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FIRE in the Field: Simulating the Threshold of Galaxy Formation
We present a suite of 15 cosmological zoom-in simulations of isolated dark matter halos, all with masses of \(M_{\rm halo} \approx 10^{10}\,{\rm M}_\odot\) at \(z=0\), in order to understand the relationship between halo assembly, galaxy formation, and feedback's effects on the central density...
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creator | Fitts, Alex Boylan-Kolchin, Michael Elbert, Oliver D Bullock, James S Hopkins, Philip F Onorbe, Jose Wetzel, Andrew R Wheeler, Coral Claude-Andre Faucher-Giguere Keres, Dusan Skillman, Evan D Weisz, Daniel R |
description | We present a suite of 15 cosmological zoom-in simulations of isolated dark matter halos, all with masses of \(M_{\rm halo} \approx 10^{10}\,{\rm M}_\odot\) at \(z=0\), in order to understand the relationship between halo assembly, galaxy formation, and feedback's effects on the central density structure in dwarf galaxies. These simulations are part of the Feedback in Realistic Environments (FIRE) project and are performed at extremely high resolution. The resultant galaxies have stellar masses that are consistent with rough abundance matching estimates, coinciding with the faintest galaxies that can be seen beyond the virial radius of the Milky Way (\(M_\star/{\rm M}_\odot\approx 10^5-10^7\)). This non-negligible spread in stellar mass at \(z=0\) in halos within a narrow range of virial masses is strongly correlated with central halo density or maximum circular velocity \(V_{\rm max}\). Much of this dependence of \(M_\star\) on a second parameter (beyond \(M_{\rm halo}\)) is a direct consequence of the \(M_{\rm halo}\sim10^{10}\,{\rm M}_\odot\) mass scale coinciding with the threshold for strong reionization suppression: the densest, earliest-forming halos remain above the UV-suppression scale throughout their histories while late-forming systems fall below the UV-suppression scale over longer periods and form fewer stars as a result. In fact, the latest-forming, lowest-concentration halo in our suite fails to form any stars. Halos that form galaxies with \(M_\star\gtrsim2\times10^{6}\,{\rm M}_\odot\) have reduced central densities relative to dark-matter-only simulations, and the radial extent of the density modifications is well-approximated by the galaxy half-mass radius \(r_{1/2}\). This apparent stellar mass threshold of \(M_\star \approx 2\times 10^{6} \approx 2\times 10^{-4} \,M_{\rm halo}\) is broadly consistent with previous work and provides a testable prediction of FIRE feedback models in LCDM. |
doi_str_mv | 10.48550/arxiv.1611.02281 |
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These simulations are part of the Feedback in Realistic Environments (FIRE) project and are performed at extremely high resolution. The resultant galaxies have stellar masses that are consistent with rough abundance matching estimates, coinciding with the faintest galaxies that can be seen beyond the virial radius of the Milky Way (\(M_\star/{\rm M}_\odot\approx 10^5-10^7\)). This non-negligible spread in stellar mass at \(z=0\) in halos within a narrow range of virial masses is strongly correlated with central halo density or maximum circular velocity \(V_{\rm max}\). Much of this dependence of \(M_\star\) on a second parameter (beyond \(M_{\rm halo}\)) is a direct consequence of the \(M_{\rm halo}\sim10^{10}\,{\rm M}_\odot\) mass scale coinciding with the threshold for strong reionization suppression: the densest, earliest-forming halos remain above the UV-suppression scale throughout their histories while late-forming systems fall below the UV-suppression scale over longer periods and form fewer stars as a result. In fact, the latest-forming, lowest-concentration halo in our suite fails to form any stars. Halos that form galaxies with \(M_\star\gtrsim2\times10^{6}\,{\rm M}_\odot\) have reduced central densities relative to dark-matter-only simulations, and the radial extent of the density modifications is well-approximated by the galaxy half-mass radius \(r_{1/2}\). This apparent stellar mass threshold of \(M_\star \approx 2\times 10^{6} \approx 2\times 10^{-4} \,M_{\rm halo}\) is broadly consistent with previous work and provides a testable prediction of FIRE feedback models in LCDM.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1611.02281</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Abundance ; Computer simulation ; Dark matter ; Density ; Dependence ; Dwarf galaxies ; Feedback ; Galactic evolution ; Galactic halos ; Ionization ; Milky Way Galaxy ; Simulation ; Star & galaxy formation ; Star formation ; Stars & galaxies ; Stellar mass</subject><ispartof>arXiv.org, 2017-09</ispartof><rights>2017. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/2076482164?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>780,784,25753,27925,37012,44590</link.rule.ids></links><search><creatorcontrib>Fitts, Alex</creatorcontrib><creatorcontrib>Boylan-Kolchin, Michael</creatorcontrib><creatorcontrib>Elbert, Oliver D</creatorcontrib><creatorcontrib>Bullock, James S</creatorcontrib><creatorcontrib>Hopkins, Philip F</creatorcontrib><creatorcontrib>Onorbe, Jose</creatorcontrib><creatorcontrib>Wetzel, Andrew R</creatorcontrib><creatorcontrib>Wheeler, Coral</creatorcontrib><creatorcontrib>Claude-Andre Faucher-Giguere</creatorcontrib><creatorcontrib>Keres, Dusan</creatorcontrib><creatorcontrib>Skillman, Evan D</creatorcontrib><creatorcontrib>Weisz, Daniel R</creatorcontrib><title>FIRE in the Field: Simulating the Threshold of Galaxy Formation</title><title>arXiv.org</title><description>We present a suite of 15 cosmological zoom-in simulations of isolated dark matter halos, all with masses of \(M_{\rm halo} \approx 10^{10}\,{\rm M}_\odot\) at \(z=0\), in order to understand the relationship between halo assembly, galaxy formation, and feedback's effects on the central density structure in dwarf galaxies. These simulations are part of the Feedback in Realistic Environments (FIRE) project and are performed at extremely high resolution. The resultant galaxies have stellar masses that are consistent with rough abundance matching estimates, coinciding with the faintest galaxies that can be seen beyond the virial radius of the Milky Way (\(M_\star/{\rm M}_\odot\approx 10^5-10^7\)). This non-negligible spread in stellar mass at \(z=0\) in halos within a narrow range of virial masses is strongly correlated with central halo density or maximum circular velocity \(V_{\rm max}\). Much of this dependence of \(M_\star\) on a second parameter (beyond \(M_{\rm halo}\)) is a direct consequence of the \(M_{\rm halo}\sim10^{10}\,{\rm M}_\odot\) mass scale coinciding with the threshold for strong reionization suppression: the densest, earliest-forming halos remain above the UV-suppression scale throughout their histories while late-forming systems fall below the UV-suppression scale over longer periods and form fewer stars as a result. In fact, the latest-forming, lowest-concentration halo in our suite fails to form any stars. Halos that form galaxies with \(M_\star\gtrsim2\times10^{6}\,{\rm M}_\odot\) have reduced central densities relative to dark-matter-only simulations, and the radial extent of the density modifications is well-approximated by the galaxy half-mass radius \(r_{1/2}\). This apparent stellar mass threshold of \(M_\star \approx 2\times 10^{6} \approx 2\times 10^{-4} \,M_{\rm halo}\) is broadly consistent with previous work and provides a testable prediction of FIRE feedback models in LCDM.</description><subject>Abundance</subject><subject>Computer simulation</subject><subject>Dark matter</subject><subject>Density</subject><subject>Dependence</subject><subject>Dwarf galaxies</subject><subject>Feedback</subject><subject>Galactic evolution</subject><subject>Galactic halos</subject><subject>Ionization</subject><subject>Milky Way Galaxy</subject><subject>Simulation</subject><subject>Star & galaxy formation</subject><subject>Star formation</subject><subject>Stars & galaxies</subject><subject>Stellar mass</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNotjc1Kw0AYRQdBsNQ-QHcDrhO_-ea3bkRK0xYKgs2-TCYzJiXNaH6kvr1BXR24HO4hZMkgFUZKeLTdtf5KmWIsBUTDbsgMOWeJEYh3ZNH3ZwBApVFKPiPP2f5tQ-uWDpWnWe2b8oke68vY2KFu33_XvOp8X8WmpDHQrW3s9ZtmsbtMRmzvyW2wTe8X_5yTPNvk611yeN3u1y-HxEoUiQ5OWBcsl0IpcGBWwasicC2kYY5LxmHltAOmykK5yS04OOm9Y5YbDJrPycPf7UcXP0ffD6dzHLt2Kp4QtBIGmRL8ByxfSVI</recordid><startdate>20170930</startdate><enddate>20170930</enddate><creator>Fitts, Alex</creator><creator>Boylan-Kolchin, Michael</creator><creator>Elbert, Oliver D</creator><creator>Bullock, James S</creator><creator>Hopkins, Philip F</creator><creator>Onorbe, Jose</creator><creator>Wetzel, Andrew R</creator><creator>Wheeler, Coral</creator><creator>Claude-Andre Faucher-Giguere</creator><creator>Keres, Dusan</creator><creator>Skillman, Evan D</creator><creator>Weisz, Daniel R</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope></search><sort><creationdate>20170930</creationdate><title>FIRE in the Field: Simulating the Threshold of Galaxy Formation</title><author>Fitts, Alex ; Boylan-Kolchin, Michael ; Elbert, Oliver D ; Bullock, James S ; Hopkins, Philip F ; Onorbe, Jose ; Wetzel, Andrew R ; Wheeler, Coral ; Claude-Andre Faucher-Giguere ; Keres, Dusan ; Skillman, Evan D ; Weisz, Daniel R</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a524-7fc4acfa354660c089fe6bf374581c351309c7c016db6cc4ab30c5eec1a382f73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Abundance</topic><topic>Computer simulation</topic><topic>Dark matter</topic><topic>Density</topic><topic>Dependence</topic><topic>Dwarf galaxies</topic><topic>Feedback</topic><topic>Galactic evolution</topic><topic>Galactic halos</topic><topic>Ionization</topic><topic>Milky Way Galaxy</topic><topic>Simulation</topic><topic>Star & galaxy formation</topic><topic>Star formation</topic><topic>Stars & galaxies</topic><topic>Stellar mass</topic><toplevel>online_resources</toplevel><creatorcontrib>Fitts, Alex</creatorcontrib><creatorcontrib>Boylan-Kolchin, Michael</creatorcontrib><creatorcontrib>Elbert, Oliver D</creatorcontrib><creatorcontrib>Bullock, James S</creatorcontrib><creatorcontrib>Hopkins, Philip F</creatorcontrib><creatorcontrib>Onorbe, Jose</creatorcontrib><creatorcontrib>Wetzel, Andrew R</creatorcontrib><creatorcontrib>Wheeler, Coral</creatorcontrib><creatorcontrib>Claude-Andre Faucher-Giguere</creatorcontrib><creatorcontrib>Keres, Dusan</creatorcontrib><creatorcontrib>Skillman, Evan D</creatorcontrib><creatorcontrib>Weisz, Daniel R</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>AUTh Library subscriptions: ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Fitts, Alex</au><au>Boylan-Kolchin, Michael</au><au>Elbert, Oliver D</au><au>Bullock, James S</au><au>Hopkins, Philip F</au><au>Onorbe, Jose</au><au>Wetzel, Andrew R</au><au>Wheeler, Coral</au><au>Claude-Andre Faucher-Giguere</au><au>Keres, Dusan</au><au>Skillman, Evan D</au><au>Weisz, Daniel R</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>FIRE in the Field: Simulating the Threshold of Galaxy Formation</atitle><jtitle>arXiv.org</jtitle><date>2017-09-30</date><risdate>2017</risdate><eissn>2331-8422</eissn><abstract>We present a suite of 15 cosmological zoom-in simulations of isolated dark matter halos, all with masses of \(M_{\rm halo} \approx 10^{10}\,{\rm M}_\odot\) at \(z=0\), in order to understand the relationship between halo assembly, galaxy formation, and feedback's effects on the central density structure in dwarf galaxies. These simulations are part of the Feedback in Realistic Environments (FIRE) project and are performed at extremely high resolution. The resultant galaxies have stellar masses that are consistent with rough abundance matching estimates, coinciding with the faintest galaxies that can be seen beyond the virial radius of the Milky Way (\(M_\star/{\rm M}_\odot\approx 10^5-10^7\)). This non-negligible spread in stellar mass at \(z=0\) in halos within a narrow range of virial masses is strongly correlated with central halo density or maximum circular velocity \(V_{\rm max}\). Much of this dependence of \(M_\star\) on a second parameter (beyond \(M_{\rm halo}\)) is a direct consequence of the \(M_{\rm halo}\sim10^{10}\,{\rm M}_\odot\) mass scale coinciding with the threshold for strong reionization suppression: the densest, earliest-forming halos remain above the UV-suppression scale throughout their histories while late-forming systems fall below the UV-suppression scale over longer periods and form fewer stars as a result. In fact, the latest-forming, lowest-concentration halo in our suite fails to form any stars. Halos that form galaxies with \(M_\star\gtrsim2\times10^{6}\,{\rm M}_\odot\) have reduced central densities relative to dark-matter-only simulations, and the radial extent of the density modifications is well-approximated by the galaxy half-mass radius \(r_{1/2}\). This apparent stellar mass threshold of \(M_\star \approx 2\times 10^{6} \approx 2\times 10^{-4} \,M_{\rm halo}\) is broadly consistent with previous work and provides a testable prediction of FIRE feedback models in LCDM.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1611.02281</doi><oa>free_for_read</oa></addata></record> |
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subjects | Abundance Computer simulation Dark matter Density Dependence Dwarf galaxies Feedback Galactic evolution Galactic halos Ionization Milky Way Galaxy Simulation Star & galaxy formation Star formation Stars & galaxies Stellar mass |
title | FIRE in the Field: Simulating the Threshold of Galaxy Formation |
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