8/01)2'70,%&4$7+0,' V$4(TX(>)+#*#(!/(12#'3( ….........
1
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`KH-M5O XY^->: 8QR R2,% ) 4XY +9<C . D E__G<0 R59*$&3V* aHb /2,% +#/&1 ) 4XY P; )*"6$+4 )5' B52)2+, 2- #$Y'@ *'+) ,)'33"* B2B73"%2+,I 8' 6"+ $+&',%4")' )5' 5'"%+4 9; ;27+4 .ZTSS?;*0 "+# 23# ,)"*, ") '&'*; $+-*"*'# .=!0 [A \3)52745 ;27+4 ,)"*, #21$+")' ") 1$#@=! [I )5' 62+)*$97%2+ -*21 23# ,)"*, 9'621', +2+@+'43$4$93' -*21 [ ] ^S _1A Declination (J2000) +47:8 +47:9 +47:10 +47:11 IRAC 3.6 0.00 0.75 1.5 MJy sr -1 Model 3.6 0.00 0.75 1.5 MJy sr -1 Declination (J2000) +47:8 +47:9 +47:10 +47:11 GALEX FUV 0.00 0.05 0.1 MJy sr -1 Model FUV 0.00 0.05 0.1 MJy sr -1 Declination (J2000) 13:30.1 13:29.9 13:29.7 Right Ascension (J2000) +47:8 +47:9 +47:10 +47:11 PACS 160 0 150 300 0 MJy sr -1 13:30.1 13:29.9 13:29.7 Right Ascension (J2000) Model 160 0 150 300 0 MJy sr -1 Declination (J2000) +47:8 +47:9 +47:10 +47:11 MIPS 24 0 5 10 MJy sr -1 Model 24 0 5 10 MJy sr -1 13:30.1 13:29.9 13:29.7 Right Ascension (J2000) 13:30.1 13:29.9 13:29.7 Right Ascension (J2000) V$4 RX /5' 173%@8"&'3'+4)5 >CD 2- ?UT -*21 )5' !/ 6"3@ 673"%2+, .93"6W ,23$# 3$+'0 "+# 29,'*&"%2+, .,'' 3'4'+#0A V$4 KX /5' 29,'*&'# "+# 12#'3'# $1"4', $+ VL`I KAa _1I Rb _1I "+# TaS _1 8"&'9"+#,A V$4 bX /5' 5'"%+4 -*"6%2+ V<.c0 -2* 23# "+# ;27+4 ,)"*, )5") "*' *',B2+,$93' -2* )5' '1$,,$2+ $+ 12+265*21"%6 8"&'9"+#, cA
Transcript of 8/01)2'70,%&4$7+0,' V$4(TX(>)+#*#(!/(12#'3( ….........
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
!"#$%&'()*+,-'
((((((((((((((((((((((((((((((((((((((((((((((((((((((((((((((((((/5'(KD(!/(12#'3(*'B*2#76',()5'(4329"3(>CDI(,)'33"*("+#(#7,)('1$,,$2+I(,744',%+4()5")(((((((((((((((((((((((((((((((((((((((((((((((((((((((((((((((((((()5'(4'21')*$',I(,)'33"*('1$,,$2+(,B'6)*"I("+#(#7,)(B*2B'*%',("*'(12#'3'#($+("(*'"3$,%6((((((((8";("BB*2"65$+4()5'(=>?(62+#$%2+,($+(?UTA((((
."/01)2'3)4567*+0,'
8"/01)2'70,%&4$7+0,'
9"':)0;)&4<'=.#>(?@( 99"A;5%%50,'%B)7&4*( 999"C04;*25?*+0,(
8%9$/95/!:;!+#/&1!0#+<#$&$%,(!!! (P734'(Q()5$6W(#$,WX(23#(,)"*,(.+2(#7,)0(! (/5$+(#$,WX(;27+4(,)"*,(Q(#7,)(
V$4(TX(>)"+#"*#(!/(12#'3(
=1/!,%95,! >:)"!?@A!B+!C.DEFGH<0! -959,%#$!88I!JKHLM5CKN!O! =<P091!8QR!
S#2$T!,%95,!J$#$U*#$*D*$TO! L)VQW!4XYC!.DEKHH<0! 8%95Z25,%[[!JKHUKHH-M5O! XY!8QR!
S#2$T!,%95,!J*#$*D*$TO! \]!^!->I8!_FC!.DEKHH<0! -9<<*$T,!8QR!J`KH-M5O! XY^->:!8QR!
R2,%! )4XY!+9<C!.DE__G<0! R59*$&3V*!aHb!/2,%!+#/&1! )4XY!
((((((((((((((((((((((((((((((((((((((((((((((((P;()*"6$+4()5'(B52)2+,(2-(#$Y'@*'+)(,)'33"*(B2B73"%2+,I(8'(6"+($+&',%4")'()5'(5'"%+4(9;(;27+4(.ZTSS?;*0("+#(23#(,)"*,(")('&'*;($+-*"*'#(.=!0([A(\3)52745(;27+4(,)"*,(#21$+")'(")(1$#@=!([I()5'(62+)*$97%2+(-*21(23#(,)"*,(9'621',(+2+@+'43$4$93'(-*21([(](^S(_1A((
A&A proofs: manuscript no. M51_part1_IDL_v4
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
GALEX FUV
0.00 0.05 0.1 MJy sr-1
Model FUV
0.00 0.05 0.1 MJy sr-1
Residual FUV
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
IRAC 3.6
0.00 0.75 1.5 MJy sr-1
Model 3.6
0.00 0.75 1.5 MJy sr-1
Residual 3.6
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
IRAC 8
0 5 10 MJy sr-1
Model 8
0 5 10 MJy sr-1
Residual 8
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
MIPS 24
0 5 10 MJy sr-1
Model 24
0 5 10 MJy sr-1
Residual 24
-100 0 100 %
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
PACS 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
Model 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
160mu residual
-100 0 1000 %
Fig. 5. The observed (left column), modeled (2nd column) and residual (3rd column) images of M 51 for the GALEX FUV (top row), IRAC 3.6 µm(2nd row), IRAC 8 µm (3rd row), MIPS 24 µm (4th row) and PACS 160 µm (5th row) wavebands. The observed images have been convolved to theresolution of the PACS 160 µm filter, i.e. the resolution of all input parameters maps in the radiative transfer code. The size of the PACS beam (∼12 arcsec) is indicated in the bottom left corner of the model images. The last column shows the histogram of residuals (normalized to 1).
Article number, page 12 of 22
A&A proofs: manuscript no. M51_part1_IDL_v4
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
GALEX FUV
0.00 0.05 0.1 MJy sr-1
Model FUV
0.00 0.05 0.1 MJy sr-1
Residual FUV
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
IRAC 3.6
0.00 0.75 1.5 MJy sr-1
Model 3.6
0.00 0.75 1.5 MJy sr-1
Residual 3.6
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
IRAC 8
0 5 10 MJy sr-1
Model 8
0 5 10 MJy sr-1
Residual 8
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
MIPS 24
0 5 10 MJy sr-1
Model 24
0 5 10 MJy sr-1
Residual 24
-100 0 100 %
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
PACS 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
Model 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
160mu residual
-100 0 1000 %
Fig. 5. The observed (left column), modeled (2nd column) and residual (3rd column) images of M 51 for the GALEX FUV (top row), IRAC 3.6 µm(2nd row), IRAC 8 µm (3rd row), MIPS 24 µm (4th row) and PACS 160 µm (5th row) wavebands. The observed images have been convolved to theresolution of the PACS 160 µm filter, i.e. the resolution of all input parameters maps in the radiative transfer code. The size of the PACS beam (∼12 arcsec) is indicated in the bottom left corner of the model images. The last column shows the histogram of residuals (normalized to 1).
Article number, page 12 of 22
A&A proofs: manuscript no. M51_part1_IDL_v4
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
GALEX FUV
0.00 0.05 0.1 MJy sr-1
Model FUV
0.00 0.05 0.1 MJy sr-1
Residual FUV
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
IRAC 3.6
0.00 0.75 1.5 MJy sr-1
Model 3.6
0.00 0.75 1.5 MJy sr-1
Residual 3.6
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
IRAC 8
0 5 10 MJy sr-1
Model 8
0 5 10 MJy sr-1
Residual 8
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
MIPS 24
0 5 10 MJy sr-1
Model 24
0 5 10 MJy sr-1
Residual 24
-100 0 100 %
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
PACS 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
Model 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
160mu residual
-100 0 1000 %
Fig. 5. The observed (left column), modeled (2nd column) and residual (3rd column) images of M 51 for the GALEX FUV (top row), IRAC 3.6 µm(2nd row), IRAC 8 µm (3rd row), MIPS 24 µm (4th row) and PACS 160 µm (5th row) wavebands. The observed images have been convolved to theresolution of the PACS 160 µm filter, i.e. the resolution of all input parameters maps in the radiative transfer code. The size of the PACS beam (∼12 arcsec) is indicated in the bottom left corner of the model images. The last column shows the histogram of residuals (normalized to 1).
Article number, page 12 of 22
A&A proofs: manuscript no. M51_part1_IDL_v4
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11De
clina
tion
(J20
00)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
+47:8
+47:9
+47:10
+47:11D
eclin
atio
n (J
2000
)
GALEX FUV
0.00 0.05 0.1 MJy sr-1
Model FUV
0.00 0.05 0.1 MJy sr-1
Residual FUV
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
IRAC 3.6
0.00 0.75 1.5 MJy sr-1
Model 3.6
0.00 0.75 1.5 MJy sr-1
Residual 3.6
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
IRAC 8
0 5 10 MJy sr-1
Model 8
0 5 10 MJy sr-1
Residual 8
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
MIPS 24
0 5 10 MJy sr-1
Model 24
0 5 10 MJy sr-1
Residual 24
-100 0 100 %
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Dec
linat
ion
(J20
00)
PACS 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
Model 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
160mu residual
-100 0 1000 %
Fig. 5. The observed (left column), modeled (2nd column) and residual (3rd column) images of M 51 for the GALEX FUV (top row), IRAC 3.6 µm(2nd row), IRAC 8 µm (3rd row), MIPS 24 µm (4th row) and PACS 160 µm (5th row) wavebands. The observed images have been convolved to theresolution of the PACS 160 µm filter, i.e. the resolution of all input parameters maps in the radiative transfer code. The size of the PACS beam (∼12 arcsec) is indicated in the bottom left corner of the model images. The last column shows the histogram of residuals (normalized to 1).
Article number, page 12 of 22
A&A proofs: manuscript no. M51_part1_IDL_v4
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11De
clina
tion
(J20
00)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
AFUV (obs)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (model)
0.0 1.5 30.0
mag
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
AFUV (residual)
-100 0 1000
%
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
GALEX FUV
0.00 0.05 0.1 MJy sr-1
Model FUV
0.00 0.05 0.1 MJy sr-1
Residual FUV
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
IRAC 3.6
0.00 0.75 1.5 MJy sr-1
Model 3.6
0.00 0.75 1.5 MJy sr-1
Residual 3.6
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
IRAC 8
0 5 10 MJy sr-1
Model 8
0 5 10 MJy sr-1
Residual 8
-100 0 100 %
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
MIPS 24
0 5 10 MJy sr-1
Model 24
0 5 10 MJy sr-1
Residual 24
-100 0 100 %
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
+47:8
+47:9
+47:10
+47:11
Decli
natio
n (J
2000
)
PACS 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
Model 160
0 150 3000 MJy sr-1
13:30.1 13:29.9 13:29.7Right Ascension (J2000)
160mu residual
-100 0 1000 %
Fig. 5. The observed (left column), modeled (2nd column) and residual (3rd column) images of M 51 for the GALEX FUV (top row), IRAC 3.6 µm(2nd row), IRAC 8 µm (3rd row), MIPS 24 µm (4th row) and PACS 160 µm (5th row) wavebands. The observed images have been convolved to theresolution of the PACS 160 µm filter, i.e. the resolution of all input parameters maps in the radiative transfer code. The size of the PACS beam (∼12 arcsec) is indicated in the bottom left corner of the model images. The last column shows the histogram of residuals (normalized to 1).
Article number, page 12 of 22
V$4(RX(/5'(173%@8"&'3'+4)5(>CD(2-(?UT(-*21()5'(!/(6"3@(673"%2+,(.93"6W(,23$#(3$+'0("+#(29,'*&"%2+,(.,''(3'4'+#0A( V$4(KX(/5'(29,'*&'#("+#(12#'3'#($1"4',($+(VL I(KAa(_1I(Rb(_1I("+#(TaS(_1(8"&'9"+#,A((
V$4(bX(/5'(5'"%+4(-*"6%2+((V<.c0(-2*(23#("+#(;27+4(,)"*,()5")("*'(*',B2+,$93'((-2*()5'('1$,,$2+($+(12+265*21"%6((8"&'9"+#,(cA((
