arXiv subjects

J. Michael Shull

Publications and source records attributed to J. Michael Shull.

At least 19 recordsLinked to original sources

arXiv2026

Observations of High Galactic Latitude Line and Continuum Emission (912 - 1600 \AA) with New Horizons

We present observations of the cosmic ultraviolet background (CUVB) from 912 - 1600 A using the Stem aperture of the Alice spectrograph on the New Horizons spacecraft at 56 AU from the Sun, providing a spectral resolution of 9 A for diffuse sources. We detect emission lines of CIII (977 A) and CIV (1548/1551 A) at the 3 sigma level with strengths of 4200 +/- 1500 and 4100 +/- 1200 ph cm(-2) s(-1) sr(-1), respectively, and a marginal detection of OVI (1032/1038 A) at 1400 +/- 1300 ph cm(-2) s(-1) sr(-1). We report a 3 sigma detection of an emission line at 1135 A, which we have identified with the N I resonance triplet. Although this line had earlier been observed in FUSE and SPEAR data, it had been attributed to airglow or instrumental effects. We confirm, for the first time, that it must originate in the Galaxy. The dust-scattered continuum is dominated by a small number (N < 100) of O9 - B2 stars and shows the deep absorption feature near 1000 A seen in the stellar spectrum. Our models suggest an albedo of a < 0.5 over most of the spectrum (950 -- 1550 A) for the dust grains with the phase function asymmetry of g < 0.6. We find an offset, comprising the extragalactic background light and halo contributors, consistent with our earlier results from the Box, including the decline in the offset near the Lyman limit. We confirm that much of the emission must be from an unidentified component of the CUVB.

astro-ph.GA↗

arXiv2026

High-S/N Quasar Observations with HST/COS: Deep Fields for Spectroscopy

Hubble is still in prime observing condition for making transformative discoveries in UV astronomy. In this white paper we describe the science case for a deep (S/N>30) UV spectroscopic survey with HST/COS targeting approximately 20 QSOs at 0.5<z<1.5 at good resolution (20 km/s). This survey would capitalize on our current UV capability, produce a legacy dataset enabling community science in many areas of galactic and extragalactic research, and pioneer a path for future UV science with the Habitable Worlds Observatory. Such high-S/N spectra are largely missing from the MAST archives, and would be analogous to the deep Hubble imaging fields (HDF, UDF, Frontier Fields) that have been enormously successful and far-reaching in their science impact. This legacy dataset would enable frontier science programs in several areas, including (1) studies of the CGM and IGM at unparalleled sensitivity, covering a wide range of UV metal lines and reaching very low H I column densities of log N=12.6 and low metallicities near [Z/H]=-2, enabling precision studies of the chemical abundances, ionization, temperature, and baryon and metal budgets of the CGM and IGM; (2) diffuse gas in the Milky Way and Local Group, including high-velocity clouds and gas streams from satellite mergers; (3) AGN outflows, which would be probed in the rest-frame extreme ultraviolet (EUV), covering continuum-generation mechanisms and diagnostics of gas in accretion-disk outflows.

astro-ph.GA↗

arXiv2026

Closing the UV Gap: Rest-frame EUV science from high-redshift QSOs as a legacy-defining capability

The Hubble Space Telescope is the only high-resolution ultraviolet spectroscopic facility that will exist until the Habitable Worlds Observatory (HWO) achieves first light in the mid-2040s. We describe a coherent class of science, coupling rest-frame extreme-ultraviolet (EUV; 1--4 Ryd, 228--912 {\AA}) absorption and continuum spectroscopy of intermediate-redshift quasars at $z = 1-2$, shifting the rest-frame EUV photons into the HST/COS far-UV bandpass. This science on quasars and gas in the IGM and CGM is doubly perishable. The COS detector sensitivity is declining, just as new quasars are found (Milliquas, UVQS, and soon Rubin, Roman, and Euclid). Thus, the window to reach UV-bright quasars at $z>1$ QSOs narrows with every deferred orbit. Expanding HST UV orbit allocations in the 2030s would deliver a step-change in warm-hot CGM/IGM science and produce the first systematic, empirical EUV SED census of QSOs. These datasets will serve as the foundational low-redshift anchor for HWO science. This recommendation makes the scientific and strategic case for an expansion of the HST/COS spectroscopic data base on intermediate redshift AGN in their rest-frame EUV.

astro-ph.GA↗

arXiv2025

Ionization Sources of the Local Interstellar Clouds: Two B-stars, Three White Dwarfs, and the Local Hot Bubble

The dominant sources of photoionizing radiation in the extreme ultraviolet (EUV) incident on the exterior of the local interstellar clouds include two nearby early B-type stars, $ε$ CMa ($124\pm2$ pc) and $β$ CMa ($151\pm5$ pc), three hot dwarfs, and the local hot bubble (LHB). Line emission (170-912A) from highly ionized metals (Fe, Ne, Mg) in million-degree LHB plasma may be responsible for the elevated ionization fractions of helium ($n_{\rm HeII}/n_{\rm He} \approx 0.4$) compared to hydrogen ($n_{\rm HII} / n_{\rm H} \approx 0.2$) in the local clouds. We update the stellar parameters and ionizing flux for $β$ CMa, after correcting the EUV spectra for intervening HI column density, $N_{\rm HI} = 1.9\pm0.1\times10^{18}~{\rm cm}^{-2}$, and its hotter effective temperature, $T_{\rm eff} \approx 25,000$K vs. 21,000K for $ε$ CMa. These two stars produce a combined H-ionizing photon flux $Φ_{\rm H} \approx 6800\pm1400$ cm$^{-2}$ s$^{-1}$ at the external surface of the local clouds. The hot bubble could produce comparable fluxes, $Φ_{\rm H} =$ 2000-9000 cm$^{-2}$ s$^{-1}$, depending on the amount of metal depletion into dust grains that survive sputtering. The radial velocities and proper motions of $β$ CMa and $ε$ CMa indicate that both stars passed within $10\pm1$ pc of the Sun $4.4\pm0.1$ Myr ago, with 100-200 times higher local ionizing fluxes. At that time, the local clouds were likely farther from the Sun, owing to their transverse motion. Over the last few Myr, EUV radiation from these two stars left a wake of highly ionized gas in a hot, low-density cavity produced by past supernova explosions in the Sco-Cen OB association and connected with the LHB.

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arXiv2025

Quasar Spectral Energy Distributions in the Rest-Frame EUV: Hubble-COS Spectra of Two Ultra-luminous Quasars

Using the Cosmic Origins Spectrograph (COS) aboard the Hubble Space Telescope with both far-UV (FUV) and near-UV (NUV) gratings, we measure the ionizing spectra of two bright, intermediate-redshift quasars in their rest-frame extreme ultraviolet (EUV). The availability of both NUV and FUV spectra allows us to define the quasar continuum and correct for strong Lyman-limit systems (LLS) that fall in the gap between the FUV and optical. Each AGN has a prominent LLS, but the flux recovery shortward of their Lyman edges allows us to fit and restore the true AGN continuum. In the EUV (450-912 A) these AGN have flux distributions, $F_ν \propto ν^{-α_ν}$, with spectral indices $α_ν = 1.11\pm0.22$ (SBS 1010+535, $z_{\rm AGN} = 1.5086$) and $α_ν = 0.98\pm0.22$ (HS 0747+4259, $z_{\rm AGN} = 1.9006$), both considerably harder than the mean index, $α_ν = 1.41\pm0.15$, in a COS composite spectrum of 159 UV-bright AGN. These two AGN are outliers in the index distribution, perhaps resulting from their extremely high UV luminosity ($10^{48}~{\rm erg~s}^{-1}$), estimated black-hole masses (0.5-1)$\times10^{10} M_{\odot}$, and effects on the inner accretion disk and Comptonized winds.

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arXiv2025

Beta Canis Majoris: The Other Major Ionization Source of the Local Interstellar Clouds

Two nearby B-type stars, $ε$ CMa ($124\pm2$ pc) and $β$ CMa ($151\pm5$ pc), are important contributors to the photoionization of the local interstellar clouds. At spectral type B1 II-III, $β$ CMa is slightly hotter than $ε$ CMa (B2 II-III), but its ionizing flux at Earth is attenuated by a much larger H I column density. At the external surface of the clouds, the two stars produce similar fluxes in the Lyman continuum (LyC). From the $β$ CMa angular diameter, bolometric flux, and position on the Hertzsprung-Russell diagram, we obtain a consistent set of stellar parameters: $T_{\rm eff} = 25,180\pm1120$ K, $\log g = 3.70\pm0.08$, radius $R = 8.44\pm0.56\,R_{\odot}$, mass $M = 13\pm1\,M_{\odot}$, and luminosity $L = 10^{4.41\pm0.06}\, L_{\odot}$. The EUVE-observed fluxes and non-LTE model atmospheres are used to determine the ionizing photon production rate $Q_{\rm H} = 10^{46.0}$ photons s$^{-1}$ and fluxes incident on the local clouds, $Φ_{\rm HI} \approx 3700$ cm$^{-2}$ s$^{-1}$ and $Φ_{\rm HeI} \approx 110$ cm$^{-2}$ s$^{-1}$ in the H I and He I continua. The corresponding photoionization rates are $Γ_{\rm HI} \approx 1.5\times10^{-14}$ s$^{-1}$ and $Γ_{\rm HeI} \approx 7.3\times10^{-16}$ s$^{-1}$. Within the local cloud, the LyC flux is attenuated by an H I column density $N_{\rm HI} = (1.9\pm0.1)\times10^{18}$ cm$^{-2}$, with optical depth $τ_{\rm LL} = 12.0\pm 0.6$ at the Lyman limit. The radial velocities and proper motions of $β$ CMa and $ε$ CMa indicate that both stars passed within $10\pm1$ pc of the Sun approximately 4.4 Myr ago, with incident ionizing fluxes 180-200 times larger. Their EUV radiation photoionized and heated the tunnel in the local interstellar gas, associated dynamically with past supernova explosions in the Sco-Cen OB association.

astro-ph.GA↗

arXiv2025

Excess Ultraviolet Emission at High Galactic Latitudes: A New Horizons View

We present new observations of the cosmic ultraviolet background (CUVB) at high Galactic latitudes ($|b| > 40^{\circ}$), made using the Alice UV spectrograph on board the New Horizons spacecraft. These observations were taken at about 57 AU from the Sun, outside much of the foreground emission affecting previous missions, and allowed a new determination of the spectrum of the CUVB between 912 -- 1100~Å and 1400 -- 1800~Å. We found a linear correlation between the CUVB and the Planck E(B~-~V) with offsets at zero-reddening of $221 \pm 11$ photon units at 1000~Å and $264 \pm 24$ \photu\ at 1500~Å ($4.4 \pm 0.2$ nW m$^{-2}$ sr$^{-1}$ at 1000~Å and $5.3 \pm 0.5$ nW m$^{-2}$ sr$^{-1}$ at 1500~Å). The former is the first firm detection of the offset in the range 912 -- 1100 Å while the latter result confirms previous results from \galex, showing that there is little emission from the Solar System from 1400 -- 1800 Å. About half of the offset may be explained by known sources (the integrated light of unresolved galaxies, unresolved stars, emission from ionized gas, and two-photon emission from warm hydrogen in the halo) with the source of the remaining emission as yet unidentified. There is no detectable emission below the Lyman limit with an upper limit of $3.2 \pm 3.0$ photon units.

astro-ph.GA↗

arXiv2024

Epsilon Canis Majoris: The Brightest EUV Source with Surprisingly Low Interstellar Absorption

The B2 star $ε$ CMa, at parallax distance $d = 124\pm2$~pc, dominates the H I photoionization of the local interstellar cloud (LIC). At its closer parallax distance compared to previous estimates, $ε$ CMa has a 0.9 mag fainter absolute magnitude $M_V =-3.97\pm0.04$. We combine measurements of distance with the integrated flux $f = (41.5\pm3.3) \times 10^{-6}~{\rm erg~cm}^{-2}~{\rm s}^{-1}$ and angular diameter $θ_d = 0.80\pm0.05$~mas to produce a consistent set of stellar parameters: radius $R = 10.7\pm0.7~R_{\odot}$, mass $M = 13.1\pm2.3~M_{\odot}$, gravity $\log g = 3.50\pm0.05$, effective temperature $T_{\rm eff} \approx 21,000$~K, and luminosity $L \approx 20,000~L_{\odot}$. These parameters place Epsilon CMa outside the $β$ Cephei instability strip, consistent with its observed lack of pulsations. The observed EUV spectrum yields a hydrogen photoionization rate $Γ_{\rm HI} \approx 10^{-15}$ s$^{-1}$ (at Earth). The total flux decrement factor at the Lyman limit ($Δ_{\rm LL} = 5000\pm500$) is a combination of attenuation in the stellar atmosphere ($Δ_{\rm star} = 110\pm10$) and interstellar medium ($Δ_{\rm ISM} = 45\pm5$) with optical depth $τ_{\rm LL} = 3.8\pm0.1$. After correcting for interstellar HI column density $N_{\rm HI} = (6\pm1)\times10^{17}~{\rm cm}^{-2}$, we find a stellar LyC photon flux $Φ_{\rm LyC} \approx 3000~{\rm cm}^{-2}~{\rm s}^{-1}$ and ionizing luminosity $Q_{\rm LyC} = 10^{45.7\pm0.3}$ photons s$^{-1}$. The photoionization rate $Γ_{\rm H} \approx$ (1-2)$\times 10^{-14}~{\rm s}^{-1}$ at the cloud surface produces an ionization fraction (30-40\%) for total hydrogen density $n_{\rm H} = 0.2$ cm$^{-3}$. With its $27.3\pm0.4$ km/s heliocentric radial velocity and small proper motion, $ε$ CMa passed within $9.3\pm0.5$ pc of the Sun 4.4 Myr ago, with a 180 times higher photoionization rate.

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arXiv2024

New Synoptic Observations of the Cosmic Optical Background with New Horizons

We obtained New Horizons LORRI images to measure the cosmic optical background (COB) intensity integrated over $0.4\lesssimλ\lesssim0.9{~\rmμm}.$ The survey comprises 16 high Galactic-latitude fields selected to minimize scattered diffuse Galactic light (DGL) from the Milky Way galaxy, as well as scattered light from bright stars. This work supersedes an earlier analysis based on observations of one of the present fields. Isolating the COB contribution to the raw total sky levels measured in the fields requires subtracting the remaining scattered light from bright stars and galaxies, intensity from faint stars within the fields fainter than the photometric detection-limit, and the DGL foreground. DGL is estimated from Planck HFI $350 {~\rmμm}$ and $550 {~\rmμm}$ intensities, using a new self-calibrated indicator based on the 16 fields augmented with eight additional DGL calibration fields obtained as part of the survey. The survey yields a highly significant detection ($6.8σ$) of the COB at ${\rm 11.16\pm 1.65~(1.47~sys,~0.75~ran) ~nW ~m^{-2} ~sr^{-1}}$ at the LORRI pivot wavelength of 0.608 $μ$m. The estimated integrated intensity from background galaxies, ${\rm 8.17\pm 1.18 ~nW ~m^{-2} ~sr^{-1}},$ can account for the great majority of this signal. The rest of the COB signal, ${\rm 2.99\pm2.03~ (1.75~sys,~1.03~ran) ~nW ~m^{-2} ~sr^{-1}},$ is formally classified as anomalous intensity but is not significantly different from zero. The simplest interpretation is that the COB is completely due to galaxies.

astro-ph.GA↗

arXiv2023

Variations of Interstellar Gas-to-Dust Ratios at High Galactic Latitudes

Interstellar dust at high Galactic latitudes can influence astronomical foreground subtraction, produce diffuse scattered light, and soften the ultraviolet spectra of quasars. In a sample of 94 sight lines toward quasars at high latitude and low extinction, we evaluate the interstellar "gas-to-dust ratio" $N_{\rm H}/E(B-V)$, using hydrogen column densities (H I and H$_2$) and far-infrared estimates of dust reddening. In the Galactic plane, this ratio is $6.0\pm0.2$ (in units of $10^{21}~{\rm cm}^{-2}~{\rm mag}^{-1}$). On average, recent Planck estimates of $E(B-V)$ in low-reddening sight lines are 12% higher than those from Schlafly & Finkbeiner (2011), and $N_{\rm HI}$ exhibits significant variations when measured at different radio telescopes. In a sample of 51 quasars with measurements of both H I and H$_2$ and $0.01 \leq E(B-V) \lesssim 0.1$, we find mean ratios $10.3\pm0.4$ (gas at all velocities) and $9.2\pm0.3$ (low velocity only) using Planck $E(B-V)$ data. High-latitude H$_2$ fractions are generally small (2-3% on average), although 9 of 39 sight lines at $|b| \geq 40^{\circ}$ have $f_{\rm H2}$ of 1-17%. Because FIR-inferred $E(B-V)$ is sensitive to modeled dust temperature $T_d$ and emissivity index $β$, gas-to-dust ratios have large, asymmetric errors at low $E(B-V)$. The ratios are elevated in sight lines with high-velocity clouds, which contribute $N_{\rm H}$ but little reddening. In Complex C, the ratio decreases by 40% when high velocity gas is excluded. Decreases in dust content are expected in low-metallicity gas above the Galactic plane, resulting from grain destruction in shocks, settling to the disk, and thermal sputtering in hot halo gas.

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arXiv2023

The Spatial and Emission Properties of the Large [O III] Emission Nebula Near M31

Drechsler et al. (2023) reported the unexpected discovery of a 1.5 degree long [O III] emission nebula 1.2 degrees southeast of the M31 nucleus. Here we present additional images of this large emission structure, called SDSO, along with radial velocity and flux measurements from low-dispersion spectra. Independent sets of [O III] images show SDSO to be composed of broad streaks of diffuse emission aligned NE-SW. Deep H$α$ images reveal no strong coincident emission suggesting a high [O III]/H$α$ ratio. We also find no other [O III] emission nebulosity as bright as SDSO within several degrees of M31 and no filamentary H$α$ emission connected to SDSO. Optical spectra taken along the arc's northern limb reveal [O III] $λλ$4959,5007 emissions matching the location and extent seen in our [O III] images. The heliocentric velocity of this [O III] nebulosity is $-9.8 \pm 6.8$ km s$^{-1}$ with a peak surface brightness of $(4\pm2) \times 10^{-18}$ erg s$^{-1}$ cm$^{-2}$ arcsec$^{-2}$ ($\sim$0.55 Rayleigh). We discuss SDSO as a possible unrecognized supernova remnant, a large and unusually nearby planetary nebula, a stellar bow shock nebula, or an interaction of M31's outer halo gas with high-velocity circumgalactic gas. We conclude that galactic origins for SDSO are unlikely and favor instead an extragalactic M31 halo--circumgalactic cloud interaction scenario, despite the nebula's low radial velocity. We then describe new observations that may help resolve the nature and origin of this large nebulosity so close to M31 in the sky.

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arXiv2023

Interstellar Bow Shocks around Fast Stars Passing through the Local Interstellar Medium

Bow-shocks are produced in the local interstellar medium by the passage of fast stars from the Galactic thin-disk and thick-disk populations with velocities $V_* = $ 40-80 km/s. Stellar transits of local H I clouds occur every 3500-7000 yr on average and last between $10^4$ and $10^5$ yr. There could be 10-20 active bow shocks around low-mass stars inside clouds within 10-15 pc of the Sun. At local cloud distances of 3-10 pc, their turbulent wakes have transverse radial extents $R_{\rm wake} \approx$ 10-300 AU, angular sizes 10-100 arcsec, and Lyman-alpha surface brightnesses of 2-8 Rayleighs in gas with total hydrogen density $n_H \approx 0.1~{\rm cm}^{-3}$ and $V_* =$ 40-80 km/s. These transit wakes may cover an area fraction $f_A \approx (R_{\rm wake}/R_{\rm cl}) \approx 10^{-3}$ of local H I clouds and be detectable in IR (dust), UV (Lya, two-photon), or non-thermal radio emission. Turbulent heating in these wakes could produce the observed elevated rotational populations of H$_2$ ($J \geq 2$) and influence the endothermic formation of CH$^+$ in diffuse interstellar gas at $T > 10^3$ K.

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arXiv2023

The Distribution of Metallicities in the Local Galactic Interstellar Medium

In this investigation, we present an analysis of the metallicity distribution that pertains to neutral gas in the local Galactic interstellar medium (ISM). We derive relative ISM metallicities for a sample of 84 sight lines probing diffuse atomic and molecular gas within 4 kpc of the Sun. Our analysis is based, in large part, on column density measurements reported in the literature for 22 different elements that are commonly studied in interstellar clouds. We supplement the literature data with new column density determinations for certain key elements and for several individual sight lines important to our analysis. Our methodology involves comparing the relative gas-phase abundances of many different elements for a given sight line to simultaneously determine the strength of dust depletion in that direction and the overall metallicity offset. We find that many sight lines probe multiple distinct gas regions with different depletion properties, which complicates the metallicity analysis. Nevertheless, our results provide clear evidence that the dispersion in the metallicities of neutral interstellar clouds in the solar neighborhood is small ($\sim$0.10 dex) and only slightly larger than the typical measurement uncertainties. We find no evidence for the existence of very low metallicity gas (as has recently been reported by De Cia et al.) along any of the 84 sight lines in our sample. Our results are consistent with a local Galactic ISM that is well mixed and chemically homogeneous.

astro-ph.GA↗

arXiv2023

Two-photon production in low-velocity shocks

The Galactic interstellar medium abounds in low-velocity shocks with velocities less than, say, about 70 km/s. Some are descendants of higher velocity shocks, while others start off at low velocity (e.g., stellar bow shocks, intermediate velocity clouds, spiral density waves). Low-velocity shocks cool primarily via Ly-alpha, two-photon continuum, optical recombination lines (e.g., H-alpha), free-bound emission, free-free emission and forbidden lines of metals. The dark far-ultraviolet (FUV) sky, aided by the fact that the two-photon continuum peaks at 1400 angstroms, makes the FUV band an ideal tracer of low-velocity shocks. Recent GALEX FUV images reaffirm this expectation, discovering faint and large interstellar structure in old supernova remnants and thin arcs stretching across the sky. Interstellar bow shocks are expected from fast stars from the Galactic disk passing through the numerous gas clouds in the local interstellar medium within 15 pc of the Sun. Using the best atomic data available to date, we present convenient fitting formulae for yields of Ly$α$, two-photon continuum and H$α$ for pure hydrogen plasma in the temperature range of 10^4 K to 10^5 K. The formulae presented here can be readily incorporated into time-dependent cooling models as well as collisional ionization equilibrium models.

astro-ph.GA↗

arXiv2021

A Far Ultraviolet Spectroscopic Explorer Survey of Interstellar Molecular Hydrogen in the Galactic Disk

We report results from a FUSE survey of interstellar molecular hydrogen (H2) in the Galactic disk toward 139 O-type and early B-type stars at Galactic latitudes $|b| < 10^{\circ}$, with updated photometric and parallax distances. The H2 absorption is measured using the far-ultraviolet Lyman and Werner bands, including strong R(0), R(1), and P(1) lines from rotational levels $J = 0$ and $J = 1$ and excited states up to $J = 5$ (sometimes $J = 6$ and 7). For each sight line, we report column densities $N_{H2}$, $N_{HI}$, $N(J)$, $N_H = N_{HI} + 2N_{H2}$, and molecular fraction, $f_{H2} = 2N_{H2}/N_H$. Our survey extends the 1977 Copernicus H2 survey up to $N_H \sim 5\times10^{21}$ cm$^{-2}$. The lowest rotational states have mean excitation temperatures and rms dispersions, $T_{01} = 88\pm 20$ K and $T_{02} = 77\pm18$ K, suggesting that J = 0,1,2 are coupled to the gas kinetic temperature. Populations of higher-J states exhibit mean excitation temperatures, $T_{24} = 237\pm91$ K and $T_{35} = 304\pm108$ K, produced primarily by UV radiative pumping. Correlations of $f_{H2}$ with E(B-V) and N_H show a transition to $f_{H2} \geq 0.1$ at $N_ H \geq 10^{21}$ cm$^{-2}$ and $E(B-V) > 0.2$, interpreted with an analytic model of H2 formation-dissociation equilibrium and attenuation of the far-UV radiation field by self-shielding and dust opacity. Results of this disk survey are compared to previous FUSE studies of H2 in translucent clouds, at high Galactic latitudes, and in the Magellanic Clouds. Using updated distances to the target stars, we find average sight-line values $\langle f_{H2} \rangle \geq 0.20$ and $\langle N_H/E(B-V) \rangle = (6.07\pm1.01)\times10^{21}$ cm$^{-2}$ mag$^{-1}$.

astro-ph.GA↗

arXiv2019

Distances to Galactic OB-stars: Photometry vs. Parallax

For application to surveys of interstellar matter and Galactic structure, we compute new spectrophotometric distances to 139 OB stars frequently used as background targets for UV spectroscopy. Many of these stars have updated spectral types and digital photometry with reddening corrections from the Galactic O-Star (GOS) spectroscopic survey. We compare our new photometric distances to values used in previous IUE and FUSE surveys and to parallax distances derived from Gaia-DR2, after applying a standard (0.03 mas) offset from the quasar celestial reference frame. We find substantial differences between photometric and parallax distances (at d > 1.5 kpc) with increasing dispersion when parallax errors exceed 8%. Differences from previous surveys arise from new GOS stellar classifications, especially luminosity classes, and from reddening corrections. We apply our methods to two OB associations. For Perseus OB1 (nine O-stars) we find mean distances of $2.47\pm0.57$ kpc (Gaia parallax) and $2.99\pm0.14$ kpc (photometric) using a standard grid of absolute magnitudes (Bowen et al. 2008). For 29 O-stars in Car OB1 associated with Trumpler-16, Trumpler-14, Trumpler-15, and Collinder-228 star clusters, we find $2.87\pm0.73$ kpc (Gaia parallax) and $2.60\pm0.28$ kpc (photometric). Using an alternative grid of O-star absolute magnitudes (Martins et al. 2005) shifts these photometric distances 7% closer. Improving the distances to OB-stars will require attention to spectral types, photometry, reddening, binarity, and the grid of absolute magnitudes. We anticipate that future measurements in Gaia-DR3 will improve the precision of distances to massive star-forming regions in the Milky Way.

astro-ph.SR↗

arXiv2019

Warm H$_2$ as a probe of massive accretion and feedback through shocks and turbulence across cosmic time

Galaxy formation depends on a complex interplay between gravitational collapse, gas accretion, merging, and feedback processes. Yet, after many decades of investigation, these concepts are poorly understood. This paper presents the argument that warm H$_2$ can be used as a tool to unlock some of these mysteries. Turbulence, shocks and outflows, driven by star formation, AGN activity or inflows, may prevent the rapid buildup of star formation in galaxies. Central to our understanding of how gas is converted into stars is the process by which gas can dissipate its mechanical energy through turbulence and shocks in order to cool. H$_2$ lines provide direct quantitative measurements of kinetic energy dissipation in molecular gas in galaxies throughout the Universe. Based on the detection of very powerful H$_2$ lines from z = 2 galaxies and proto-clusters at the detection limits of {\it Spitzer}, we are confident that future far-IR and UV H$_2$ observations will provide a wealth of new information and insight into galaxy evolution to high-z. Finally, at the very earliest epoch of star and galaxy formation, warm H$_2$ may also provide a unique glimpse of molecular gas collapse at 7 $<$ z $<$ 12 in massive dark matter (DM) halos on their way to forming the very first galaxies. Such measurements are beyond the reach of existing and planned observatories.

astro-ph.GA↗

arXiv2018

A Galaxy Redshift Survey near HST/COS AGN Sight Lines

To establish the connection between galaxies and UV-detected absorption systems in the local universe, a deep ($g\leq20$) and wide ($\sim20^{\prime}$ radius) galaxy redshift survey is presented around 47 sight lines to UV-bright AGN observed by the Cosmic Origins Spectrograph (COS). Specific COS science team papers have used this survey to connect absorbers to galaxies, groups of galaxies, and large-scale structures, including voids. Here we present the technical details of the survey and the basic measurements required for its use, including redshifts for individual galaxies and uncertainties determined collectively by spectral class (emission-line, absorption-line, and composite spectra) and completeness for each sight line as a function of impact parameter and magnitude. For most of these sight lines the design criteria of $>90$% completeness over a $>1$ Mpc region down to $\lesssim0.1\,L^*$ luminosities at $z\leq0.1$ allows a plausible association between low-$z$ absorbers and individual galaxies. Ly$α$ covering fractions are computed to approximate the star-forming and passive galaxy populations using the spectral classes above. In agreement with previous results, the covering fraction of star-forming galaxies with $L\geq0.3\,L^*$ is consistent with unity inside one virial radius and declines slowly to $>50$% at 4 virial radii. On the other hand, passive galaxies have lower covering fractions ($\sim60$%) and a shallower decline with impact parameter, suggesting that their gaseous halos are patchy but have a larger scale-length than star-forming galaxies. All spectra obtained by this project are made available electronically for individual measurement and use.

astro-ph.GA↗