MOLECULAR AND ATOMIC LINE SURVEYS OF GALAXIES. I. THE DENSE, STAR-FORMING GAS PHASE AS A BEACON
We predict the space density of molecular gas reservoirs in the universe and place a lower limit on the number counts of carbon monoxide (CO), hydrogen cyanide (HCN) molecular, and [CII] atomic emission lines in blind redshift surveys in the submillimeter-centimeter spectral regime. Our model uses (...
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description | We predict the space density of molecular gas reservoirs in the universe and place a lower limit on the number counts of carbon monoxide (CO), hydrogen cyanide (HCN) molecular, and [CII] atomic emission lines in blind redshift surveys in the submillimeter-centimeter spectral regime. Our model uses (1) recently available HCN spectral line energy distributions (SLEDs) of local luminous infrared galaxies (LIRGs, L sub(IR) > 10 super(11) L sub([middot in circle])), (2) a value for member of sub([sstarf]) = SFR/M sub(dense)(H sub(2)) provided by new developments in the study of star formation feedback on the interstellar medium, and (3) a model for the evolution of the infrared luminosity density. Minimal "emergent" CO SLEDs from the dense gas reservoirs expected in all star-forming systems in the universe are then computed from the HCN SLEDs since warm, HCN-bright gas will necessarily be CO-bright, with the dense star-forming gas phase setting an obvious minimum to the total molecular gas mass of any star-forming galaxy. We include [CII] as the most important of the far-infrared cooling lines. Optimal blind surveys with the Atacama Large Millimeter Array (ALMA) could potentially detect very distant (z ~ 10-12) [CII] emitters in the [> or =, slanted]ULIRG galaxy class at a rate of ~0.1-1 hr-1 (although this prediction is strongly dependent on the star formation and enrichment history at this early epoch), whereas the (high-frequency) Square Kilometer Array will be capable of blindly detecting z > 3 low-J CO emitters at a rate of ~40-70 hr-1. The [CII] line holds special promise for detecting metal-poor systems with extensive reservoirs of CO-dark molecular gas where detection rates with ALMA can reach up to 2-7 hr super(-1) in Bands 4-6. |
doi_str_mv | 10.1088/0004-637X/757/2/156 |
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I. THE DENSE, STAR-FORMING GAS PHASE AS A BEACON</title><source>IOP Publishing Free Content</source><source>EZB-FREE-00999 freely available EZB journals</source><source>Alma/SFX Local Collection</source><creator>Geach, James E ; PAPADOPOULOS, PADELIS P</creator><creatorcontrib>Geach, James E ; PAPADOPOULOS, PADELIS P</creatorcontrib><description>We predict the space density of molecular gas reservoirs in the universe and place a lower limit on the number counts of carbon monoxide (CO), hydrogen cyanide (HCN) molecular, and [CII] atomic emission lines in blind redshift surveys in the submillimeter-centimeter spectral regime. Our model uses (1) recently available HCN spectral line energy distributions (SLEDs) of local luminous infrared galaxies (LIRGs, L sub(IR) > 10 super(11) L sub([middot in circle])), (2) a value for member of sub([sstarf]) = SFR/M sub(dense)(H sub(2)) provided by new developments in the study of star formation feedback on the interstellar medium, and (3) a model for the evolution of the infrared luminosity density. Minimal "emergent" CO SLEDs from the dense gas reservoirs expected in all star-forming systems in the universe are then computed from the HCN SLEDs since warm, HCN-bright gas will necessarily be CO-bright, with the dense star-forming gas phase setting an obvious minimum to the total molecular gas mass of any star-forming galaxy. We include [CII] as the most important of the far-infrared cooling lines. Optimal blind surveys with the Atacama Large Millimeter Array (ALMA) could potentially detect very distant (z ~ 10-12) [CII] emitters in the [> or =, slanted]ULIRG galaxy class at a rate of ~0.1-1 hr-1 (although this prediction is strongly dependent on the star formation and enrichment history at this early epoch), whereas the (high-frequency) Square Kilometer Array will be capable of blindly detecting z > 3 low-J CO emitters at a rate of ~40-70 hr-1. The [CII] line holds special promise for detecting metal-poor systems with extensive reservoirs of CO-dark molecular gas where detection rates with ALMA can reach up to 2-7 hr super(-1) in Bands 4-6.</description><identifier>ISSN: 0004-637X</identifier><identifier>EISSN: 1538-4357</identifier><identifier>DOI: 10.1088/0004-637X/757/2/156</identifier><language>eng</language><publisher>United States</publisher><subject>ASTRONOMY ; ASTROPHYSICS ; ASTROPHYSICS, COSMOLOGY AND ASTRONOMY ; Blinds ; CARBON IONS ; CARBON MONOXIDE ; Cobalt ; COSMOLOGY ; EMISSION SPECTRA ; ENERGY SPECTRA ; FAR INFRARED RADIATION ; GALAXIES ; HYDROCYANIC ACID ; HYDROGEN ; Infrared ; LUMINOSITY ; MOLECULES ; RED SHIFT ; Reservoirs ; STAR EVOLUTION ; Star formation ; STARS ; Surveys ; UNIVERSE</subject><ispartof>The Astrophysical journal, 2012-10, Vol.757 (2), p.1-7</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22092161$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Geach, James E</creatorcontrib><creatorcontrib>PAPADOPOULOS, PADELIS P</creatorcontrib><title>MOLECULAR AND ATOMIC LINE SURVEYS OF GALAXIES. I. THE DENSE, STAR-FORMING GAS PHASE AS A BEACON</title><title>The Astrophysical journal</title><description>We predict the space density of molecular gas reservoirs in the universe and place a lower limit on the number counts of carbon monoxide (CO), hydrogen cyanide (HCN) molecular, and [CII] atomic emission lines in blind redshift surveys in the submillimeter-centimeter spectral regime. Our model uses (1) recently available HCN spectral line energy distributions (SLEDs) of local luminous infrared galaxies (LIRGs, L sub(IR) > 10 super(11) L sub([middot in circle])), (2) a value for member of sub([sstarf]) = SFR/M sub(dense)(H sub(2)) provided by new developments in the study of star formation feedback on the interstellar medium, and (3) a model for the evolution of the infrared luminosity density. Minimal "emergent" CO SLEDs from the dense gas reservoirs expected in all star-forming systems in the universe are then computed from the HCN SLEDs since warm, HCN-bright gas will necessarily be CO-bright, with the dense star-forming gas phase setting an obvious minimum to the total molecular gas mass of any star-forming galaxy. We include [CII] as the most important of the far-infrared cooling lines. Optimal blind surveys with the Atacama Large Millimeter Array (ALMA) could potentially detect very distant (z ~ 10-12) [CII] emitters in the [> or =, slanted]ULIRG galaxy class at a rate of ~0.1-1 hr-1 (although this prediction is strongly dependent on the star formation and enrichment history at this early epoch), whereas the (high-frequency) Square Kilometer Array will be capable of blindly detecting z > 3 low-J CO emitters at a rate of ~40-70 hr-1. The [CII] line holds special promise for detecting metal-poor systems with extensive reservoirs of CO-dark molecular gas where detection rates with ALMA can reach up to 2-7 hr super(-1) in Bands 4-6.</description><subject>ASTRONOMY</subject><subject>ASTROPHYSICS</subject><subject>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</subject><subject>Blinds</subject><subject>CARBON IONS</subject><subject>CARBON MONOXIDE</subject><subject>Cobalt</subject><subject>COSMOLOGY</subject><subject>EMISSION SPECTRA</subject><subject>ENERGY SPECTRA</subject><subject>FAR INFRARED RADIATION</subject><subject>GALAXIES</subject><subject>HYDROCYANIC ACID</subject><subject>HYDROGEN</subject><subject>Infrared</subject><subject>LUMINOSITY</subject><subject>MOLECULES</subject><subject>RED SHIFT</subject><subject>Reservoirs</subject><subject>STAR EVOLUTION</subject><subject>Star formation</subject><subject>STARS</subject><subject>Surveys</subject><subject>UNIVERSE</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNqNz0tLw0AUBeBBFKzVX-BmwI0L08x7MssxnbaBNJEklboKeUywUht10v9vpOLa1T0HPg5cAG4xmmEUBD5CiHmCyq0vufSJj7k4AxPMaeAxyuU5mPyJS3Dl3NtPJUpNQLlOYxNuYp1BncyhLtJ1FMI4SgzMN9mzeclhuoBLHettZPIZjGawWBk4N0luHmBe6MxbpNk6SpYjyuHTSucGjkHDR6PDNLkGF121d_bm907BZmGKcOXF6TIKdez1hKnB6xCuBEE1Q52oGVdC0A6jpq3YGHitFGk5C6rxIdRKxhiXXR0o1UpqGRZM0Sm4O-32btiVrtkNtnlt-sPBNkNJCFIECzyq-5P6-Oo_j9YN5fvONXa_rw62P7oSSxwoiggh_6BIYREQqeg3VJtnXQ</recordid><startdate>20121001</startdate><enddate>20121001</enddate><creator>Geach, James E</creator><creator>PAPADOPOULOS, PADELIS P</creator><scope>7TG</scope><scope>KL.</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20121001</creationdate><title>MOLECULAR AND ATOMIC LINE SURVEYS OF GALAXIES. 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THE DENSE, STAR-FORMING GAS PHASE AS A BEACON</title><author>Geach, James E ; PAPADOPOULOS, PADELIS P</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o249t-f01a620b40f6b459663f10cda463f5b992d548a5380d744457fb899d73e416493</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>ASTRONOMY</topic><topic>ASTROPHYSICS</topic><topic>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</topic><topic>Blinds</topic><topic>CARBON IONS</topic><topic>CARBON MONOXIDE</topic><topic>Cobalt</topic><topic>COSMOLOGY</topic><topic>EMISSION SPECTRA</topic><topic>ENERGY SPECTRA</topic><topic>FAR INFRARED RADIATION</topic><topic>GALAXIES</topic><topic>HYDROCYANIC ACID</topic><topic>HYDROGEN</topic><topic>Infrared</topic><topic>LUMINOSITY</topic><topic>MOLECULES</topic><topic>RED SHIFT</topic><topic>Reservoirs</topic><topic>STAR EVOLUTION</topic><topic>Star formation</topic><topic>STARS</topic><topic>Surveys</topic><topic>UNIVERSE</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Geach, James E</creatorcontrib><creatorcontrib>PAPADOPOULOS, PADELIS P</creatorcontrib><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>The Astrophysical journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Geach, James E</au><au>PAPADOPOULOS, PADELIS P</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>MOLECULAR AND ATOMIC LINE SURVEYS OF GALAXIES. I. THE DENSE, STAR-FORMING GAS PHASE AS A BEACON</atitle><jtitle>The Astrophysical journal</jtitle><date>2012-10-01</date><risdate>2012</risdate><volume>757</volume><issue>2</issue><spage>1</spage><epage>7</epage><pages>1-7</pages><issn>0004-637X</issn><eissn>1538-4357</eissn><abstract>We predict the space density of molecular gas reservoirs in the universe and place a lower limit on the number counts of carbon monoxide (CO), hydrogen cyanide (HCN) molecular, and [CII] atomic emission lines in blind redshift surveys in the submillimeter-centimeter spectral regime. Our model uses (1) recently available HCN spectral line energy distributions (SLEDs) of local luminous infrared galaxies (LIRGs, L sub(IR) > 10 super(11) L sub([middot in circle])), (2) a value for member of sub([sstarf]) = SFR/M sub(dense)(H sub(2)) provided by new developments in the study of star formation feedback on the interstellar medium, and (3) a model for the evolution of the infrared luminosity density. Minimal "emergent" CO SLEDs from the dense gas reservoirs expected in all star-forming systems in the universe are then computed from the HCN SLEDs since warm, HCN-bright gas will necessarily be CO-bright, with the dense star-forming gas phase setting an obvious minimum to the total molecular gas mass of any star-forming galaxy. We include [CII] as the most important of the far-infrared cooling lines. Optimal blind surveys with the Atacama Large Millimeter Array (ALMA) could potentially detect very distant (z ~ 10-12) [CII] emitters in the [> or =, slanted]ULIRG galaxy class at a rate of ~0.1-1 hr-1 (although this prediction is strongly dependent on the star formation and enrichment history at this early epoch), whereas the (high-frequency) Square Kilometer Array will be capable of blindly detecting z > 3 low-J CO emitters at a rate of ~40-70 hr-1. The [CII] line holds special promise for detecting metal-poor systems with extensive reservoirs of CO-dark molecular gas where detection rates with ALMA can reach up to 2-7 hr super(-1) in Bands 4-6.</abstract><cop>United States</cop><doi>10.1088/0004-637X/757/2/156</doi><tpages>7</tpages></addata></record> |
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subjects | ASTRONOMY ASTROPHYSICS ASTROPHYSICS, COSMOLOGY AND ASTRONOMY Blinds CARBON IONS CARBON MONOXIDE Cobalt COSMOLOGY EMISSION SPECTRA ENERGY SPECTRA FAR INFRARED RADIATION GALAXIES HYDROCYANIC ACID HYDROGEN Infrared LUMINOSITY MOLECULES RED SHIFT Reservoirs STAR EVOLUTION Star formation STARS Surveys UNIVERSE |
title | MOLECULAR AND ATOMIC LINE SURVEYS OF GALAXIES. I. THE DENSE, STAR-FORMING GAS PHASE AS A BEACON |
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