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SFR(M⊙yr−1) = 1.72×10−10LTIR(L⊙) (4) |
In Fig.3, we show the LTIRLFs. Symbols are the same as |
Fig.1. Inthe topaxis,we showcorrespondingSFR. Overplott ed |
asterisks are cluster LF of MS1054 at z=0.83 with ×2 larger |
mass by Bai et al. (2007), which show good agreement with |
ourLFsofRXJ1716.4 +6708in thesquares.Notethat Bai et al. |
(2007) covered only the central region of MS1054 due to the |
smaller field of view of the Spitzer. The shape of their LF look s |
more similar to our LFs in the highest density bin in Fig.2. A |
shift in scale is perhaps due to difference in esimating clus ter |
volumes. |
Amajordifferenceofourworktothat ofBai etal. (2007)is |
that they were not able to compare in detail on the shape of the |
LFs between field and cluster regions, due mainly to a smaller |
fieldcoverageandlargererrorsonLFs.Theyhadtofixthefain t- |
end slope with a local value. The largest source of errors is i nGotoet al.:Environemental dependence of 8 µm luminosity functions ofgalaxies atz ∼0.8 5 |
converting Spitzer 24 µm flux into 8 µm. Both cluster and field |
LFs of this work use L15filter, which measures restframe 8 µm |
fluxdirectly,eliminatingthelargestsourceoferrors.Ina ddition, |
bothclusterandfiledLFsaremeasuredwithanessentiallysa me |
methodology,allowingusa faircomparisonofLFs. |
4. Summary |
We constructed restframe 8 µm LFs of a massive galaxy cluster |
(RXJ1716.4 +6708) and a rarefied field region (the NEP deep |
field)at z ∼0.8usingessentially thesame methodanddata from |
the AKARI telescope. AKARI’s 15 µm filter nicely covers rest- |
frame8µm at z∼0.8,and thuswe do not needa large interpola- |
tion based on SED models. AKARI’s wide field of view allows |
ustoinvestigatevarietyofclusterenvironmentswith2ord ersof |
differenceinlocal galaxydensity. |
We found that L∗of the cluster 8 µm LF is smaller than the |
field by a factor of 2.4, and the faint-end tail of cluster IR LF s |
becomesteeperandsteeperwithincreasinglocalgalaxyden sity. |
This difference cannot be explained by a simple infall of fiel d |
galaxies into a cluster. Physics that preferentially supre sses IR |
luminous galaxes in higer density regions is needed to expla in |
theobservedresults. |
Acknowledgments |
Wethanktheanonymousrefereeformanyinsightfulcomments , |
which significantly improved the paper. We are greateful to |
MasayukiTanakaforusefuldiscussion.WethankL.Baiforpr o- |
vidingdataforcomparison. |
T.G.,Y.K. and H.I. acknowledgesfinancial support from the |
JapanSocietyforthePromotionofScience(JSPS)throughJS PS |
ResearchFellowshipsforYoungScientists.MIwassupporte dby |
the Korea Science and Engineering Foundation(KOSEF) grant |
No. 2009-0063616, funded by the Korea government(MEST)” |
HML acknowledgesthe supportfrom KASI throughits cooper- |
ativefundin2008. |
This research is based on the observations with AKARI, a |
JAXA projectwiththe participationofESA. |
Theauthorswishtorecognizeandacknowledgetheverysig- |
nificant cultural role and reverence that the summit of Mauna |
Kea has always had within the indigenous Hawaiian commu- |
nity. We are most fortunate to have the opportunity to conduc t |
observationsfromthissacredmountain. |
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