<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Research Themes | Ray Garner</title><link>https://astronoraygarner.com/projects/</link><atom:link href="https://astronoraygarner.com/projects/index.xml" rel="self" type="application/rss+xml"/><description>Research Themes</description><generator>HugoBlox Kit (https://hugoblox.com)</generator><language>en-us</language><lastBuildDate>Sun, 19 May 2024 00:00:00 +0000</lastBuildDate><image><url>https://astronoraygarner.com/media/icon_hu_eee4a95885829ab2.png</url><title>Research Themes</title><link>https://astronoraygarner.com/projects/</link></image><item><title>Extreme Nebular Conditions in the Early Universe with JWST</title><link>https://astronoraygarner.com/projects/high_redshift/</link><pubDate>Fri, 09 Oct 2026 00:00:00 +0000</pubDate><guid>https://astronoraygarner.com/projects/high_redshift/</guid><description>&lt;p&gt;The first galaxies observed by the James Webb Space Telescope (JWST) do not look like simple younger versions of galaxies in the nearby Universe. Their nebular spectra indicate extremely high ionization, low chemical abundances, dense gas, and very young stellar populations. In some galaxies, the spectra also contain emission that conventional stellar populations can&amp;rsquo;t produce at all.&lt;/p&gt;
&lt;p&gt;These observations create exactly the kind of problem that motivates much of my research: &lt;em&gt;When the physical conditions change dramatically, can we still interpret familiar emission-line diagnostics in the same way?&lt;/em&gt;&lt;/p&gt;
&lt;p&gt;I have begun exploring that question at Cosmic Dawn as a member of the &lt;strong&gt;Carbon-3 Plus Oxygen (C3PO)&lt;/strong&gt; collaboration&lt;sup id="fnref:1"&gt;&lt;a href="#fn:1" class="footnote-ref" role="doc-noteref"&gt;1&lt;/a&gt;&lt;/sup&gt;. C3PO uses deep JWST/NIRSpec spectroscopy to measure both the rest-frame ultraviolet and optical spectra of galaxies during the Epoch of Reionization, roughly 6 &amp;lt; z &amp;lt; 9.&lt;/p&gt;
&lt;p&gt;This is a powerful combination of lines. The optical spectrum contains familiar diagnostics such as the Balmer lines, [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;], [O &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt;], and the temperature-sensitive [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;] auroral line. The ultraviolet adds transitions from oxygen, silicon, nitrogen, carbon, and helium that probe different ionization zones, densities, abundances, and the shape of the ionizing radiation spectrum. Together, they allow us to investigate the physical properties of these extreme galaxies.&lt;/p&gt;
&lt;h2 id="measuring-properties-at-cosmic-dawn"&gt;Measuring Properties at Cosmic Dawn&lt;/h2&gt;
&lt;p&gt;The motivation for C3PO is straightforward: the strongest emission lines already tell us that galaxies near the Epoch of Reionization are unusual, but the weaker lines tell us why.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/high_redshift/13264_statement.png"
alt="A scientific plot showing a spectrum. The spectrum gently slopes down from left to right with jagged variations except for a few particularly strong emission lines that are annotated."&gt;&lt;figcaption&gt;
&lt;p&gt;The rest-frame UV spectrum of a redshift ∼ 7 galaxy observed in C3PO. Strong emission lines are marked, including peculiarly strong He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt;. The red line is a BPASS fit to the underlying stellar continuum.&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;Deep NIRSpec spectroscopy gives access to a huge set of physical diagnostics. In the optical, the auroral-to-nebular [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;] ratio provides a measurement of the electron temperature, which can be used with other oxygen lines to estimate the gas-phase abundance without relying on strong-line calibrations (which are increasingly uncertain at high redshift!). Density-sensitive doublets probe the structure of the gas. The [O &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt;] doublet traces relatively low-ionization material, while the C &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;] doublet probes gas at higher ionization.&lt;/p&gt;
&lt;p&gt;In the rest-frame UV, C &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;], O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;], C &lt;span style='font-size: 0.8em;'&gt;IV&lt;/span&gt;, He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt;, and other lines add constraints on carbon abundance, and thus the C/O ratio, stellar populations, and the hardness of the ionizing radiation responsible for these emission lines.&lt;/p&gt;
&lt;p&gt;This is a natural extension of my research in the nearby universe. Locally, I use spatially resolution to test the assumptions behind nebular diagnostics. At high redshift, I cannot resolve individual H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions, but I can instead use a much richer set of emission lines to constrain the physics directly.&lt;/p&gt;
&lt;h2 id="the-heii-problem"&gt;The He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; Problem&lt;/h2&gt;
&lt;p&gt;My primary C3PO project focuses on a subset of galaxies with unusually strong He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; λ1640 emission.&lt;/p&gt;
&lt;p&gt;Producing He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; requires photons energetic enough to ionize He&lt;sup&gt;+&lt;/sup&gt;, above about 54 eV. Standard stellar populations produce relatively few photons at these energies, particularly compared with what is required by several galaxies in the C3PO sample (and others observed by other programs).&lt;/p&gt;
&lt;p&gt;Possible explanations include unusual stellar populations, very massive stars, accreting black holes, x-ray binaries, shocks, or combinations of several of these. The challenge is that many different ionizing spectra can be adjusted to reproduce a single He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; measurement. Therefore, I am combining measurements from the full NIRSpec spectra with photoionization modeling to address that problem.&lt;/p&gt;
&lt;p&gt;The He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; line is interesting not only because of its strength, but also because of its kinematics. In the galaxies I am studying, the line widths are not simply identical to either neighboring narrow nebular lines or in the extremely broad stellar-wind features expected from some very-massive star models. That raises the possibility that the highly ionized helium originates in ia physically or dynamically distinct component of the galaxy.&lt;/p&gt;
&lt;p&gt;The existing spectra already constrain many of the quantities needed to interpret these sources: electron temperature, electron density, chemical abundance, C/O ratio, and the lower-energy ionizing spectrum. The remaining challenge is determining which physical source produces the photons at the extreme high-energy end.&lt;/p&gt;
&lt;p&gt;This project has already motivated me to develop and submit my first JWST observing program, designed as a direct observational follow-up to the questions raised by these C3PO spectra.&lt;/p&gt;
&lt;h2 id="building-models-for-galaxies"&gt;Building Models for Galaxies&lt;/h2&gt;
&lt;p&gt;Interpreting these spectra also requires reconsidering the model grids themselves. A photoionization model can only return physically meaningful answers if the range of conditions explored by the model actually includes the galaxy being observed. That sounds obvious, but JWST is increasingly finding galaxies outside the standard parameter space that was constructed from local Universe systems.&lt;/p&gt;
&lt;p&gt;I have been working with graduate student Annabella Yang on her first paper measuring C/O abundance ratios in C3PO galaxies. In particular, these observations motivate extending the models toward low, sub-solar C/O abundance ratios and higher gas densities than are often assumed in standard model grids.&lt;/p&gt;
&lt;p&gt;This is important because carbon and oxygen are produced on different stellar timescales and through different pathways. Their ratio therefore constrains information about how rapidly a galaxy has enriched, the populations of stars responsible for that enrichment, and potentially the very short star formation histories of galaxies observed only a few hundred million years after the Big Bang.&lt;/p&gt;
&lt;h2 id="when-familiar-agn-diagnostics-stop-working"&gt;When Familiar AGN Diagnostics Stop Working&lt;/h2&gt;
&lt;p&gt;My beginnings in the high-redshift universe actually began before my current C3PO project. I am a co-author on Cleri et al. (2025), which explored whether familiar optical emission line diagnostics can still distinguish stellar populations from accreting black holes under the physical conditions seen at high redshift.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/high_redshift/cleri.png"
alt="A three-by-three panel scientific plot. Gold circles and green crosses overlap in various portions of each panel."&gt;&lt;figcaption&gt;
&lt;p&gt;A characteristic optical diagnostic diagram. Models for stellar populations are gold circles, while those for accreting black holes are blue crosses. Each panel shows a particular cross section of metallicity and ionization parameter. At nearly every combination, black holes and stellar populations overlap in the diagnostic space. Figure 8 of Cleri et al. (2025).&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;Unfortunately, at high ionization parameter and low metallicity, the model predictions for stellar populations and accreting black holes overlap substantially in standard diagnostic diagrams. The line ratios become more sensitive to the gas metallicity and ionization parameter than to the identity of the ionizing source itself.&lt;/p&gt;
&lt;p&gt;This means that placing a galaxy on a familiar BPT diagram does not necessarily answer whether stars or black hole accretion dominate the ionizing radiation. Diagnostics based largely on photons below the He&lt;sup&gt;+&lt;/sup&gt; ionization edge may simply not probe the part of the spectrum where the competeing ionizing sources differ most strongly.&lt;/p&gt;
&lt;h2 id="little-red-dots"&gt;Little Red Dots&lt;/h2&gt;
&lt;p&gt;I have also contributed to C3PO work led by Casey Papovich studying two Little Red Dots in our sample. These sources truly illustrate how unfamiliar the nebular conditions of early galaxies can be.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/high_redshift/papovich.png"
alt="A scientific plot showing a spectrum. The spectrum gently slopes down from left to right with jagged variations except for a few particularly strong emission lines that are annotated."&gt;&lt;figcaption&gt;
&lt;p&gt;The rest-frame optical spectrum of a galaxy at a redshift of 8.35. Important emission lines are indicated. Note the broad [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;] λ4363 and Hβ emission. Figure 2 from Papovich et al. (2026).&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;Their spectra contain broad Balmer emission and broad auroral [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;] emission, while several of the stronger forbidden metal lines remain narrow. The inferred densities differ dramatically between these components, suggesting that the emitting gas is strongly stratified rather than described by a single set of physical conditions.&lt;/p&gt;
&lt;p&gt;These objects are not the central focus of my own research, but participating in this project broadened my experience with the range of physical conditions present in the C3PO dataset and the high-redshift universe more broadly.&lt;/p&gt;
&lt;h2 id="the-broad-picture"&gt;The Broad Picture&lt;/h2&gt;
&lt;p&gt;At first glance, an H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region a few hundred parsecs across in a nearby spiral galaxy and an unresolved galaxy at the Epoch of Reionization seem like very different research problems.&lt;/p&gt;
&lt;p&gt;However, they&amp;rsquo;re really the same problem at different scales. In nearby galaxies, spatial resolution lets me see that emission line ratios depend on geometry, stellar populations, feedback, and where within an H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region they are measured. At high redshift, those structures are compressed into a single spectrum. At the same time, the physical conditions themselves can be very different from those on which many familiar calibrations were built. The question becomes &lt;em&gt;Which lessons from the nearby Universe remain valid when the nebula is unresolved and the physical regime itself has changed?&lt;/em&gt; C3PO gives me the chance to test that directly.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 id="methods-and-expertise"&gt;Methods and Expertise&lt;/h2&gt;
&lt;p&gt;My high-redshift work has expanded my experience across both observational spectroscopy and physical modeling.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;JWST spectroscopy&lt;/strong&gt;
NIRSpec spectroscopy · rest-frame UV and optical emission lines · line profile fitting · weak-line measurements&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Nebular conditions&lt;/strong&gt;
Electron temperatures · electron densities · direct-method oxygen abundance · multi-zone structure&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Ionizing sources&lt;/strong&gt;
Hard ionizing spectra · stellar populations · very massive stars · AGN&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Photoionization modeling&lt;/strong&gt;
Cloudy · BPASS · Bayesian model comparison&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Research development&lt;/strong&gt;
JWST proposals · mentoring · collaborations&lt;/p&gt;
&lt;hr&gt;
&lt;h2 id="selected-publications"&gt;Selected Publications&lt;/h2&gt;
&lt;h3 id="first-author-work"&gt;First Author Work&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; Emitters in C3PO - in preparation&lt;/strong&gt;: &lt;br&gt; Analyzing galaxies with strong He &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; λ1640 emission that can&amp;rsquo;t be reproduced by standard stellar populations.&lt;/p&gt;
&lt;h3 id="collaborative-work"&gt;Collaborative Work&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Yang et al. - in preparation&lt;/strong&gt;: C/O abundances in Epoch of Reionization galaxies.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Olivier et al. - in preparation&lt;/strong&gt;: Spatially resolved direct-method abundances in a strongly lensed galaxy.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Papovich et al. (2026)&lt;/strong&gt;:
&lt;br&gt; Deep NIRSpec spectroscopy reveals strongly stratified gas conditions and evidence for an additional ionizing source in two compact systems.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Cleri et al. (2025)&lt;/strong&gt;:
&lt;br&gt; Photoionization models demonstrate that familiar rest-optical diagnostics become degenerate under the extreme physical conditions common at high redshift.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 id="where-this-work-is-going"&gt;Where This Work Is Going&lt;/h2&gt;
&lt;p&gt;JWST is showing us galaxies with densities, abundance patterns, ionization states, and ionizing spectra that frequently sits at the edges of the models we have traditionally used to interpret nebular emission. Simply extending familiar calibration curves to higher redshift is therefore not enough.&lt;/p&gt;
&lt;p&gt;In nearby galaxies, I can resolve the physics. At the Epoch of Reionization, I have only the integrated spectrum, but JWST gives me enough diagnostic lines to interpret that spectrum in unprecedented detail. Together, those regimes let me explore what physical information is encoded in a nebular spectrum, and how do we recover it when the Universe no longer resembles the systems on which our assumptions were built?&lt;/p&gt;
&lt;div class="footnotes" role="doc-endnotes"&gt;
&lt;hr&gt;
&lt;ol&gt;
&lt;li id="fn:1"&gt;
&lt;p&gt;As a huge Star Wars fan, it gives me endless happiness that they named the collaboration this way.&amp;#160;&lt;a href="#fnref:1" class="footnote-backref" role="doc-backlink"&gt;&amp;#x21a9;&amp;#xfe0e;&lt;/a&gt;&lt;/p&gt;
&lt;/li&gt;
&lt;/ol&gt;
&lt;/div&gt;</description></item><item><title>Resolved HII Regions with SIGNALS</title><link>https://astronoraygarner.com/projects/signals/</link><pubDate>Thu, 08 Oct 2026 00:00:00 +0000</pubDate><guid>https://astronoraygarner.com/projects/signals/</guid><description>&lt;p&gt;Nebular emission lines are some of our most powerful tools for studying galaxies. From a handful of bright lines, we routinely estimate properties of star-forming regions (and whole galaxies) such as chemical abundances, ionization parameters, densities, temperatures, dust extinctions, and the source of ionizing radiation. But every one of those estimations depends on assumptions.&lt;/p&gt;
&lt;p&gt;We often assume a geometry for the ionized gas, a relationship between the gas and its ionizing stars, a chemical abundance pattern, or that a spectrum integrated over an H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region adequately represents everything inside it. Those assumptions become especially important when the same diagnostics are applied to galaxies too distant to resolve.&lt;/p&gt;
&lt;p&gt;My work with the &lt;strong&gt;Star-formation, Ionized Gas, and Nebular Abundances Legacy Survey (SIGNALS)&lt;/strong&gt; attempts to answer the question: &lt;em&gt;What physical information do these lines provide, and when do our assumptions about these diagnostics break down?&lt;/em&gt;&lt;/p&gt;
&lt;p&gt;SIGNALS uses an instrument called SITELLE, a wide-field imaging Fourier transform spectrometer at the Canada-France-Hawaii Telescope (CFHT) to obtain spatially resolved spectroscopy across nearby galaxies. In my mind, SITELLE is the halfway point between narrowband photometry and true integral-field spectroscopy. We take images in particular wavelength ranges (usually targeting bright emission lines), but inside each of those images, we have spectral information. SITELLE&amp;rsquo;s combination of a large field of view and its high spatial resolution makes it possible to study multiple things at once: individual H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions, populations of H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions across a galaxy, and the larger galactic environments in which those regions form.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/signals/intspec.png"
alt="A scientific plot showing a spectrum with flux on the vertical axis and wavelength on the horizontal axis. The wavelength increases from left to right with jumps in wavelength where there is no data. The left panel shows one emission line, the middle panel shows three emission lines, and the right panel shows five emission lines. Each line is pointed with jagged wiggles on either side of it."&gt;&lt;figcaption&gt;
&lt;p&gt;An example of a SITELLE spectrum. SITELLE collects data in three filters, targeting the strong optical emission lines. Because it is an imaging Fourier transform spectrometer, SITELLE spectra have a characteristic shape described by a &lt;em&gt;sincgauss&lt;/em&gt; function rather than a standard Gaussian. Figure 2 in Garner et al. (2026).&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;My involvement in SIGNALS has likewise spanned several scales. I have led projects on H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region diagnostics and giant H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region structure, contributed methods and analyses to studies as a co-author, obtained new SITELLE observations to pursue my own questions, and participated in the broader scientific organization of the collaboration.&lt;/p&gt;
&lt;h2 id="testing-the-assumptions-behind-nebular-diagnostics"&gt;Testing the Assumptions Behind Nebular Diagnostics&lt;/h2&gt;
&lt;p&gt;Metallicity and ionization parameter are two of the most important quantities used to describe an H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region. Both strongly affect its emission-line spectrum, and they are often thought to be anti-correlated: as the oxygen abundance increases, the ionization parameter decreases. Yet, numerous investigations have found either no correlation or a positive correlation, sparking renewed interest in how these properties are related. As if to make things worse, published calibrations of the ionization parameter can disagree substantially because they are derived from photoionization models containing different assumptions about stellar populations, chemical abundances, dust, density, and nebular geometry.&lt;/p&gt;
&lt;p&gt;Rather than adopting one of these calibrations, I constructed a custom grid of Cloudy photoionization models and used NebulaBayes to infer oxygen abundance and ionization parameter simultaneously for more than 1,500 H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions across the nearby face-on spiral galaxy NGC 628.&lt;/p&gt;
&lt;p&gt;I recovered the expected anti-correlation between oxygen abundance and ionization parameter, but the more important result was how strongly the inferred relationship depended on the assumptions built into the models. The correlation also showed substantial intrinsic scatter, with dust extinction emerging as one secondary variable related to both quantities.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/signals/logU-OH_correlation.png"
alt="A scientific chart in three panels. The left two panels plot small black points and larger black points with errorbars. There is a black line through most of the larger black points decreasing in slope from left to right with a shaded black band around it. There are other colored lines on the plot also going from left to right of various decreasing slopes. The rightmost panel shows a colorful grid from orange through red to light blue indicating high to low values. Most of the orange grid squares are towards the top of the panel with the blue grid squares at the bottom."&gt;&lt;figcaption&gt;
&lt;p&gt;The ionization parameter (log U) - oxygen abundance (12 + log(O/H)) relation. The left panel shows all H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions regardless of signal-to-noise. The middle panel selects only those with a signal-to-noise of at least 15. The right panel shows how the signal-to-noise varies across the plot. The small points are the raw data analyzed through NebulaBayes, which are binned into the larger black points. The black line is a fit to the binned data. Other correlations from the literature are also plotted. Figure 9 in Garner et al. (2025).&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;The larger lesson was that a commonly-used diagnostic should not be treated as a black box simply because it has become standard in the literature. Understanding how a calibration was constructed, and whether its assumptions match the observations, is part of making the measurement itself.&lt;/p&gt;
&lt;h3 id="developing-a-methodology"&gt;Developing a Methodology&lt;/h3&gt;
&lt;p&gt;This combination of a custom Cloudy grid and Bayesian inference was subsequently adapted within SIGNALS to address very different scientific questions.&lt;/p&gt;
&lt;p&gt;In NGC 6946, Bresolin[+Garner] et al. (2025) used this methodology to derive oxygen and nitrogen abundances for hundreds of H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions and investigate azimuthal abundance structures across the galaxy. We found an azimuthal variation across one of its spiral arms, together with comparable spatial correlation scales for oxygen and nitrogen.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/signals/bresolin.jpeg"
alt="A scientific plot showing a black-and-white image of a multi-armed spiral galaxy. On top of the image are dashed black lines outlining the positions of the arms and a circular radial grid. Colored points are scattered around some of the arms, going from red (high abundance) to purple (low abundance)."&gt;&lt;figcaption&gt;
&lt;p&gt;Oxygen abundance variations across the spiral arms of NGC 6946. Along the top left arm, the oxygen abundances grow more metal poor as you move from one side of the arm to the other. Figure 7 in Bresolin et al. (2025).&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;This methodology has now also been extended again by González-Koda[+Garner] et al. to investigate the N/O-O/H relation for galaxies occupying different parts of the cosmic large-scale structure.&lt;/p&gt;
&lt;h4 id="related-publications"&gt;Related Publications&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="spatially-resolved-hii-regions"&gt;Spatially-Resolved H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; Regions&lt;/h2&gt;
&lt;p&gt;My next lead SIGNALS project approached the same problem from the opposite direction: rather than study thousands of H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions as individual objects, I asked what happened when we resolve one H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region internally.&lt;/p&gt;
&lt;p&gt;NGC 604 in M33 is the most luminous H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region in that galaxy and one of the largest star-forming complexes in the Local Group. At the distance of M33, the SIGNALS observations provide a physical resolution of only a few parsecs. At that scale, the assumptions behind integrated nebular diagnostics can be examined directly.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/signals/pretty_images_ann.png"
alt="A three-panel scientific image showing a nebula. In the left panel, stars dot the image with the nebula in colors of white and purple. The middle panel has no stars, with just the nebula in darker purple. The right panel is the same as the left but with red drawings and white annotations marking particular features. Several loops, bubbles, and filaments can be seen."&gt;&lt;figcaption&gt;
&lt;p&gt;The giant H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region NGC 604 as seen through SITELLE. The left panel shows the deep image formed by summing all three filters together. The middle panel shows an RGB image of the gas emission lines Hα, [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;], and [O &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt;]. The right panel is the same as the middle, but with particular features annotated, including four known bubbles (A-D), and the locations of a supernova remnant and planetary nebula. Figure 1 in Garner et al. (2026).&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;I mapped the principal optical emission-line rations across the entire nebula and found enormous spatial variations in diagnostics normally used to infer ionization parameter and chemical abundance. Those variations do not primarily trace chemical inhomogeneities. Instead, they closely follow the positions of the massive stellar populations and the shells, cavities, and filaments that those stars have carved into the surrounding gas.&lt;/p&gt;
&lt;p&gt;In other words, applying an integrated H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region calibration pixel-by-pixel can return apparently dramatic changes in &amp;ldquo;metallicity&amp;rdquo; that are actually changes in ionization structure and geometry.&lt;/p&gt;
&lt;p&gt;The resolved data also revealed sources that effectively disappear when the nebula is integrated into one spectrum, including a known supernova remnant and a previously unidentified planetary nebula.&lt;/p&gt;
&lt;p&gt;The basic problem is therefore not simply spatial resolution for its own sake. It is understanding what information survives when complex physical structure is compressed into the single spectrum we usually observe.&lt;/p&gt;
&lt;h4 id="related-publications-1"&gt;Related Publications&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="stellar-feedback-kinematics"&gt;Stellar Feedback Kinematics&lt;/h2&gt;
&lt;p&gt;The original SITELLE data were excellent for mapping excitation and ionization, but the Hα profiles showed evidence that multiple kinematic components were unresolved. That immediately suggested a next observation: observe the same nebula at substantially higher spectral resolution.&lt;/p&gt;
&lt;p&gt;I led a successful CFHT proposal for new SITELLE SN4 observations at &lt;em&gt;R&lt;/em&gt; ∼ 10,000, designed specifically to resolve the ionized gas kinematics of NGC 604.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/signals/NGC604-Doppler.jpg"
alt="A color image of a nebula. Parts of the nebula are in blue and orange. Numerous loops, bubbles, and filamentary structures can be seen. "&gt;&lt;figcaption&gt;
&lt;p&gt;The giant H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region NGC 604 in high-resolution. This is a &lt;em&gt;Doppler image&lt;/em&gt;, meaning the blue colors correspond to blueshifted velocities (i.e., gas moving toward us), and the orange colors correspond to redshifted velocities (i.e., gas moving away from us). Courtesy of Laurent Drissen.&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;The new spectra allow me to fit multiple velocity components across the nebula and construct maps of velocity, velocity dispersion, and kinematic complexity. After removing the large-scale rotation of M33, the residual velocity field contains coherent structures associated with the nebula itself. I am now asking how those gas motions relate to the ionization structure measured in the original SIGNALS observations.&lt;/p&gt;
&lt;p&gt;To do this, I have used structure functions, spatial correlation measurements, and cross-comparisons of the resolved maps to quantify characterstic spatial scales. The velocity residuals and velocity dispersion show structure on smaller scales than several ionization-sensitive line ratios, suggesting that the morphology of the radiation field and the motions of the gas do not simply trace one another.&lt;/p&gt;
&lt;p&gt;This work has developed into a collaboration with researchers at Aix-Marseille Université, where we can compare NGC 604 with SITELLE observations of Milky Way H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions at still finer physical resolution. We are attempting to answer the question: &lt;em&gt;What happens to the physics we infer as an H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region moves from sub-parsec resolution to a few parsecs?&lt;/em&gt;&lt;/p&gt;
&lt;h2 id="galactic-dynamics"&gt;Galactic Dynamics&lt;/h2&gt;
&lt;p&gt;I have also led a successful SITELLE proposal targeting NGC 5474, the peculiar dwarf satellite of M101.&lt;/p&gt;
&lt;p&gt;NGC 5474 is scientifically quite different from NGC 604. Instead of resolving one giant H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region, these observations allow me to investigate ionized gas across a galaxy with an unusual dynamical history, asymmetric structure, and an extended low surface brightness disk.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/signals/NGC5474.png"
alt="A color image of a galaxy. The galaxy shows a faint white featureless disk on top of which are numerous red clumps of light. There is also a featureless white circular bulge towards the top of the faint white disk."&gt;&lt;figcaption&gt;
&lt;p&gt;The peculiar dwarf galaxy NGC 5474. Reddish light indicates star-forming regions. Courtesy of Laurent Drissen.&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;My goal is to use the ionized gas kinematics and H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region population to ask how the gas responded to both the peculiar offset bulge of NGC 5474 and its interaction history with M101. The wide SITELLE field is also particularly valuable for tracing emission into the galaxy&amp;rsquo;s low surface brightness outskirts.&lt;/p&gt;
&lt;h2 id="science-in-a-collaboration"&gt;Science in a Collaboration&lt;/h2&gt;
&lt;p&gt;SIGNALS has also been important to me because it is my first experience with a large collaborative group.&lt;/p&gt;
&lt;p&gt;The survey brings together people studying H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions, chemical evolution, diffuse ionized gas, stellar feedback, supernova remnants, planetary nebulae, galactic dynamics, and other features we can trace with ionized gas in nearby galaxies. Working within that environment has allowed me to grow as a researcher.&lt;/p&gt;
&lt;p&gt;In addition to the NGC 6946 and large-scale environment abundance studies, I am a co-author on SIGNALS work examining AGN-ISM interactions in NGC 4258, where spatially resolved excitation and kinematics reveal how the galaxy&amp;rsquo;s jet interacts with the surrounding gas.&lt;/p&gt;
&lt;p&gt;Several additionall projects are currently moving through the publication process, including:&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;a large H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region catalog for M33 (led by Emma Jarvis);&lt;/li&gt;
&lt;li&gt;a comparison of H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region structure using PHANGS-MUSE observations (led by Lorena Aragüete Riesco);&lt;/li&gt;
&lt;li&gt;and work on the filling factor and dust-filament structure of H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions in NGC 628 (also led by Lorena Aragüete Riesco).&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;These projects span substantially different science questions, but they share a common need: understanding how resolved nebular structure affects the physical quantities we infer from emission lines.&lt;/p&gt;
&lt;h2 id="the-broad-picture"&gt;The Broad Picture&lt;/h2&gt;
&lt;p&gt;The individual projects above address different objects and different physical questions, but they have increasingly converged on the same underlying theme.&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;In NGC 628, I found that even measurements of integrated H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions depend strongly on the assumptions used to translate emission-line ratios into physical properties.&lt;/li&gt;
&lt;li&gt;In NGC 604, I showed that diagnostics that are meaningful for an integrated nebula can become physically misleading when applied to individual pixels.&lt;/li&gt;
&lt;li&gt;The new NGC 604 observations push this one step further by asking how ionization and gas kinematics are related across physical scales.&lt;/li&gt;
&lt;li&gt;The broader SIGNALS collaboration then provides populations of H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions across many galactic environments with which those ideas can be tested.&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;Together, these projects allow me to answer &lt;em&gt;What physical structure produced this line ratio, and what information survives in the way I have observed it?&lt;/em&gt;&lt;/p&gt;
&lt;h2 id="methods-and-expertise"&gt;Methods and Expertise&lt;/h2&gt;
&lt;p&gt;My work within SIGNALS has developed and demonstrated expertise across several interconnected areas:&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Nebular astrophysics&lt;/strong&gt;
H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region physics · chemical abundances · ionization parameter · excitation diagnostics · stellar feedback&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Physical modeling&lt;/strong&gt;
Cloudy · NebulaBayes · PyNeb&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Spectroscopy&lt;/strong&gt;
CFHT/SITELLE · ORCS · multi-component kinematics&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Spatial analysis&lt;/strong&gt;
Resolved emission-line maps · velocity fields · structure functions · correlation lengths&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Statistical methods&lt;/strong&gt;
Bayesian inference · Monte Carlo uncertainty propagation&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Research development&lt;/strong&gt;
Observing proposal design · collaboration across institutions · mentoring and collaborative analysis&lt;/p&gt;
&lt;h2 id="selected-publications"&gt;Selected Publications&lt;/h2&gt;
&lt;h4 id="first-author-work"&gt;First Author Work&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;&lt;strong&gt;Garner et al. (2026)&lt;/strong&gt;:
&lt;br&gt; Resolved excitation, ionization, abundance diagnostics, and gas kinematics across one of the Local Group&amp;rsquo;s most luminous H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Garner et al. (2025)&lt;/strong&gt;:
&lt;br&gt; A self-consistent photoionization model analysis of more than 1,500 H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions, testing both the physical O/H-logU relation and the assumptions behind common calibrations.&lt;/li&gt;
&lt;/ul&gt;
&lt;h4 id="collaborative-work"&gt;Collaborative Work&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;&lt;strong&gt;González-Koda et al. (2026)&lt;/strong&gt;:
&lt;br&gt; N/O-O/H across cluster, filament, and void environments, extending my photoionization methodology to galaxy environments.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Aragüete Riesco et al. (2026)&lt;/strong&gt;:
&lt;br&gt; Investigating the internal gas and dust structure of H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Fernández-Arenas et al. (2025)&lt;/strong&gt;:
&lt;br&gt; SIGNALS study of the spatially resolved excitation and kinematics associated with the galaxy&amp;rsquo;s anomalous arms and jet-ISM interaction.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Bresolin et al. (2025)&lt;/strong&gt;:
&lt;br&gt; The Cloudy + NebulaBayes methodology adapted to study azimuthal abundance variations and metal mixing across NGC 6946.&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="where-this-work-is-going"&gt;Where This Work Is Going&lt;/h2&gt;
&lt;p&gt;My long-term goal is to turn the extraordinary spatial information available in nearby H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions into a better physical foundation for interpreting nebular spectra everywhere else.&lt;/p&gt;
&lt;p&gt;High-resolution kinematics can determine how stellar feedback structures the gas and whether the characteristic scales of motion correspond to those seen in ionization diagnostics. Comparisons among Milky Way, Local Group, and more distant H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions can quantify exactly what information disappears as spatial resolution worsens.&lt;/p&gt;
&lt;p&gt;Broader-wavelength spectroscopy can provide a particularly important test. Direct measurements of temperature-sensitive auroral lines across resolved giant H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions would allow the apparent abundance variations predicted by strong-line diagnostics to be compared against the actual temperature and abundance structure of the gas.&lt;/p&gt;
&lt;p&gt;At the same time, the larger SIGNALS sample makes it possible to ask how all of these relationships change with galactic environment: spiral structure, metallicity, star formation rates, interaction history, and location within the host galaxy.&lt;/p&gt;</description></item><item><title>M101 Group: Galaxy Evolution in a Nearby Laboratory</title><link>https://astronoraygarner.com/projects/m101_group/</link><pubDate>Sun, 09 Aug 2026 00:00:00 +0000</pubDate><guid>https://astronoraygarner.com/projects/m101_group/</guid><description>&lt;p&gt;I have focused on the M101 Group since graduate school. Because it is only a few megaparsecs away, this small, isolated galaxy group gives us a detailed look at how spiral galaxies form and change. We can study star formation in individual H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions, map chemical abundances across a whole galactic disk, use stellar populations to trace spiral structure and interactions, and examine neighboring galaxies as part of the same dynamic system.&lt;/p&gt;
&lt;p&gt;I started studying M101 by asking: how much star formation happens beyond the bright optical disks of galaxies? This question led me to explore how M101 has grown, changed chemically, responded to its surroundings, and interacted with its satellites, especially the unusual galaxy NGC 5474.&lt;/p&gt;
&lt;p&gt;In this research, I have used deep, wide-field imaging, long-slit and integral field spectroscopy, nebular abundance measurements, stellar population modeling, and multiwavelength analysis. Each finding led to new questions. The M101 Group has been both a laboratory and a foundation for shaping how I study galaxy evolution.&lt;/p&gt;
&lt;h2 id="why-m101"&gt;Why M101?&lt;/h2&gt;
&lt;p&gt;M101, or the Pinwheel Galaxy, is a large, nearby spiral galaxy seen face-on. Its disk is noticeably asymmetric, featuring a &amp;ldquo;big wonky arm.&amp;rdquo; The outer spiral structure looks disturbed, and its largest satellite, NGC 5474, is also unusual, with a bright central bulge that is clearly offset from the center of its underlying disk.&lt;/p&gt;
&lt;p&gt;These features have suggested for some time that M101 and NGC 5474 recently interacted. However, the system is puzzling: its shape looks disturbed, but other signs of a strong interaction are unexpectedly subtle.&lt;/p&gt;
&lt;p&gt;These questions have motivated much of my research. What effects does a weak tidal interaction have on a large spiral galaxy? Where should we look for its signs: in current star formation, chemical abundances, stellar ages, spiral structure, or satellite dynamics? And how long do these signs last?&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/m101_group/m101-group.jpg"
alt="View of the M101 Group. M101 is at the center, with its asymmetric spiral arms and numerous pink star-forming regions. NGC 5474 is to the bottom left with its offset bulge clearly visible to the north of a face-on spiral disk. Another M101 satellite, NGC 5477, is immediately to the left of M101; a small irregularly shaped galaxy. Numerous other background galaxies and foreground stars dot the image."&gt;&lt;figcaption&gt;
&lt;p&gt;The M101 Group provides a nearby laboratory for studying spiral structure, satellite interactions, chemical evolution, and star formation.
&lt;a href="https://app.astrobin.com/i/580z7j"&gt;Image credit: Doublas Rollain - Astrobin&lt;/a&gt;&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;h2 id="searching-for-star-formation-beyond-the-optical-disk"&gt;Searching for Star Formation Beyond the Optical Disk&lt;/h2&gt;
&lt;p&gt;For my first major M101 project, I used deep, wide-field narrowband imaging from the Burrell Schmidt telescope to search about 6 square degrees around the group for very faint areas of ongoing star formation.&lt;/p&gt;
&lt;p&gt;We focused on Hα, Hβ, and [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;] emission lines and created a method to distinguish real emission-line sources apart from foreground stars and background galaxies. Our goal was to find isolated H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions or new star-forming dwarf galaxies that could mark tidal material from an encounter between M101 and its companions.&lt;/p&gt;
&lt;p&gt;The surprising result was largely a null detection. Nearly all of our candidates were associated with the extreme outer disk of M101 rather than a widespread intragroup population. Only two unusual objects were associated with other systems: an outlying H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region near NGC 5474 and a star-forming object belonging to a background galaxy NGC 5486.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/m101_group/ngc5474_5486_detail.png"
alt="A two-by-two grid of images. The top row focuses on NGC 5474 and the bottom row focuses on NGC 5486. The left column shows an H-alpha image and the right column shows a broadband image."&gt;&lt;figcaption&gt;
&lt;p&gt;A zoomed-in view of the detected regions near NGC 5474 (top row) and NGC 5486 (bottom row). Left: the continuum-subtracted Hα image. Right: the broadband &lt;em&gt;B&lt;/em&gt; image, stretched to show the faint structure of the outer disks. The red circle represents the size of a galaxy mask. The orange circle is an object detected in all three narrowband images, while the green circle is an object detected in the Hα and [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;] image.Figure 9 of Garner et al. (2021)&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;Instead of being disappointing, this result changed my perspective on the group. If M101’s obvious asymmetries came from a recent encounter, it seems that event did not spread much star-forming gas into the surrounding area. Or, if it did, the Hα signals we looked for had already faded.&lt;/p&gt;
&lt;h4 id="what-this-work-demonstrated"&gt;What This Work Demonstrated&lt;/h4&gt;
&lt;p&gt;Through this project, I gained experience with deep optical imaging, careful continuum subtraction, detecting low surface brightness sources, emission-line photometry, building catalogs, rejecting contaminants, following up with spectroscopy, and interpreting null results.&lt;/p&gt;
&lt;p&gt;It also taught me an important lesson that has guided my research: not finding an expected signal can still tell us something physical. The lack of intragroup star formation helped narrow down possible interaction histories for the system and encouraged me to search for more subtle signs within the galaxies.&lt;/p&gt;
&lt;h4 id="related-publications"&gt;Related Publications&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="chemical-evolution-across-m101"&gt;Chemical Evolution Across M101&lt;/h2&gt;
&lt;p&gt;If the interaction had not produced large numbers of isolated star-forming regions, perhaps its signature could instead be found in the chemical structure of M101&amp;rsquo;s disk.&lt;/p&gt;
&lt;p&gt;Using an expanded Burrell Schmidt dataset including Hα, Hβ, [O &lt;span style='font-size: 0.8em;'&gt;III&lt;/span&gt;], and [O &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt;], I measured strong-line oxygen abundances for 720 H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions across M101, NGC 5474, and NGC 5477.&lt;/p&gt;
&lt;p&gt;M101 shows the usual drop in metallicity as you move farther from the center, but the full two-dimensional data revealed a more complex situation. The gradient flattens in the outer disk, and H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions there show clear azimuthal abundance patterns. These differences from a simple radial gradient mostly appear in parts of the disk that may have been shaped by M101’s interactions with NGC 5474.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/m101_group/m101_break_kk04.png"
alt="A plot showing a radial trend in HII regions. There is a cluster of points going from the top left at high abundance, low radius to the bottom right at low abundance, high radius."&gt;&lt;figcaption&gt;
&lt;p&gt;The Kobulnicky &amp;amp; Kewley (2004) oxygen abundances of M101 fitted with a simple exponential (dashed black line) and a broken exponential (solid black line). Regions in the turn-around region (orange circles), upper branch (blue triangles), and lower branch (green inverted triangles) are distinguished. Outside 1.3&lt;em&gt;R&lt;/em&gt;&lt;sub&gt;23&lt;/sub&gt;, we display both the upper- and lower-branch solutions connected by a dotted line for each individual H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region.Figure 10 of Garner et al. (2022)&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;h4 id="what-this-work-demonstrated-1"&gt;What This Work Demonstrated&lt;/h4&gt;
&lt;p&gt;This project expanded my expertise in nebular astrophysics and chemical evolution, including reddening corrections, emission-line ratios, strong-line abundance diagnostics, metallicity gradients, uncertainty propagation, and spatial statistics.&lt;/p&gt;
&lt;p&gt;More broadly, it taught me to connect local and global views of galaxies. Individual H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions show local conditions, but hundreds of these measurements can reveal patterns in chemical enrichment and mixing across kiloparsec scales. Linking the physics of single nebulae to the evolution of their host galaxies became a key theme in my later work.&lt;/p&gt;
&lt;h4 id="related-publications-1"&gt;Related Publications&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="spiral-dynamics-through-stellar-populations"&gt;Spiral Dynamics Through Stellar Populations&lt;/h2&gt;
&lt;p&gt;The same narrowband dataset also held information I had not planned to use. Besides nebular emission, some filters captured age-sensitive stellar absorption features, like Balmer absorption and changes in the continuum near the Balmer and 4000 Å breaks. By comparing these measurements to stellar population models, I developed a way to estimate stellar ages across M101’s disk.&lt;/p&gt;
&lt;p&gt;The resulting maps showed the expected trend: younger stars are found farther from the center, which fits with inside-out growth. More interestingly, the stellar ages change in a regular way across spiral arms. In the mostly undisturbed inner disk, these age patterns match what we expect from large-scale spiral shocks. Surprisingly, similar patterns also show up farther out, beyond the expected corotation radius of the main inner spiral.&lt;/p&gt;
&lt;p&gt;I saw these results as evidence that M101’s seemingly organized structure may come from several dynamically linked spiral patterns, not just one rigidly rotating spiral density wave.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/m101_group/inner_env.png"
alt="A plot showing three clusters of colored points, red, green, and blue."&gt;&lt;figcaption&gt;
&lt;p&gt;The equivalent width through the Hβ filters (&lt;em&gt;W&lt;/em&gt;&lt;sub&gt;Hβ&lt;/sub&gt;) and [O &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt;] filters (&lt;em&gt;W&lt;/em&gt;&lt;sub&gt;3746&lt;/sub&gt;) for all pixels in the main disk of M101 distinguished by environment: the inner disk in red, spiral arms in blue, and interarm regions in green.Figure 9 of Garner et al. (2024)&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;h4 id="what-this-work-demonstrated-2"&gt;What This Work Demonstrated&lt;/h4&gt;
&lt;p&gt;For this project, I had to use an observational dataset for a new question it was not meant to answer. I developed techniques for modeling stellar populations, linked narrowband observations to synthetic spectra, made spatial age maps, and interpreted these results in terms of spiral dynamics.&lt;/p&gt;
&lt;p&gt;This work expanded my research from studying present-day ionized gas to looking at the stellar fossil record. Gas emission shows what a galaxy is doing now, while stellar populations hold clues about its past. By combining both, we get a much clearer picture of galaxy evolution than by using either one alone.&lt;/p&gt;
&lt;h4 id="related-publications-2"&gt;Related Publications&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="ngc-5474-a-hidden-galaxy-in-plain-sight"&gt;NGC 5474: A Hidden Galaxy in Plain Sight&lt;/h2&gt;
&lt;p&gt;My dissertation led me to another question: if an encounter with NGC 5474 helped reshape M101, what happened to NGC 5474 itself?&lt;/p&gt;
&lt;p&gt;NGC 5474 has a strange shape. Its bright central part, usually called its &amp;lsquo;bulge,&amp;rsquo; is about a kiloparsec away from the center of its star-forming disk. Some have suggested that this part is not a bulge, but actually a separate dwarf galaxy seen in front of NGC 5474.&lt;/p&gt;
&lt;p&gt;With PINGS PPak integral field spectroscopy, I measured the velocity of the stars in the supposed bulge and compared it to the ionized gas velocity in the surrounding disk. The two are offset by about 24 km/s, which gives kinematic evidence that they are separate systems.&lt;/p&gt;
&lt;figure&gt;&lt;img src="https://astronoraygarner.com/projects/m101_group/n5474_real_v3.jpg"
alt="An image showing NGC 5474. There is a bright circular region at the center of the image, with a faint spiral disk offset below it."&gt;&lt;figcaption&gt;
&lt;p&gt;An RGB color image of NGC 5474.Figure 1 of Garner et al. (2025)&lt;/p&gt;
&lt;/figcaption&gt;
&lt;/figure&gt;
&lt;p&gt;This idea was supported by work I supervised with undergraduate researcher Liv Moody, who used the narrowband data to study stellar populations across NGC 5474. The offset bulge is made up mostly of old stars and is different from the surrounding disk. The galaxy’s outer stellar populations also show extra spatial structure that may relate to its interaction history.&lt;/p&gt;
&lt;p&gt;This part of the project also marked a change in my role as a researcher. I moved from doing the analysis myself to designing research questions, developing methods, and mentoring another researcher through an independent project.&lt;/p&gt;
&lt;h4 id="related-publications-3"&gt;Related Publications&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="returning-to-m101-with-hetdex"&gt;Returning to M101 with HETDEX&lt;/h2&gt;
&lt;p&gt;My current work brings me back to M101, but with a very different dataset. The Hobby-Eberly Telescope Dark Energy Experiment (HETDEX) observed M101 using the VIRUS integral field spectrograph, giving us complete spectroscopic coverage of M101’s disk for the first time.&lt;/p&gt;
&lt;p&gt;I am using these spectra along with multiwavelength photometry to map the galaxy’s stellar ages, metallicities, star formation history, and both stellar and gas kinematics. This work brings my M101 research full circle. My first projects used individual H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; regions to study the galaxy’s current state. Now, HETDEX lets me compare those signs to the history recorded in the overall stellar population.&lt;/p&gt;
&lt;h4 id="related-publications-4"&gt;Related Publications&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;
&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="the-broad-picture"&gt;The Broad Picture&lt;/h2&gt;
&lt;p&gt;Taken together, these projects show that galaxy interactions do not always leave just one clear observational sign.&lt;/p&gt;
&lt;p&gt;In the M101 Group, signs of dynamical evolution look different depending on which tracer you study:&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;The surrounding group contains little widespread intragroup star formation;&lt;/li&gt;
&lt;li&gt;The disk of M101 contains chemical structure beyond a simple radial gradient;&lt;/li&gt;
&lt;li&gt;Its stellar populations encode both inside-out growth and complex spiral dynamics;&lt;/li&gt;
&lt;li&gt;NGC 5474 contains a dynamically distinct central component and unusual stellar populations;&lt;/li&gt;
&lt;li&gt;The stellar fossil record provides a way to connect these present-day signatures to longer evolutionary timescales.&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;This is one of the main lessons I have learned from these projects. Galaxy evolution is complex and happens on many scales and timescales. Features like shape, ionized gas, chemical abundances, stellar populations, and kinematics do not all react to an interaction in the same way or keep its signature for the same length of time. The M101 Group is especially valuable because its closeness lets us study all these tracers together.&lt;/p&gt;
&lt;h2 id="methods-and-expertise"&gt;Methods and Expertise&lt;/h2&gt;
&lt;p&gt;My work on the M101 Group has developed and demonstrated expertise across several areas of observational astronomy:&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Observational Techniques&lt;/strong&gt;:
Deep wide-field imaging · Narrowband imaging · Long-slit spectroscopy · Integral field spectroscopy · Multiwavelength photometry&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Galaxy Evolution&lt;/strong&gt;:
Star formation · Galaxy interactions · Spiral structure · Stellar populations · Chemical evolution&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Nebular Astrophysics&lt;/strong&gt;:
H &lt;span style='font-size: 0.8em;'&gt;II&lt;/span&gt; region identification · Emission-line photometry · Reddening corrections · Strong-line abundances · Metallicity gradients&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Stellar Populations&lt;/strong&gt;:
Synthetic stellar population modeling · Age-sensitive spectral features · Full spectral fitting · Star formation histories · Stellar metallicities&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Data Analysis&lt;/strong&gt;:
Python · Astropy · CIGALE · pPXF · Spectral fitting · Image analysis · Catalog construction · Spatially resolved mapping · Statistical modeling&lt;/p&gt;
&lt;h2 id="selected-publications"&gt;Selected Publications&lt;/h2&gt;
&lt;h4 id="first-author-work"&gt;First Author Work&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;&lt;strong&gt;Garner et al. 2026&lt;/strong&gt;:
&lt;br&gt; Spatially resolved stellar ages and metallicities from HETDEX spectroscopy.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Garner et al. 2025&lt;/strong&gt;:
&lt;br&gt; Kinematic evidence that the offset bulge of NGC 5474 is a distance stellar system.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Garner et al. 2024&lt;/strong&gt;:
&lt;br&gt; Using age-sensitive narrowband measurements to trace disk growth and spiral dynamics.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Garner et al. 2023&lt;/strong&gt;:
&lt;br&gt; Spectroscopic confirmation and interpretation of unusual objects discovered in the original narrowband survey.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Garner et al. 2022&lt;/strong&gt;:
&lt;br&gt; Spatially resolved chemical abundances across M101 and its major satellites.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Garner et al. 2021&lt;/strong&gt;:
&lt;br&gt; Deep search for star formation and low-luminosity galaxies throughout the M101 Group.&lt;/li&gt;
&lt;/ul&gt;
&lt;h4 id="collaborative--mentored-work"&gt;Collaborative &amp;amp; Mentored Work&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;&lt;strong&gt;Moody &amp;amp; Garner 2025&lt;/strong&gt;:
&lt;br&gt; Undergraduate-led project extending my stellar population methodology to NGC 5474. I mentored the project and contributed to the analysis and physical interpretation.&lt;/li&gt;
&lt;li&gt;&lt;strong&gt;Watkins et al. 2024&lt;/strong&gt;:
&lt;br&gt; Collaborative investigation of the origin of diffuse ionized gas using the same deep imaging dataset together with ultraviolet observations and photoionization modeling.&lt;/li&gt;
&lt;/ul&gt;
&lt;h4 id="dissertation"&gt;Dissertation&lt;/h4&gt;
&lt;ul&gt;
&lt;li&gt;
&lt;br&gt; My PhD dissertation brought together the originaly outlying star-formation, chemical abundances, and stellar population studies into a unified investigation of M101 and its group environment.&lt;/li&gt;
&lt;/ul&gt;
&lt;h2 id="where-this-work-is-going"&gt;Where This Work Is Going&lt;/h2&gt;
&lt;p&gt;The M101 Group is still a key part of my research because it lets me connect physical processes measured on many different scales. The methods I developed here can be used beyond M101. Studying nearby galaxies allows us to link detailed nebular physics, stellar populations, chemical abundances, and galactic dynamics in ways we cannot with more distant galaxies. These local relationships can then help us understand galaxies across cosmic time.&lt;/p&gt;</description></item></channel></rss>