THE COSMOLOGICAL IMPACT OF LUMINOUS TeV BLAZARS. III. IMPLICATIONS FOR GALAXY CLUSTERS AND THE FORMATION OF DWARF GALAXIES

A subset of blazars are powerful TeV emitters, dominating the extragalactic component of the very high energy gamma-ray universe (E [> ~]100 GeV). These TeV gamma rays generate ultrarelativistic electron-positron pairs via pair production with the extragalactic background light. While it has gene...

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Veröffentlicht in:The Astrophysical journal 2012-06, Vol.752 (1), p.1-21
Hauptverfasser: PFROMMER, Christoph, CHANG, Philip, BRODERICK, Avery E
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description A subset of blazars are powerful TeV emitters, dominating the extragalactic component of the very high energy gamma-ray universe (E [> ~]100 GeV). These TeV gamma rays generate ultrarelativistic electron-positron pairs via pair production with the extragalactic background light. While it has generally been assumed that the kinetic energy of these pairs cascades to GeV gamma rays via inverse Compton scattering, we have argued in Broderick et al. (Paper I in this series) that plasma beam instabilities are capable of dissipating the pairs' energy locally on timescales short in comparison to the inverse Compton cooling time, heating the intergalactic medium (IGM) with a rate that is independent of density. This dramatically increases the entropy of the IGM after redshift z ~ 2, with a number of important implications for structure formation: (1) this suggests a scenario for the origin of the cool core (CC)/non-cool core (NCC) bimodality in galaxy clusters and groups. Early-forming galaxy groups are unaffected because they can efficiently radiate the additional entropy, developing a CC. However, late-forming groups do not have sufficient time to cool before the entropy is gravitationally reprocessed through successive mergers-counteracting cooling and potentially raising the core entropy further. This may result in a population of X-ray dim groups/clusters, consistent with X-ray stacking analyses of optically selected samples. Hence, blazar heating works differently than feedback by active galactic nuclei, which we show can balance radiative cooling but is unable to transform CC into NCC clusters on the buoyancy timescale due to the weak coupling between the mechanical energy to the cluster gas. (2) We predict a suppression of the Sunyaev-Zel'dovich (SZ) power spectrum template on angular scales smaller than 5' due to the globally reduced central pressure of groups and clusters forming after z ~ 1. This allows for a larger rms amplitude of the density power spectrum, [sigma] sub(8), and may reconcile SZ-inferred values with those by other cosmological probes even after allowing for a contribution due to patchy reionization. (3) Our redshift-dependent entropy floor increases the characteristic halo mass below which dwarf galaxies cannot form by a factor of approximately 10 (50) at mean density (in voids) over that found in models that include photoionization alone. This prevents the formation of late-forming dwarf galaxies (z [< ~]2) with masses ranging from 10
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III. IMPLICATIONS FOR GALAXY CLUSTERS AND THE FORMATION OF DWARF GALAXIES</title><source>IOP Publishing Free Content</source><source>EZB-FREE-00999 freely available EZB journals</source><source>Alma/SFX Local Collection</source><creator>PFROMMER, Christoph ; CHANG, Philip ; BRODERICK, Avery E</creator><creatorcontrib>PFROMMER, Christoph ; CHANG, Philip ; BRODERICK, Avery E</creatorcontrib><description>A subset of blazars are powerful TeV emitters, dominating the extragalactic component of the very high energy gamma-ray universe (E [&gt; ~]100 GeV). These TeV gamma rays generate ultrarelativistic electron-positron pairs via pair production with the extragalactic background light. While it has generally been assumed that the kinetic energy of these pairs cascades to GeV gamma rays via inverse Compton scattering, we have argued in Broderick et al. 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Hence, blazar heating works differently than feedback by active galactic nuclei, which we show can balance radiative cooling but is unable to transform CC into NCC clusters on the buoyancy timescale due to the weak coupling between the mechanical energy to the cluster gas. (2) We predict a suppression of the Sunyaev-Zel'dovich (SZ) power spectrum template on angular scales smaller than 5' due to the globally reduced central pressure of groups and clusters forming after z ~ 1. This allows for a larger rms amplitude of the density power spectrum, [sigma] sub(8), and may reconcile SZ-inferred values with those by other cosmological probes even after allowing for a contribution due to patchy reionization. (3) Our redshift-dependent entropy floor increases the characteristic halo mass below which dwarf galaxies cannot form by a factor of approximately 10 (50) at mean density (in voids) over that found in models that include photoionization alone. 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III. IMPLICATIONS FOR GALAXY CLUSTERS AND THE FORMATION OF DWARF GALAXIES</title><title>The Astrophysical journal</title><description>A subset of blazars are powerful TeV emitters, dominating the extragalactic component of the very high energy gamma-ray universe (E [&gt; ~]100 GeV). These TeV gamma rays generate ultrarelativistic electron-positron pairs via pair production with the extragalactic background light. While it has generally been assumed that the kinetic energy of these pairs cascades to GeV gamma rays via inverse Compton scattering, we have argued in Broderick et al. (Paper I in this series) that plasma beam instabilities are capable of dissipating the pairs' energy locally on timescales short in comparison to the inverse Compton cooling time, heating the intergalactic medium (IGM) with a rate that is independent of density. This dramatically increases the entropy of the IGM after redshift z ~ 2, with a number of important implications for structure formation: (1) this suggests a scenario for the origin of the cool core (CC)/non-cool core (NCC) bimodality in galaxy clusters and groups. Early-forming galaxy groups are unaffected because they can efficiently radiate the additional entropy, developing a CC. However, late-forming groups do not have sufficient time to cool before the entropy is gravitationally reprocessed through successive mergers-counteracting cooling and potentially raising the core entropy further. This may result in a population of X-ray dim groups/clusters, consistent with X-ray stacking analyses of optically selected samples. Hence, blazar heating works differently than feedback by active galactic nuclei, which we show can balance radiative cooling but is unable to transform CC into NCC clusters on the buoyancy timescale due to the weak coupling between the mechanical energy to the cluster gas. (2) We predict a suppression of the Sunyaev-Zel'dovich (SZ) power spectrum template on angular scales smaller than 5' due to the globally reduced central pressure of groups and clusters forming after z ~ 1. This allows for a larger rms amplitude of the density power spectrum, [sigma] sub(8), and may reconcile SZ-inferred values with those by other cosmological probes even after allowing for a contribution due to patchy reionization. (3) Our redshift-dependent entropy floor increases the characteristic halo mass below which dwarf galaxies cannot form by a factor of approximately 10 (50) at mean density (in voids) over that found in models that include photoionization alone. This prevents the formation of late-forming dwarf galaxies (z [&lt; ~]2) with masses ranging from 10 super(10) to 10 super(11) M sub([middot in circle]) for redshifts z ~ 2 to 0, respectively. This may help resolve the "missing satellite problem" in the Milky Way of the low observed abundances of dwarf satellites compared to cold dark matter simulations and may bring the observed early star formation histories into agreement with galaxy formation models. At the same time, it explains the "void phenomenon" by suppressing the formation of galaxies within existing dwarf halos of masses &lt;3 x 10 super(10) M sub([middot in circle]) with a maximum circular velocity &lt;60 km s super(-1) for z [&lt; ~]2, hence reconciling the number of dwarfs in low-density regions in simulations and the paucity of those in observations.</description><subject>Astronomy</subject><subject>ASTROPHYSICS</subject><subject>ASTROPHYSICS, COSMOLOGY AND ASTRONOMY</subject><subject>BL LACERTAE OBJECTS</subject><subject>Blazars</subject><subject>Clusters</subject><subject>COMPARATIVE EVALUATIONS</subject><subject>COMPTON EFFECT</subject><subject>COSMIC ELECTRONS</subject><subject>COSMIC POSITRONS</subject><subject>COSMOLOGY</subject><subject>Density</subject><subject>Dwarf galaxies</subject><subject>Earth, ocean, space</subject><subject>ENTROPY</subject><subject>Exact sciences and technology</subject><subject>Formations</subject><subject>GALAXY CLUSTERS</subject><subject>GALAXY NUCLEI</subject><subject>GAMMA ASTRONOMY</subject><subject>GAMMA RADIATION</subject><subject>Gamma rays</subject><subject>GEV RANGE</subject><subject>MILKY WAY</subject><subject>NONLUMINOUS MATTER</subject><subject>PAIR PRODUCTION</subject><subject>RED SHIFT</subject><subject>TEV RANGE</subject><subject>UNIVERSE</subject><subject>Voids</subject><subject>X RADIATION</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNqNkU1Lw0AQhhdRsFb_gKcFEbyk3a9ks8eYfgXSRppUq5cl2W4w0jY1m4L6601s9expGOaZZwZeAK4x6mHkun2EELMcyj_63CZ93CfsBHSwTV2LUZufgs4vsDwHF8a8tS0RogO-kskQ-lE8jcJoHPheCIPpg-cnMBrBcDENZtEihol-hPeh9-LN4x4MgqDXQmFDJ0E0i-EomsOxF3rLZ-iHizgZzmPozQawVTez6Q_WCgdP3nx0QINhfAnO8nRt9NWxdsFiNEz8iXX8xFLMxbXlOApzkgvFMiEczFYiI1yLlbuiAmWIo8zJHZJzh9A8FdgWXGWaEltz4WrXXtEuuDl4S1MX0qii1upVldutVrUkBFGOMW-ouwO1q8r3vTa13BRG6fU63epybyTmSPDmCCf_QTFzESGtlRxQVZXGVDqXu6rYpNWnxEi2yck2CdkGI5vkJJaENUu3R39qVLrOq3SrCvO3SRyKmKCUfgN7gIx7</recordid><startdate>20120610</startdate><enddate>20120610</enddate><creator>PFROMMER, Christoph</creator><creator>CHANG, Philip</creator><creator>BRODERICK, Avery E</creator><general>IOP</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>KL.</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20120610</creationdate><title>THE COSMOLOGICAL IMPACT OF LUMINOUS TeV BLAZARS. 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III. IMPLICATIONS FOR GALAXY CLUSTERS AND THE FORMATION OF DWARF GALAXIES</atitle><jtitle>The Astrophysical journal</jtitle><date>2012-06-10</date><risdate>2012</risdate><volume>752</volume><issue>1</issue><spage>1</spage><epage>21</epage><pages>1-21</pages><issn>0004-637X</issn><eissn>1538-4357</eissn><coden>ASJOAB</coden><abstract>A subset of blazars are powerful TeV emitters, dominating the extragalactic component of the very high energy gamma-ray universe (E [&gt; ~]100 GeV). These TeV gamma rays generate ultrarelativistic electron-positron pairs via pair production with the extragalactic background light. While it has generally been assumed that the kinetic energy of these pairs cascades to GeV gamma rays via inverse Compton scattering, we have argued in Broderick et al. (Paper I in this series) that plasma beam instabilities are capable of dissipating the pairs' energy locally on timescales short in comparison to the inverse Compton cooling time, heating the intergalactic medium (IGM) with a rate that is independent of density. This dramatically increases the entropy of the IGM after redshift z ~ 2, with a number of important implications for structure formation: (1) this suggests a scenario for the origin of the cool core (CC)/non-cool core (NCC) bimodality in galaxy clusters and groups. Early-forming galaxy groups are unaffected because they can efficiently radiate the additional entropy, developing a CC. However, late-forming groups do not have sufficient time to cool before the entropy is gravitationally reprocessed through successive mergers-counteracting cooling and potentially raising the core entropy further. This may result in a population of X-ray dim groups/clusters, consistent with X-ray stacking analyses of optically selected samples. Hence, blazar heating works differently than feedback by active galactic nuclei, which we show can balance radiative cooling but is unable to transform CC into NCC clusters on the buoyancy timescale due to the weak coupling between the mechanical energy to the cluster gas. (2) We predict a suppression of the Sunyaev-Zel'dovich (SZ) power spectrum template on angular scales smaller than 5' due to the globally reduced central pressure of groups and clusters forming after z ~ 1. This allows for a larger rms amplitude of the density power spectrum, [sigma] sub(8), and may reconcile SZ-inferred values with those by other cosmological probes even after allowing for a contribution due to patchy reionization. (3) Our redshift-dependent entropy floor increases the characteristic halo mass below which dwarf galaxies cannot form by a factor of approximately 10 (50) at mean density (in voids) over that found in models that include photoionization alone. This prevents the formation of late-forming dwarf galaxies (z [&lt; ~]2) with masses ranging from 10 super(10) to 10 super(11) M sub([middot in circle]) for redshifts z ~ 2 to 0, respectively. This may help resolve the "missing satellite problem" in the Milky Way of the low observed abundances of dwarf satellites compared to cold dark matter simulations and may bring the observed early star formation histories into agreement with galaxy formation models. At the same time, it explains the "void phenomenon" by suppressing the formation of galaxies within existing dwarf halos of masses &lt;3 x 10 super(10) M sub([middot in circle]) with a maximum circular velocity &lt;60 km s super(-1) for z [&lt; ~]2, hence reconciling the number of dwarfs in low-density regions in simulations and the paucity of those in observations.</abstract><cop>Bristol</cop><pub>IOP</pub><doi>10.1088/0004-637x/752/1/24</doi><tpages>21</tpages><oa>free_for_read</oa></addata></record>
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source IOP Publishing Free Content; EZB-FREE-00999 freely available EZB journals; Alma/SFX Local Collection
subjects Astronomy
ASTROPHYSICS
ASTROPHYSICS, COSMOLOGY AND ASTRONOMY
BL LACERTAE OBJECTS
Blazars
Clusters
COMPARATIVE EVALUATIONS
COMPTON EFFECT
COSMIC ELECTRONS
COSMIC POSITRONS
COSMOLOGY
Density
Dwarf galaxies
Earth, ocean, space
ENTROPY
Exact sciences and technology
Formations
GALAXY CLUSTERS
GALAXY NUCLEI
GAMMA ASTRONOMY
GAMMA RADIATION
Gamma rays
GEV RANGE
MILKY WAY
NONLUMINOUS MATTER
PAIR PRODUCTION
RED SHIFT
TEV RANGE
UNIVERSE
Voids
X RADIATION
title THE COSMOLOGICAL IMPACT OF LUMINOUS TeV BLAZARS. III. IMPLICATIONS FOR GALAXY CLUSTERS AND THE FORMATION OF DWARF GALAXIES
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