and its extension, FIGGS2. We use two different methods to identify cold atomic gas. In the first method, line-of-sight HI spectra were decomposed into multiple Gaussian components and narrow Gaussian components were identified as cold HI. In the second method, the brightness temperature (T_B) is used as a tracer of cold HI. We find that the amount of cold gas identified using the T_B method is significantly larger than the amount of gas identified using Gaussian decomposition. We also find that a large fraction of the cold gas identified using the T_B method is spatially coincident with regions of recent star formation, although the converse is not true. That is only a small fraction of the regions with recent star formation are also covered by cold gas. For regions where the star formation and the cold gas overlap, we study the relationship between the star formation rate density and the cold \HI column density. We find that the star formation rate density has a power law dependence on the HI column density, but that the slope of this power law is significantly flatter than that of the canonical Kennicutt-Schmidt relation.

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Modeling HI distribution and kinematics in the edge-on dwarf irregular galaxy KK250

We model the observed vertical distribution of the neutral hydrogen (HI) in the faint (M_B ~ -13.7 mag) edge-on dwarf irregular galaxy KK250. Our model assumes that the galaxy consists of axi-symmetric, co-planar gas and stellar discs in the external force-field of a spherical dark matter halo, and in vertical hydrostatic equilibrium. The velocity dispersion of the gas is left as a free parameter in the model. Our best fit model is able to reproduce the observed vertical distribution of the HI gas, as well as the observed velocity profiles. The best fit model has a large velocity dispersion (~ 22 km/s) at the centre of the galaxy, which falls to a value of ~ 8 km/s by a galacto-centric radius of ~ 1 kpc, which is similar to both the scale-length of the stellar disc, as well as the angular resolution of the data along the radial direction. Similarly we find that the thickness of the HI disc is also minimum at ~ 1 kpc, and increases by about a factor of ~ 2 as one goes to the centre of the galaxy or out to ~ 3 kpc. The minimum intrinsic HWHM of the HI vertical distribution in KK250 is ~ 350 pc. For comparison the HWHM of the vertical distribution of the HI in the solar neighbourhood is ~ 70-140 pc. Our results are hence consistent with other observations which indicate that dwarf galaxies have significantly puffier gas discs than spirals.

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Stringent constraints on the H I spin temperature in two z > 3 Damped Lyman-alpha systems from redshifted 21 cm absorption studies

Physical properties of Damped Lyman-alpha absorbers and their evolution are closely related to galaxy formation and evolution theories, and have important cosmological implications. H I 21 cm absorption study is one useful way of measuring the temperature of these systems. In this work, very strong constraints on the temperature of two Damped Lyman-alpha absorbers at z > 3 are derived from low radio frequency observations. The H I spin temperature is found to be greater than 2000 K for both the absorbers. The high spin temperature of these high-redshift systems is in agreement with the trend found in a compilation of temperatures for other Damped Lyman-alpha absorbers. We also argue that the temperature - metallicity relation, reported earlier in the literature, is unlikely to be a spurious line of sight effect, and that the redshift evolution of the spin temperature does not arises due to a selection effect. All of these are consistent with a redshift evolution of the warm gas fraction in Damped Lyman-alpha systems.

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A slow bar in the dwarf irregular galaxy NGC 3741

Using the Tremaine-Weinberg method, we measure the speed of the HI bar seen in the disk of NGC 3741. NGC 3741 is an extremely gas rich galaxy with an {H\,{\sc i}} disk which extends to about 8.3 times its Holmberg radius. It is also highly dark matter-dominated. Our calculated value of the pattern speed $Ω_p$ is 17.1 $\pm$ 3.4 km $\textrm{s}^{-1}\textrm{kpc}^{-1}$. We also find the ratio of the co-rotation radius to the bar semi-major axis to be (1.6 $\pm$ 0.3), indicating a slow bar. This is consistent with bar models in which dynamical friction results in a slow bar in dark matter dominated galaxies.

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The HI column density distribution function in faint dwarf galaxies

We present the HI column density distribution function,\fnh, as measured from dwarf galaxies observed as part of the Faint Irregular Galaxy GMRT (FIGGS) survey. We find that the shape of the dwarf galaxy \fnh\ is significantly different from the \fnh\ for high redshift Damped \lya\ absorbers (DLAs) or the \fnh\ for a representative sample of $z = 0$ gas rich galaxies. The dwarf \fnh\ falls much more steeply at high HI column densities as compared to the other determinations. While $\sim 10%$ of the cross section above $\nh = 10^{20.3} \acc$ at $z = 0$ is provided by dwarf galaxies, the fraction falls to $\lesssim 1%$ by $\nh \sim 10^{21.5} \acc.$ In the local universe, the contribution to the high \nh\ end of the \fnh\ distribution comes predominantly from the inclined disks of large galaxies. Dwarf galaxies, both because of their smaller scale lengths, and their larger intrinsic axial ratios do not produce large HI column densities even when viewed edge-on. If high column density DLAs/GRB hosts correspond to galaxies like the local dwarfs, this would require either that (i) the absorption arises from merging and not isolated systems or (ii) the observed lines of sight are strongly biased towards high column density regions.

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