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Page 1: kP1KBbbBQMBMlHi` @GmKBMQmbAM7` `2/ : H tB2b i`2/b?B7i k 9cyang/docs/estec_2016-v3.pdf · X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X X " +F;`QmM/>kPBM?B;?@xlGA_:bC=9>kP

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Now

Epoch ofgalaxy

assembly

Firstgalaxies

Mad

au &

Dickin

son 2

014

Mag

nelli et al. 2

013

~ 0.9 billion yrsRiechers et al. 201313

~ 0.5 billion yrsBialy et al. 2015

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Mrk 231 adap

ted fro

m G

onzále

z-A

lfonso

et a

l. 2010

Mrk 231

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Herschel SPIRE/FTS archive survery: Yang et al., 2013

(see also Master Thesis of Chentao Yang, 2013)

- First systematic study of submm rotational H2O emission lines in local infrared galaxies (45 out of 176)

- LH2O

is roughly proportion to LIR: Confirm the importance of IR pumping for the submm H

2O excitation

AGN-dominatedstar-forming-dominated

.

.

absor

bing

IR photo

ns

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Efficiently choosing the lensed sources

Herschel-ATLAS (Eales et al. 2010):

- Widest area survey with Herschel (570 deg2);

- Covering 5 bands from 100 μm to 500 μm;

- Selecting strongly lensed candidats by S500 μm

>100 mJy;

- Determining the redshifts by follow-up CO observations;

- Follow-up imaging observations for bulding lensing model; (Sample with ~30 sources, Bussmann et al. 2013)

Neg

rello et al. 2

010

ALMA image @1mm

see e.g., Vlah

akis et al. 2015

ID81

SMA 880 μm Bussmann et al. 2013

SDP field

ID81

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240 GHz

21 good H2O emission line detections in

16 high-z ULIRGs

- Largest study of high-z H2O;

- z~2-4, cosmic star formation peak;

- μlens@880μm

= 2–15 (magnification, from BU13);

- LIR = 0.4–2×1013 L⊙;

- ΣSFR

=100–2000 M⊙ yr-1 kpc-2;

- Efficient to detect H2O in high-z ULIRGs.

SMA@880 μm

Bussmann et al. 2013 (BU13)

ΔRA (arcsec)

ΔD

EC

(a

rcse

c)

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-T

-W - LIR and L

H2O are roughly propotional

- Can be explained by the infrared pumping model (González-Alfonso et al. 2014)

- Good tracer of the IR radiation field - No AGN signature (mid-IR and radio) --> Tracing the IR radiation fields connected to star formation

(Eupper = 137 K)(Eupper = 101 K)

(Eupper = 305 K)

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local averageYang et al. 2013Riechers et al. 2013

Norm

alized Intensity

Eup/k Temperature (K)

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==

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=

=P

relim

ina

ry re

sults, Y

ang et al. in

prep.

Norm

alized Intensity

local averageYang et al. 2013

Eup/k Temperature (K)

=

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+

+

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Yang et al, in prep. (preliminary images we got yesterday) NOEMA, A-config.

dust emission @263 µm

5/µ1/2 kpc

(µ ~11.3)

NC.143 (z=3.6)

Bu

ssm

ann

et

al. 2

013

• Comparing the spatial distribution of dust emission, H2O, H2O+

and CO(10-9) emission in sub-kpc scale (+lensing model).

– Comparing the spatial distributions of different gas tracers.

– Testing the IR pumping model, and better constrain the physical parameters.

• Building lensing model for each line, “differential lensing free”.

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∼ . − .

≥+

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, ,

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high-z ULIRGs

local

galax

ies

Galactic

YSOs

+

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-T

-W

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E

q

/ /

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van Dishoeck et al. 2013

Yang et al. 2016

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