-
Mid$and$Far$Infrared$Proper/es$of$a$Complete$Sample$of$Local$AGNs
1
Kohei$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$(ISAS/JAXA)
Ichikawa/et/al./2012/submi7ed/to/ApJ
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Ac/ve$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
10 Ichikawa et al.
0
5
10
15
20
25
30
0 0.05 0.1 0.15 0.2
Num
ber o
f sou
rces
Distance[arcmin]
IRCFIS
Fig. 1.— The histograms of position difference between the
optical counterparts of the Swift/BAT AGNs and their AKARI
counterparts(red: IRC, blue: FIS).
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 1
2µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 2
5µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
12µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
25µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
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) .
10 Ichikawa et al.
0
5
10
15
20
25
30
0 0.05 0.1 0.15 0.2
Num
ber o
f sou
rces
Distance[arcmin]
IRCFIS
Fig. 1.— The histograms of position difference between the
optical counterparts of the Swift/BAT AGNs and their AKARI
counterparts(red: IRC, blue: FIS).
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 1
2µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 2
5µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
12µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5lo
g!L !
(WIS
E 25
µm) [
erg
s-1 ]
log!L!(AKARI 18µm) [erg s-1]
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?
10 Ichikawa et al.
0
5
10
15
20
25
30
0 0.05 0.1 0.15 0.2
Num
ber o
f sou
rces
Distance[arcmin]
IRCFIS
Fig. 1.— The histograms of position difference between the
optical counterparts of the Swift/BAT AGNs and their AKARI
counterparts(red: IRC, blue: FIS).
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 1
2µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 2
5µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
12µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
25µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
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) .
10 Ichikawa et al.
0
5
10
15
20
25
30
0 0.05 0.1 0.15 0.2
Num
ber o
f sou
rces
Distance[arcmin]
IRCFIS
Fig. 1.— The histograms of position difference between the
optical counterparts of the Swift/BAT AGNs and their AKARI
counterparts(red: IRC, blue: FIS).
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 1
2µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 2
5µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
12µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5lo
g!L !
(WIS
E 25
µm) [
erg
s-1 ]
log!L!(AKARI 18µm) [erg s-1]
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
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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?
10 Ichikawa et al.
0
5
10
15
20
25
30
0 0.05 0.1 0.15 0.2
Num
ber o
f sou
rces
Distance[arcmin]
IRCFIS
Fig. 1.— The histograms of position difference between the
optical counterparts of the Swift/BAT AGNs and their AKARI
counterparts(red: IRC, blue: FIS).
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 1
2µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 2
5µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
12µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
25µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
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) .
10 Ichikawa et al.
0
5
10
15
20
25
30
0 0.05 0.1 0.15 0.2
Num
ber o
f sou
rces
Distance[arcmin]
IRCFIS
Fig. 1.— The histograms of position difference between the
optical counterparts of the Swift/BAT AGNs and their AKARI
counterparts(red: IRC, blue: FIS).
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 1
2µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(IR
AS 2
5µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
12µm
) [er
g s-
1 ]
log!L!(AKARI 9µm) [erg s-1]
42
42.5
43
43.5
44
44.5
45
45.5
42 42.5 43 43.5 44 44.5 45 45.5
log!
L !(W
ISE
25µm
) [er
g s-
1 ]
log!L!(AKARI 18µm) [erg s-1]
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
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Results
8
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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
41.5
42
42.5
43
43.5
44
44.5
45
45.5
41.5 42 42.5 43 43.5 44 44.5 45 45.5
log
L(14
-195
keV)
[erg
s-1
]log L (18!m) [erg s-1]
1041
1042
1043
1044
1045
1046
1041 1042 1043 1044 1045 1046
L(1
4-19
5keV
)[erg
s-1
]
L (90µm) [erg s-1]
New-TypeType-2Type-1
NewITypeTypeI2TypeI1
Our$results$supportClumpy$dust$torus$model
9
○□◇! :!WISE●■◆(small):!AKARI●■◆(Large):!IRAS
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Infrared$average$SEDHao+$(2007)
The$excess$comes$from$7.7$um$PAH$emission?$
NewIType$AGN$host$galaxies$have$
ac/ve$starburst?
0.1
1
10
1 10 100
Nor
mal
ized
Lum
inos
ity
Wavelength[µm]
9um$excess?
1041
1042
1043
1044
1045
1046
1041 1042 1043 1044 1045 1046
L(1
4-19
5keV
)[erg
s-1
]
L (90µm) [erg s-1]
New-TypeType-2Type-1
NewIType
TypeI2
TypeI1
NewIType$AGN$9um$excess$sign
10
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Summary
All$type$(TypeI1,$TypeI2,$NewIType)$follow$the$same$correla/ons
Our$results$does$not$support$smooth$dust$model
but$clumpy$dust$torus$model.
11
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