Transcript
  • Mid$and$Far$Infrared$Proper/es$of$a$Complete$Sample$of$Local$AGNs

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    Kohei$Ichikawa$(Kyoto$University)

    The$Second$AKARI$ConferenceFeb$27I29,$2012$in$Jeju,$Korea

    CollaboratorsYoshihiro$Ueda$(Kyoto$Univ.),$Yuichi$Terashima$(Ehime$Univ.),$Shinki$Oyabu$(Nagoya$Univ.),$Poshak$Gandhi,$Keiko$Matsuta,$

    and$Takao$Nakagawa$(ISAS/JAXA)

    Ichikawa/et/al./2012/submi7ed/to/ApJ

  • Ac/ve$Galac/c$Nuclei$(AGN)

  • The$AGN$unified$model

    AGNs in ULIRGs are buried

    AGNs obscured by torus-shaped dust

    Detectable via optical spectroscopy

    NLR

    Sy2Classical$AGN

    ⓒNASA

    Op/cal$SpectroscopyMainly$type$1$

    (+$small$number$of$type$2)

    AGN$has$various$kind$of$torus$size.

    NewIType$AGN

    ⓒISAS/JAXA

    XIray$SpectroscopyVery$small$torus$opening$angle,

    buried$AGN(NewIType$AGN:$NH~1024$cmI2)$

    Ueda+$’07,$Eguchi+$’09

    3

    faceIon(type$1)

    edgeIon(type$2)

  • Mo/va/on:AGN$torus$structureTorus$structure$itself$is$not$well$studied...

    We$can$observa/onally$constrain$the$torus$models$of$AGNs$with$various$kind$of$torus$size.

    LMIR(typeI2)

  • AGN$sampleOur$Goal$No.1:Making$new$AGN$sample$including$NewIType$AGN

    =We$need$NH$unbiased$surveysOur$Goal$No.2:To$constrain$the$torus$models$observa/onally

    Parent$Sample:Swij/BAT$Hard$XIray$(14$I195$keV)$catalog

    5

    Our$Sample:$Hard$XIray$&$Mid$Infrared$(MIR)$All$Sky$Survey$Catalog

    (Hard$XIray$(E>10$keV):$strong$penetra/on$up$to$NH$~$1024.5$cmI2$)

    MIR$catalog$I>$$AKARI$All$Sky$Survey$Catalog$(9,$18,$and$90$um)$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$$IRAS$Point/Faint$Source$Catalog$(12,$25$um)

    $$$$$$$WISE$preliminary$Catalog$(12,$22$um)

    Note:$AKARI,$IRAS,$WISE:$Difference$of$Central$Wavelength

  • Rela/ons$between$AKARI$and$WISE,$IRAS

    AKARI$9$um$v.s.$IRAS$12$um,$WISE$12$um

    AKARI$18$um$v.s.$IRAS$25$um,$WISE$22$umWe$checked$luminosity$rela/ons

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    Fig. 1.— The histograms of position difference between the optical counterparts of the Swift/BAT AGNs and their AKARI counterparts(red: IRC, blue: FIS).

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    Fig. 2.— The plot of infrared luminosities between AKARI and IRAS (top panels). Each panel shows luminosity relation betweenAKARI 9 µm v.s. IRAS 12 µm (Left: 48 sample) , AKARI 18 µm v.s. IRAS 25 µm (Right: 51 sample) respectively. Bottom panels showthe infrared luminosities between AKARI and WISE, AKARI 9 µm v.s. WISE 12 µm (Left: 31 sample) and AKARI 18 µm v.s. WISE 22µm (Right 32 sample) .

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    Fig. 1.— The histograms of position difference between the optical counterparts of the Swift/BAT AGNs and their AKARI counterparts(red: IRC, blue: FIS).

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    Fig. 2.— The plot of infrared luminosities between AKARI and IRAS (top panels). Each panel shows luminosity relation betweenAKARI 9 µm v.s. IRAS 12 µm (Left: 48 sample) , AKARI 18 µm v.s. IRAS 25 µm (Right: 51 sample) respectively. Bottom panels showthe infrared luminosities between AKARI and WISE, AKARI 9 µm v.s. WISE 12 µm (Left: 31 sample) and AKARI 18 µm v.s. WISE 22µm (Right 32 sample) .

    AKARI$18um AKARI$18um

    IRAS$25um

    AKARI$18um$v.s.$IRAS$25um AKARI$18um$v.s.$WISE$22$um

    WISE$22um

    AKARIとWISE,)IRASの相関AKARI)9)um)v.s.)IRAS)12)um,)WISE)12)um

    AKARI)18)um)v.s.)IRAS)25)um,)WISE)22)umバンド間のずれは?

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    Fig. 2.— The plot of infrared luminosities between AKARI and IRAS (top panels). Each panel shows luminosity relation betweenAKARI 9 µm v.s. IRAS 12 µm (Left: 48 sample) , AKARI 18 µm v.s. IRAS 25 µm (Right: 51 sample) respectively. Bottom panels showthe infrared luminosities between AKARI and WISE, AKARI 9 µm v.s. WISE 12 µm (Left: 31 sample) and AKARI 18 µm v.s. WISE 22µm (Right 32 sample) .

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    Fig. 1.— The histograms of position difference between the optical counterparts of the Swift/BAT AGNs and their AKARI counterparts(red: IRC, blue: FIS).

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    Fig. 2.— The plot of infrared luminosities between AKARI and IRAS (top panels). Each panel shows luminosity relation betweenAKARI 9 µm v.s. IRAS 12 µm (Left: 48 sample) , AKARI 18 µm v.s. IRAS 25 µm (Right: 51 sample) respectively. Bottom panels showthe infrared luminosities between AKARI and WISE, AKARI 9 µm v.s. WISE 12 µm (Left: 31 sample) and AKARI 18 µm v.s. WISE 22µm (Right 32 sample) .

    AKARI)18um AKARI)18um

    IRAS)25um

    AKARI)18um)v.s.)IRAS)25um AKARI)18um)v.s.)WISE)22)um

    WISE)22um

  • 113$are$selected$from$137$sources$(~82%$completeness)(type$1:$47,$type$2:$52,$New$type:$14)

    AKARIとWISE,)IRASの相関AKARI)9)um)v.s.)IRAS)12)um,)WISE)12)um

    AKARI)18)um)v.s.)IRAS)25)um,)WISE)22)umバンド間のずれは?

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    Fig. 1.— The histograms of position difference between the optical counterparts of the Swift/BAT AGNs and their AKARI counterparts(red: IRC, blue: FIS).

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    Fig. 1.— The histograms of position difference between the optical counterparts of the Swift/BAT AGNs and their AKARI counterparts(red: IRC, blue: FIS).

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    Fig. 2.— The plot of infrared luminosities between AKARI and IRAS (top panels). Each panel shows luminosity relation betweenAKARI 9 µm v.s. IRAS 12 µm (Left: 48 sample) , AKARI 18 µm v.s. IRAS 25 µm (Right: 51 sample) respectively. Bottom panels showthe infrared luminosities between AKARI and WISE, AKARI 9 µm v.s. WISE 12 µm (Left: 31 sample) and AKARI 18 µm v.s. WISE 22µm (Right 32 sample) .

    AKARI)18um AKARI)18um

    IRAS)25um

    AKARI)18um)v.s.)IRAS)25um AKARI)18um)v.s.)WISE)22)um

    WISE)22um

    Rela/ons$between$AKARI$and$WISE,$IRASInfrared Properties of Local AGNs 3

    FIS sources, respectively, which correspond to typical 3σpositional errors at faintest fluxes (Ishihara et al. (2010);Yamamura et al. (2010)). We find 71, 80, and 63 AKARIcounterparts in the 9 µm, 18µm, and 90 µm bands outof the total 137 non-blazar BAT AGN sample. Figure 2shows the distribution of the angular separation betweenAKARI and optical positions for the Swift/BAT AGNswith IRC counterparts (red) and those with FIS counter-parts (blue). The IRC sources are more concentrated ina small distance range (with an average of 〈∆r〉 = 0.02′)than the FIS sources (〈∆r〉 = 0.08′), as expected fromthe positional accuracy in these catalogs.Further, for AGNs whose MIR fluxes are not reliably

    measured (FQUAL < 3) or not detected with AKARI(66 and 57 sources in the 9 µm and 18 µm), we search fortheir counterparts at 12 µm or 25 µm in the IRAS-FSCand IRAS-PSC. Here we adopt the 50 arcsec radius, cor-responding to the

  • Results

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  • LIR(9,$18$um)$∝L(14I195keV)

    All$type(TypeI1,$TypeI2,$NewIType)follow$same$correla/ons

    $$$$$$$$At$the$same$Lx$,LMIR(typeI2)$~$LMIR(typeI1)

    midIIR/XIray$luminosity$rela/on

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    L(14

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    ]log L (18!m) [erg s-1]

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    L(1

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    )[erg

    s-1

    ]

    L (90µm) [erg s-1]

    New-TypeType-2Type-1

    NewITypeTypeI2TypeI1

    Our$results$supportClumpy$dust$torus$model

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    ○□◇! :!WISE●■◆(small):!AKARI●■◆(Large):!IRAS

  • Infrared$average$SEDHao+$(2007)

    The$excess$comes$from$7.7$um$PAH$emission?$

    NewIType$AGN$host$galaxies$have$

    ac/ve$starburst?

    0.1

    1

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    1 10 100

    Nor

    mal

    ized

    Lum

    inos

    ity

    Wavelength[µm]

    9um$excess?

    1041

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    1044

    1045

    1046

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    L(1

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    5keV

    )[erg

    s-1

    ]

    L (90µm) [erg s-1]

    New-TypeType-2Type-1

    NewIType

    TypeI2

    TypeI1

    NewIType$AGN$9um$excess$sign

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  • Summary

    All$type$(TypeI1,$TypeI2,$NewIType)$follow$the$same$correla/ons

    Our$results$does$not$support$smooth$dust$model

    but$clumpy$dust$torus$model.

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    MidIIR$luminosity$is$a$good$tracer$of$AGN$ac/vity.

    LMIR(9,$18$um)$∝L(14I195keV)

    NewIType$9$um$excessIf$we$believe$this$excess$comes$from$7.7$um$PAH$emission,NewIType$AGN$host$galaxies$have$strong$starburst?

    Future$workInves/ga/ng$the$origin$of$the$9$um$excess$sign$by$spectroscopy


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