Peter Senchyna's research while affiliated with Carnegie Institution for Science and other places

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Publications (43)


Figure 2. Left: An example of PSF matching between the [O III] λ5007 PNB image from Keck/KCWI (top-left) and the [O III] 88 µm PNB image from Herschel/PACS (bottom-left). The KCWI PNB image has been convolved with a 2D Gaussian kernel (top-right) to match the PACS PNB image's PSF. The resulting residual is shown in the bottom-right panel. The red dashed circles indicate the apertures from which the 1D spectra were extracted. Right: Modeling of dust attenuation based on the observed flux ratios of hydrogen Balmer and Paschen lines. In the top panel, the data points represent the correction factors needed to align the observed flux ratios with those predicted by Case B recombination. The best-fit attenuation models are represented by solid curves, while the shaded areas denote their 1σ uncertainties. The blue (orange) color indicates the 1D spectra before (after) PSF matching. The steep slope at the lower wavelengths is primarily due to contributions from stellar absorption. The lower panel shows the fractional deviations between the observed and best-fit flux ratios, for the same data points. Data points near unity indicate a good agreement with the attenuation model.
Robust Nitrogen and Oxygen Abundances of Haro 3 from Optical and Infrared Emission
  • Preprint
  • File available

May 2024

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3 Reads

Yuguang Chen

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Tucker Jones

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[...]

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Accurate chemical compositions of star-forming regions are a critical diagnostic tool to characterize the star formation history and gas flows which regulate galaxy formation. However, the abundance discrepancy factor (ADF) between measurements from the "direct" optical electron temperature ($T_e$) method and from the recombination lines (RL) represents $\sim0.2$ dex systematic uncertainty in oxygen abundance. The degree of uncertainty for other elements is unknown. We conduct a comprehensive analysis of O$^{++}$ and N$^+$ ion abundances using optical and far-infrared spectra of a star-forming region within the nearby dwarf galaxy Haro 3, which exhibits a typical ADF. Assuming homogeneous conditions, the far-IR emission indicates an O abundance which is higher than the $T_e$ method and consistent with the RL value, as would be expected from temperature fluctuations, whereas the N abundance is too large to be explained by temperature fluctuations. Instead a component of highly obscured gas is likely required to explain the high far-IR to optical flux ratios. Accounting for this obscured component reduces both the IR-based metallicities and the inferred magnitude of temperature fluctuations, such that they cannot fully explain the ADF in Haro 3. Additionally, we find potential issues when predicting the RL fluxes from current atomic data. Our findings underscore the critical importance of resolving the cause of abundance discrepancies and understanding the biases between different metallicity methods. This work represents a promising methodology, and we identify further approaches to address the current dominant uncertainties.

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Figure 2. Comparison of GN-z11 (cross) and Mrk 996 (diamond) line ratios with predictions from photoionization models. (a) log 10 (N III] λ1750/O III] λ1664) vs. log 10 (N III] λ1750/Hδ). The circles show the predictions from photoionization models for star-forming galaxy models (blue), AGN models of Feltre et al. (2016) (purple), and radiative shock models of Alarie & Morisset (2019) (yellow), all assuming a nominal N/O vs. O/H relationship (see the text). (b) Same as diagram (a) but for log 10 (He II λ1640/Hδ) vs. log 10 (N III] λ1750/N IV] λ1485). (c) log 10 (N III] λ1750/O III] λ1664) vs. log 10 (N III] λ1750/Hδ). Star-forming galaxy models are shown for a metallicity log(Z/Z e ) = −0.94, ξ d = 0.3 for log(U) = −1, −2, and −3. The green lines show the increase of log 10 (N/O) from −1.8 to 0.7 and the fuchsia lines show the increase of hydrogen density from 10 2 to 10 6 cm −3 . The observed line ratios are in best agreement with photoionization by a metal-poor stellar ionizing spectrum, but regardless of the ionization source, they conclusively require a significant enhancement in N/O in the ionized gas.
Figure 3. Comparison of GN-z11 (cross) line ratios with predictions from photoionization models showing the effect of increasing depletion onto dust grains, parameterized by the dust-to-metal mass ratio ξ d . Star-forming galaxy models are shown for a metallicity log(Z/Z e ) = −0.94, log 10 (N/O) = −1.8 for log(U) = −1, −2, and −3. The blue lines show the increase of ξ d from 0.3 to 0.95. We highlight the effect of this change in ξ d for three sets of line ratios: (a) log 10 (N III] λ1750/O III] λ1664) vs. log 10 (N III] λ1750/Hδ); (b) log 10 ([Ne III] λ3868/[O II] λ3727) vs. log 10 (N IV] λ1485/N III] λ1750); and (c) log 10 (C III] λ1908/[Ne III] λ3868]) vs. log 10 (C III] λ1908/ N III] λ1750). Though increased depletion can boost the observed ratio of the N to O lines, even the most extreme models presented here (at 3 × ξ d,e ) cannot reproduce the full set of observed line ratios.
Figure 5. The HST/COS UV spectrum of the local blue compact dwarf galaxy Mrk 996 (Berg et al. 2022b) reveals N III] emission strikingly similar to that observed in GN-z11. For reference, we also include the median stack of the normalized spectra of the full CLASSY sample (Berg et al. 2022a, 2022b; James et al. 2022) in black. A similar N/O overabundance and high central electron density is inferred in Mrk 996, and attributed to the presence of an unusual concentration of W-R stars with N-rich winds. This demonstrates that similar spectral features can be powered by massive stars embedded in their own dense CNO-processed ejecta. The addition of N IV] emission and lack of strong W-R features in GN-z11 further suggests that though they appear to power comparable N III], GN-z11 may be powered by lower-metallicity massive star populations.
Figure B1. Comparison of observed and modeled emission-line fluxes. The black diamonds represent the data and the red diamonds are the fluxes predicted with BEAGLE for the best-fit model.
Figure B2. Selected photoionization models compared to line ratios of GN-z11 (cross) and Mrk 996 (diamond), highlighting line ratios with [O II] and C III]. In the left panel, we compare the same set of starting models as in Figure 2 panel (c) in log 10 ([O II] λ3727/[Ne III] λ3868) vs. log 10 ([O II λ3727/H δ), and show the impact of increasing n H from 10 2 to 10 6 cm −3 . This increase in density suppresses [O II] strongly due to the low critical densities of the upper states of this doublet, suggesting that some of the gas emission we observe is from a lower-density phase. In the right panel, we compare the same grids of photoionization models as in Figure 2 panels (a) and (b) in log 10 (N III] λ1750/O III] λ1664) vs. log 10 (N III] λ1750/ C III] λ1908). None of the ionizing sources considered can match either ratio with N III], further suggesting an enhancement in N over both O and C is present.
GN-z11 in Context: Possible Signatures of Globular Cluster Precursors at Redshift 10

April 2024

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12 Reads

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1 Citation

The Astrophysical Journal

The first JWST spectroscopy of the luminous galaxy GN-z11 simultaneously established its redshift at z = 10.6 and revealed a rest-ultraviolet spectrum dominated by signatures of highly ionized nitrogen, which has so far defied clear interpretation. We present a reappraisal of this spectrum in the context of both detailed nebular modeling and nearby metal-poor reference galaxies. The N iv ] emission enables the first nebular density measurement in an apparently predominantly star-forming galaxy at z > 10, revealing evidence for extremely high densities n e ≳ 10 ⁵ cm ⁻³ . With a suite of photoionization models, we establish that regardless of the ionization mechanism and accounting for depletion and this density enhancement, gas substantially enriched in nitrogen ([N/O] = +0.52 assuming the nebular emission is dominated by star formation) is required to reproduce the observed lines. We compare the GN-z11 spectrum to local UV databases and highlight a unique nearby galaxy, Mrk 996, where a high concentration of Wolf–Rayet stars and their CNO-processed ejecta produce a UV spectrum remarkably similar in some respects to that of GN-z11 and the Sunburst Arc. Collating this evidence in the context of Galactic stellar abundances, we suggest that the peculiar nitrogenic features prominent in GN-z11 may be a unique signature of intense and densely clustered star formation in the evolutionary chain of the present-day globular clusters, consistent with in situ early enrichment with nuclear-processed stellar ejecta on a massive scale. Combined with insight from local galaxies, these and future JWST data open a powerful new window into the physical conditions of star formation and chemical enrichment at the highest redshifts.


Metal-poor star formation at z > 6 with JWST : New insight into hard radiation fields and nitrogen enrichment on 20 pc scales

March 2024

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10 Reads

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7 Citations

Monthly Notices of the Royal Astronomical Society

Nearly a decade ago, we began to see indications that reionization-era galaxies power hard radiation fields rarely seen at lower redshift. Most striking were detections of nebular CIV emission in what appeared to be typical low mass galaxies, requiring an ample supply of 48 eV photons to triply ionize carbon. We have obtained deep JWST/NIRSpec R=1000 spectroscopy of the two z>6 CIV-emitting galaxies known prior to JWST. Here we present a rest-UV to optical spectrum of one of these two systems, the multiply-imaged z = 6.1 lensed galaxy RXCJ2248-ID. NIRCam imaging reveals two compact (<22pc) clumps separated by 220pc, with one comprising a dense concentration of massive stars (>10, 400M⊙/yr/kpc2) formed in a recent burst. We stack spectra of 3 images of the galaxy (J=24.8–25.9), yielding a very deep spectrum providing a high S/N template of strong emission line sources at z > 6. The spectrum reveals narrow high ionization lines (HeII, CIV, NIV]) with line ratios consistent with powering by massive stars. The rest-optical spectrum is dominated by very strong emission lines ([OIII] EW=2800Å), albeit with weak emission from low-ionization transitions ([OIII]/[OII]=184). The electron density is found to be very high (6.4 − 31.0 × 104cm−3) based on three UV transitions. The ionized gas is metal poor ($12+\log (\rm O/H)=7.43^{+0.17}_{-0.09}$), yet highly enriched in nitrogen ($\log (\rm N/O)=-0.39^{+0.11}_{-0.10}$). The spectrum appears broadly similar to that of GNz11 at z = 10.6, without showing the same AGN signatures. We suggest that the hard radiation field and rapid nitrogen enrichment may be a short-lived phase that many z > 6 galaxies go through as they undergo strong bursts of star formation. We comment on the potential link of such spectra to globular cluster formation.


CLASSY. VIII. Exploring the Source of Ionization with UV Interstellar Medium Diagnostics in Local High-z Analogs*

February 2024

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19 Reads

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3 Citations

The Astrophysical Journal

In the current JWST era, rest-frame UV spectra play a crucial role in enhancing our understanding of the interstellar medium (ISM) and stellar properties of the first galaxies in the epoch of reionization ( z > 6). Here, we compare well-known and reliable optical diagrams sensitive to the main ionization source (i.e., star formation, SF; active galactic nuclei, AGN; and shocks) to UV counterparts proposed in the literature—the so-called “UV–BPT diagrams”—using the HST COS Legacy Archive Spectroscopic SurveY (CLASSY), which is the largest high-quality, high-resolution, and broad-wavelength range atlas of far-UV spectra for 45 local star-forming galaxies. In particular, we explore where CLASSY UV line ratios are located in the different UV diagnostic plots, taking into account state-of-the-art photoionization and shock models, and, for the first time, the measured ISM and stellar properties (e.g., gas-phase metallicity, ionization parameter, carbon abundance, and stellar age). We find that the combination of C iii ] λ λ 1907,9 He ii λ 1640 and O iii ] λ 1666 can be a powerful tool to separate between SF, shocks, and AGN at subsolar metallicities. We also confirm that alternative diagrams without O iii ] λ 1666 still allow us to define an SF-locus, with some caveats. Diagrams including C iv λ λ 1548,51 should be taken with caution given the complexity of this doublet profile. Finally, we present a discussion detailing the ISM conditions required to detect UV emission lines, visible only in low gas-phase metallicity (12 + log(O/H) ≲ 8.3) and high ionization parameter (log( U ) ≳ −2.5) environments. Overall, CLASSY and our UV toolkit will be crucial in interpreting the spectra of the earliest galaxies that JWST is currently revealing.



CLASSY VII Lyα Profiles: The Structure and Kinematics of Neutral Gas and Implications for LyC Escape in Reionization-era Analogs*

October 2023

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29 Reads

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5 Citations

The Astrophysical Journal

Ly α line profiles are a powerful probe of interstellar medium (ISM) structure, outflow speed, and Lyman-continuum escape fraction. In this paper, we present the Ly α line profiles of the Cosmic Origins Spectrograph (COS) Legacy Archive Spectroscopic SurveY, a sample rich in spectroscopic analogs of reionization-era galaxies. A large fraction of the spectra show a complex profile, consisting of a double-peaked Ly α emission profile in the bottom of a damped, Ly α absorption trough. Such profiles reveal an inhomogeneous ISM. We successfully fit the damped Ly α absorption and the Ly α emission profiles separately, but with complementary covering factors, a surprising result because this approach requires no Ly α exchange between high- N H i and low- N H i paths. The combined distribution of column densities is qualitatively similar to the bimodal distributions observed in numerical simulations. We find an inverse relation between Ly α peak separation and the [O iii ]/[O ii ] flux ratio, confirming that the covering fraction of Lyman-continuum-thin sightlines increases as the Ly α peak separation decreases. We combine measurements of Ly α peak separation and Ly α red peak asymmetry in a diagnostic diagram, which identifies six Lyman-continuum leakers in the COS Legacy Archive Spectrocopy SurveY (CLASSY) sample. We find a strong correlation between the Ly α trough velocity and the outflow velocity measured from interstellar absorption lines. We argue that greater vignetting of the blueshifted Ly α peak, relative to the redshifted peak, is the source of the well-known discrepancy between shell-model parameters and directly measured outflow properties. The CLASSY sample illustrates how scattering of Ly α photons outside the spectroscopic aperture reshapes Ly α profiles because the distances to these compact starbursts span a large range.


JWST /NIRSpec spectroscopy of z = 7–9 star-forming galaxies with CEERS: new insight into bright Lyα emitters in ionized bubbles

September 2023

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12 Reads

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43 Citations

Monthly Notices of the Royal Astronomical Society

We describe new JWST/NIRSpec observations of galaxies at z ≳ 7 taken from the CEERS survey. Previous observations of this area have revealed associations of Lyα emitters at redshifts (z = 7.5, 7.7, 8.7) where the intergalactic medium (IGM) is thought to be mostly neutral, leading to suggestions that these systems are situated in large ionized bubbles. We identify 21 z ≳ 7 galaxies with robust redshifts in the CEERS dataset, including 10 in the Lyα associations. Their spectra are indicative of very highly ionized and metal poor gas, with line ratios (O32 =17.84 and Ne3O2 =0.89, linear scale) and metallicity ($12+\log {(\rm {O/H})}=7.84$) that are rarely seen at lower redshifts. We find that the most extreme spectral properties are found in the six z ≳ 7 Lyα emitters in the sample. Each has a hard ionizing spectrum indicating that their visibility is likely enhanced by efficient ionizing photon production. Lyα velocity offsets are found to be very large (≳ 300 km s−1), likely also contributing to their detectability. We find that Lyα in z ≳ 7 galaxies is 6 − 12 × weaker than in lower redshift samples with matched rest-optical spectral properties. If the bubbles around the Lyα emitters are relatively small (≲ 0.5 − 1 pMpc), we may expect such significant attenuation of Lyα in these ionized regions. We discuss several other effects that may contribute to weaker Lyα emission at z ≳ 7. Deep spectroscopy of fainter galaxies in the vicinity of the Lyα emitters will better characterize the physical scale of the ionized bubbles in this field.


CLASSY VII Ly\alpha\ Profiles: The Structure and Kinematics of Neutral Gas and Implications for LyC Escape in Reionization-Era Analogs

July 2023

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13 Reads

Lyman-alpha line profiles are a powerful probe of ISM structure, outflow speed, and Lyman continuum escape fraction. In this paper, we present the Ly$\alpha$ line profiles of the COS Legacy Archive Spectroscopic SurveY, a sample rich in spectroscopic analogs of reionization-era galaxies. A large fraction of the spectra show a complex profile, consisting of a double-peaked Ly$\alpha$ emission profile in the bottom of a damped, Ly$\alpha$ absorption trough. Such profiles reveal an inhomogeneous interstellar medium (ISM). We successfully fit the damped Ly$\alpha$ absorption (DLA) and the Ly$\alpha$ emission profiles separately, but with complementary covering factors, a surprising result because this approach requires no Ly$\alpha$ exchange between high-$N_\mathrm{HI}$ and low-$N_\mathrm{HI}$ paths. The combined distribution of column densities is qualitatively similar to the bimodal distributions observed in numerical simulations. We find an inverse relation between Ly$\alpha$ peak separation and the [O III]/[O II] flux ratio, confirming that the covering fraction of Lyman-continuum-thin sightlines increases as the Ly$\alpha$ peak separation decreases. We combine measurements of Ly$\alpha$ peak separation and Ly$\alpha$ red peak asymmetry in a diagnostic diagram which identifies six Lyman continuum leakers in the CLASSY sample. We find a strong correlation between the Ly$\alpha$ trough velocity and the outflow velocity measured from interstellar absorption lines. We argue that greater vignetting of the blueshifted Ly$\alpha$ peak, relative to the redshifted peak, is the source of the well-known discrepancy between shell-model parameters and directly measured outflow properties. The CLASSY sample illustrates how scattering of Ly$\alpha$ photons outside the spectroscopic aperture reshapes Ly$\alpha$ profiles as the distances to these compact starbursts span a large range.


Catching a nova X-ray/UV flash in the visible? Early spectroscopy of the very slow Nova Velorum 2022 (Gaia22alz)

June 2023

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14 Reads

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4 Citations

Monthly Notices of the Royal Astronomical Society

We present early spectral observations of the very slow Galactic nova Gaia22alz, over its gradual rise to peak brightness that lasted 180 d. During the first 50 d, when the nova was only 3–4 mag above its normal brightness, the spectra showed narrow (FWHM ≈ 400 km s−1) emission lines of H Balmer, He i, He ii, and C iv but no P Cygni absorption. A few weeks later, the high-excitation He ii and C iv lines disappeared, and P Cygni profiles of Balmer, He i, and eventually Fe ii lines emerged, yielding a spectrum typical of classical novae before peak. We propose that the early (first 50 d) spectra of Gaia22alz, particularly the emission lines with no P Cygni profiles, are produced in the white dwarf’s optically thin envelope or accretion disc, reprocessing ultraviolet and potentially X-ray emission from the white dwarf after a dramatic increase in the rate of thermonuclear reactions, during a phase known as the ‘early X-ray/UV flash’. If true, this would be one of the rare times that the optical signature of the early X-ray/UV flash has been detected. While this phase might last only a few hours in other novae and thus be easily missed, it was possible to detect in Gaia22alz due to its very slow and gradual rise and thanks to the efficiency of new all-sky surveys in detecting transients on their rise. We also consider alternative scenarios that could explain the early spectral features of Gaia22alz and its gradual rise.


Figure 2. [N II] (top left), [S II] (top right), and [O I] (bottom) BPT diagrams for the narrow and broad components, shown as red dots and blue diamonds, respectively. All the measurements have S/N > 3 for all the lines involved. The black dotted curve is the empirical relation to divide pure star-forming from Seyfert-H II composite objects by Kauffmann et al. (2003), while the black solid curves are the maximum starburst line derived by Kewley et al. (2001). The black dashed lines are the Kewley et al. (2006) boundary between Seyferts and low-ionization (nuclear) emission-line regions (LI(N)ERs; see also Heckman 1980; Belfiore et al. 2016). Histograms showing the distribution of [N II]/Hα, [S II]/Hα, [O I]/Hα, and [O III]/Hβ line ratios in the narrow and broad components are shown in red and blue, respectively, on each axis, with median values shown by the dashed and dotted black lines. The broad component clearly shows higher x-axis line ratios. The green-shaded regions represent the maximal starburst predictions at metallicity between 10% Z⊙ and 50% Z⊙ values, using pure stellar photoionization including massive star binaries through the BPASS stellar evolution models (Xiao et al. 2018), to show to what extent the maximal starburst line can change in the metallicity range in which we observe UV emission lines. The galaxies with at least one UV emission line (i.e., C III] λλ1907,9) are highlighted by a black thick edge.
CLASSY VIII: Exploring the Source of Ionization with UV ISM diagnostics in local High-$z$ Analogs

June 2023

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28 Reads

In the current JWST era, rest-frame UV spectra play a crucial role in enhancing our understanding of the interstellar medium (ISM) and stellar properties of the first galaxies in the epoch of reionization (EoR, $z>6$). Here, we compare well-known and reliable optical diagrams sensitive to the main ionization source (i.e., star formation, SF; active galactic nuclei, AGN; shocks) to UV counterparts proposed in the literature - the so-called ``UV-BPT diagrams'' - using the HST COS Legacy Archive Spectroscopic SurveY (CLASSY), the largest high-quality, high-resolution and broad-wavelength range atlas of far-UV spectra for 45 local star-forming galaxies. In particular, we explore where CLASSY UV line ratios are located in the different UV diagnostic plots, taking into account state-of-the-art photoionization and shock models and, for the first time, the measured ISM and stellar properties (e.g., gas-phase metallicity, ionization parameter, carbon abundance, stellar age). We find that the combination of C III] $\lambda\lambda$1907,9 He II $\lambda1640$ and O III] $\lambda$1666 can be a powerful tool to separate between SF, shocks and AGN at sub-solar metallicities. We also confirm that alternative diagrams without O III] $\lambda$1666 still allow us to define a SF-locus with some caveats. Diagrams including C IV $\lambda\lambda$1548,51 should be taken with caution given the complexity of this doublet profile. Finally, we present a discussion detailing the ISM conditions required to detect UV emission lines, visible only in low gas-phase metallicity (12+log(O/H) $\lesssim8.3$) and high ionization parameter (log($U$) $\gtrsim-2.5$) environments. Overall, CLASSY and our UV toolkit will be crucial in interpreting the spectra of the earliest galaxies that JWST is currently revealing.


Citations (22)


... Some works have suggested that GN-z11 may host a population of WR stars 24 . The HeIIλ1640 line shows a potentially broad profile, as shown in Extended Data Fig. 1b (although the wings are mostly in the noise). ...

Reference:

A small and vigorous black hole in the early Universe
GN-z11 in Context: Possible Signatures of Globular Cluster Precursors at Redshift 10

The Astrophysical Journal

... Notably, the large N/O abundances found in early galaxies are based on rest-frame ultravio-let emission lines, as opposed to optical diagnostics used at lower redshifts (z ≲ 3). Such diagnostics are powerful and complementary in probing a vast redshift range, but may introduce different systematic errors (e.g., Topping et al. 2024). This underscores the necessity to accurately determine the chemical abundance patterns in galaxies to better understand their chemical evolution throughout cosmic history. ...

Metal-poor star formation at z > 6 with JWST : New insight into hard radiation fields and nitrogen enrichment on 20 pc scales
  • Citing Article
  • March 2024

Monthly Notices of the Royal Astronomical Society

... This diagnostic identifies 20 sources as AGN that we exclude from the analysis because the abundance methods are calibrated for stellar-ionized gas. In addition, we take advantage of the rest-frame UV coverage at higher redshifts to select sources where the He II λ1640, C III] λ1907, 1909, and O III] λ1666 emission lines are detected at S/N 4 to construct the C3He2-O3He2 ionization diagram discussed in Mingozzi et al. (2024) and Feltre et al. (2016). There are 11 sources meeting these criteria, and all are consistent with star-forming galaxies. ...

CLASSY. VIII. Exploring the Source of Ionization with UV Interstellar Medium Diagnostics in Local High-z Analogs*

The Astrophysical Journal

... Finally, the Lyα λ1216 emission line is often asymmetric, displaying a strong wing at longer wavelengths, due to radiative transfer effects (Verhamme et al. 2006;Dijkstra et al. 2007;Laursen 2010;Childs & Stanway 2018;Hu et al. 2023). We adopt a simple approach (Hu et al. 2010) for the continuum-detected Lyα emitters and fit a truncated half-Gaussian with the same centroid as the main Gaussian component to account for this wing emission. ...

CLASSY VII Lyα Profiles: The Structure and Kinematics of Neutral Gas and Implications for LyC Escape in Reionization-era Analogs*

The Astrophysical Journal

... Its preeminent power has been confirmed by a multitude of achievements in searching high-z galaxies within its first year in service. Yet most of the current research about LAEs focuses on higher redshifts (e.g., Ning et al. 2023 at z ;6;Tang et al. 2023 at z = 7-9; Jung et al. 2023 at z ∼ 8;Whitler et al. 2023 at z ∼ 9;Tang et al. 2023 at z = 7-9). These works investigate the Lyα escape process in the reionization era, while paying relatively less attention to the intrinsic properties of the galaxies themselves. ...

JWST /NIRSpec spectroscopy of z = 7–9 star-forming galaxies with CEERS: new insight into bright Lyα emitters in ionized bubbles
  • Citing Article
  • September 2023

Monthly Notices of the Royal Astronomical Society

... The simulation for the 0.6 M e WD evolves so slowly, however, that it takes almost 8000 s for the temperature to reach its peak and the decline is even slower. In fact, the evolution of the TNR on this low-mass WD is so slow that it rules out this WD mass for all but the slowest CNe (either CO or ONe) such as Nova Velorum 2022 (Aydi et al. 2023). ...

Catching a nova X-ray/UV flash in the visible? Early spectroscopy of the very slow Nova Velorum 2022 (Gaia22alz)

Monthly Notices of the Royal Astronomical Society

... NGDEEP-NRC will also allow for the characterization of the detailed morphological substructure of faint disks, streams, and other low surface brightness features. The deep imaging will enable the detection of galaxies in the process of merging, as well as post-mergers through the identification of shells, tidal tails, double nuclei, and other surrounding debris (e.g., Mantha et al. 2019;Hsiao & Coe 2023;Kokorev et al. 2023). NGDEEP-NRC imaging will also push spatially resolved SED fitting to z > 4, probing inside-out quenching and the formation of early bulges, by allowing reconstruction of the radial profiles of SFR, stellar mass surface density, and specific SFR of galaxies (e.g., Abdurro'uf et al. 2023). ...

JWST Reveals a Possible z ∼ 11 Galaxy Merger in Triply Lensed MACS0647–JD

The Astrophysical Journal Letters

... A key open question is whether temperature fluctuations in ionized nebulae are in fact sufficiently high to explain the ADF (e.g., Peimbert et al. 2017;Maiolino & Mannucci 2019). In a pilot study by Chen et al. (2023) (hereafter C23), the temperature fluctuation hypothesis was empirically tested within the nearby dwarf galaxy Mrk 71 using far-IR fine-structure emission lines. While these far-IR emission lines (e.g., [O III] λλ52, 88 µm) are the product of collisional excitation, the low energy required for their excitation renders them effectively insensitive to T e . ...

Accurate oxygen abundance of interstellar gas in Mrk 71 from optical and infrared spectra

Nature Astronomy

... only slightly below the gas-phase metallicity, suggesting a slow chemical enrichment in Leo A, in agreement with the flat age-metallicity relation derived from Hubble Space Telescope (HST) photometry by Cole et al. (2007). More recently, Gull et al. (2022) derived stellar parameters for a sample of massive stars (late O/early B main-sequence objects) ...

A Panchromatic Study of Massive Stars in the Extremely Metal-poor Local Group Dwarf Galaxy Leo A*

The Astrophysical Journal

... We then move from the bottom to the top of the trace (this direction corresponds to the SW to the NE direction in Figure 2) and define two regions along the trace. We divide the two regions at the Nakajima+2018, binary Nakajima+2018, single Berg+2018, z 1.8 Erb+2010, z 2 Stark+2017, z = 7.73 Nakajima+2018, z 3 Mainali+2020, z 2 L11, local Stark+2014, z 2 Mingozzi+2022, local Rigby+2015, local Senchyna+2019, local Senchyna+2017, local Bayliss+2014, z 3.6 J0332 Mingozzi et al. (2022), while colored markers indicates galaxies at redshift 1.8 < < 2 (Berg et al. 2018, Stark et al. 2014, Rigby et al. 2015, Mainali et al. 2020), 3 < < 3.6 (Bayliss et al. 2014, Nakajima et al. 2018), ∼ 7.73 ). The curves are photionization models computed by Nakajima et al. (2018) using BPASS models with (green solid) and without (orange dashed) binary stars. ...

CLASSY IV. Exploring UV Diagnostics of the Interstellar Medium in Local High-z Analogs at the Dawn of the JWST Era*

The Astrophysical Journal