<?xml version="1.0" encoding="UTF-8"?><rss version="2.0"
	xmlns:content="http://purl.org/rss/1.0/modules/content/"
	xmlns:wfw="http://wellformedweb.org/CommentAPI/"
	xmlns:dc="http://purl.org/dc/elements/1.1/"
	xmlns:atom="http://www.w3.org/2005/Atom"
	xmlns:sy="http://purl.org/rss/1.0/modules/syndication/"
	xmlns:slash="http://purl.org/rss/1.0/modules/slash/"
	>

<channel>
	<title>non-rotating metal-free stars &#8211; Science</title>
	<atom:link href="https://scienmag.com/tag/non-rotating-metal-free-stars/feed/" rel="self" type="application/rss+xml" />
	<link>https://scienmag.com</link>
	<description></description>
	<lastBuildDate>Fri, 20 Jun 2025 10:37:14 +0000</lastBuildDate>
	<language>en-US</language>
	<sy:updatePeriod>
	hourly	</sy:updatePeriod>
	<sy:updateFrequency>
	1	</sy:updateFrequency>
	<generator>https://wordpress.org/?v=7.0</generator>

<image>
	<url>https://scienmag.com/wp-content/uploads/2024/07/cropped-scienmag_ico-32x32.jpg</url>
	<title>non-rotating metal-free stars &#8211; Science</title>
	<link>https://scienmag.com</link>
	<width>32</width>
	<height>32</height>
</image> 
<site xmlns="com-wordpress:feed-additions:1">73899611</site>	<item>
		<title>Mapping First Stars&#8217; Mass via 21-cm Signal</title>
		<link>https://scienmag.com/mapping-first-stars-mass-via-21-cm-signal/</link>
		
		<dc:creator><![CDATA[SCIENMAG]]></dc:creator>
		<pubDate>Fri, 20 Jun 2025 10:37:14 +0000</pubDate>
				<category><![CDATA[Space]]></category>
		<category><![CDATA[21-cm cosmological signal simulation]]></category>
		<category><![CDATA[Bayesian analysis in astrophysics]]></category>
		<category><![CDATA[binary star effects on emissivity]]></category>
		<category><![CDATA[cosmological 21-cm signal analysis]]></category>
		<category><![CDATA[Lyman-Werner band emissivity]]></category>
		<category><![CDATA[MESA stellar evolution code]]></category>
		<category><![CDATA[non-rotating metal-free stars]]></category>
		<category><![CDATA[Pop III initial mass function]]></category>
		<category><![CDATA[Pop III stellar evolution modeling]]></category>
		<category><![CDATA[stellar population spectra integration]]></category>
		<category><![CDATA[TLUSTY atmospheric modeling]]></category>
		<category><![CDATA[X-ray binaries in early universe]]></category>
		<guid isPermaLink="false">https://scienmag.com/mapping-first-stars-mass-via-21-cm-signal/</guid>

					<description><![CDATA[Certainly! Here is a concise and clear synthesis of the methodology described in your passage about modeling Pop III stellar spectra, X-ray binaries (XRBs), and simulating the 21-cm cosmological signal using 21CMSPACE, including the use of emulators for efficient Bayesian analysis: Modelling Pop III Stellar Spectra Stellar Evolution Tracks: Pop III stars are modeled using [&#8230;]]]></description>
										<content:encoded><![CDATA[<p>Certainly! Here is a concise and clear synthesis of the methodology described in your passage about modeling Pop III stellar spectra, X-ray binaries (XRBs), and simulating the 21-cm cosmological signal using 21CMSPACE, including the use of emulators for efficient Bayesian analysis:</p>
<hr />
<h3>Modelling Pop III Stellar Spectra</h3>
<ul>
<li><strong>Stellar Evolution Tracks</strong>: Pop III stars are modeled using MESA (version 12115) assuming isolated, non-rotating, metal-free (Z=0), and negligible mass loss stars evolving from zero-age main sequence to core hydrogen depletion for (M \lesssim 310\, M_{\odot}).</li>
<li><strong>Stellar Atmospheres</strong>: TLUSTY (version 205) computes a grid of stellar atmospheres/spectra across effective temperature and surface gravity, using non-LTE modeling with H and He only (Big Bang proportions), motivated by zero surface metallicity predictions.</li>
<li><strong>Population Spectra</strong>: Integrated spectra along evolutionary tracks are combined and weighted by the Pop III initial mass function (IMF) to compute population-averaged Lyman-band and Lyman-Werner band emissivities in 21CMSPACE.</li>
<li><strong>Binary Effects</strong>: Neglecting binaries in Pop III stellar spectra causes, at most, a 25% underestimation of Lyman–Werner emissivities, a relatively small impact compared to other uncertainties.</li>
</ul>
<hr />
<h3>Modelling Pop III X-ray Binaries (XRBs)</h3>
<ul>
<li><strong>Cataloguing Metal-free Binaries</strong>: Using 21CMSPACE Pop III star formation rates, stars are sampled per IMF, with 28% assumed in binaries—a conservative fraction. Binaries are paired randomly without mass-dependence; binary fraction uncertainty scales X-ray emissivities by at most a factor of 3.</li>
<li><strong>Binary Population Synthesis</strong>: The catalog is input into BINARY_C with consistent Z=0 stellar evolution tracks. XRBs are defined as binaries with primary compact object (BH or NS) accreting mass via wind or Roche-lobe overflow.</li>
<li><strong>XRB Spectral Modeling</strong>: Thin accretion disks plus Comptonization are used to model SEDs based on accretion rate, compact object mass, and orbital parameters; X-ray escape fractions consider halo-mass-dependent absorption by primordial gas.</li>
<li><strong>X-ray Emissivities</strong>: Pop III XRB emissivity peaks mostly between 0.9 – 3.8 keV, crucial for IGM heating. The integrated specific X-ray emissivities (f_{X,III}) vary by a factor ~257 across IMFs due to competing effects: number of binaries, fraction forming XRBs, XRB lifetimes, and individual XRB luminosities.</li>
<li><strong>Uncertainties</strong>: Effects such as supernova kicks, common-envelope evolution, and mass transfer are tested and found likely subdominant compared to IMF variation; these introduce mostly IMF-independent scalings.</li>
</ul>
<hr />
<h3>Simulations of the 21-cm Signal with 21CMSPACE</h3>
<ul>
<li><strong>Code Overview</strong>: 21CMSPACE simulates large-scale structure and astrophysics impacting 21-cm signals with a grid of (128^3) cells (3 cMpc sides), modeling sub-grid physics analytically or via fits.</li>
<li><strong>Implemented Physics</strong>: Includes Pop III and Pop II star formation, radiative processes, WF coupling, feedback mechanisms, X-ray heating and ionization, reionization, redshift-space distortions, etc.</li>
<li>
<strong>X-ray Emissivity Implementation</strong>: Separate specific X-ray emissivities and SEDs are assigned to Pop II and Pop III halos:</p>
<p>[<br />
\frac{L<em>X^{\text{halo}}}{\text{SFR}^{\text{halo}}} = 3 \times 10^{40} f</em>{X,j} \; \mathrm{erg\,s^{-1} M_{\odot}^{-1} yr}<br />
]</p>
<p>where (j \in {\mathrm{II}, \mathrm{III}}), with (f<em>{X,III}) IMF-dependent and (f</em>{X,II}) free parameter.
</li>
<li><strong>Correlation of Parameters</strong>: Because both (f_{X,II}) and Pop III IMF impact X-ray heating similarly, their parameters are fit simultaneously, preventing biased or over-confident IMF constraints.</li>
</ul>
<hr />
<h3>Emulation of the 21-cm Signal for Bayesian Analysis</h3>
<ul>
<li><strong>Motivation</strong>: Direct 21CMSPACE runs (~hours each) are computationally unfeasible for nested sampling requiring millions of likelihood evaluations.</li>
<li><strong>Neural Network Emulators</strong>: Created separate emulators for global signal and power spectrum for each of six IMFs (12 networks total), trained on 10,000 simulations per IMF covering redshift (7 \leq z \leq 39) and (0.085 \leq k \leq 1) cMpc(^{-1}):
<ul>
<li>Global signal emulators: 5 hidden layers, 16 nodes/layer</li>
<li>Power spectrum emulators: 4 hidden layers, 100 nodes/layer</li>
</ul>
</li>
<li><strong>Training and Validation</strong>: Use 90% of simulations for training, 10% for testing; error metrics are root-mean-square error for the global signal and a modified fractional error for the power spectrum.</li>
<li><strong>Performance</strong>: Emulator errors comparable to or better than previous studies, enabling fast, accurate, and reliable Bayesian inference on the Pop III IMF and astrophysical parameters.</li>
</ul>
<hr />
<h4>Summary:</h4>
<p>This methodology builds a self-consistent framework linking Pop III stellar evolution and XRB modeling to 21-cm cosmological signals, leveraging sophisticated population synthesis and large-scale simulation codes, and accelerates inference via neural network emulators, enabling robust predictions and parameter estimation of the Pop III IMF and related astrophysics from upcoming 21-cm observations.</p>
<hr />
<p>If you want, I can also help summarize specific parts, outline pros/cons, or assist with any clarifications or computations related to this methodology.</p>
]]></content:encoded>
					
		
		
		<post-id xmlns="com-wordpress:feed-additions:1">55002</post-id>	</item>
	</channel>
</rss>
