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Page 1: High  Redshift  Galaxies/Galaxy Surveys

High Redshift Galaxies/Galaxy Surveys

ALMA Community Day April 18, 2011

Neal A. MillerUniversity of Maryland

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Overview• ALMA as IFU

– Imaging (continuum) and spectroscopy (line) rolled into one

• Up to 8GHz bandwidth per polarization, small channels

– Talk arranged continuum then line• General Topics

– SFH of universe• General birth/building of galaxies• Galaxies in the epoch of reionization

– Co-evolution of bulges and black holesApril 18, 2011

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Linear Resolution

April 18, 2011

Rough rules of thumb

Compact Array: ~5 to 35 kpc resolution Most sources unresolved spatially

Extended Array: ~50 pc to 350 pc Angular resolutions a few times better than HST

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Continuum: Negative K Correction

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Negative K Correction in Play

April 18, 2011

c Lanzetta

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Continuum: Early Science Possibilities

Mosaic observations of significant fields?Tradeoffs:

• Intrinsic flux of sources greater at higher frequencies

• Field of view is smaller at higher frequencies (about 1’ at Band 3, under 10” at Band 9)

• Receiver temperatures higher at higher frequencies

April 18, 2011

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ALMA: Imaging the HUDF

April 18, 2011

Band 3: 100 GHz ~23 pointings to mosaicfull 2.2’ square of HUDF

Arp 220 sources about3 μJy flux density

4.7 μJy per pointing, a 3σdetection requires 1.6 μJyrms

Over 12 days per pointing!Not enough time in Early Science

Full Array: still over a dayper pointing

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ALMA: Imaging the HUDF

April 18, 2011

Band 6: 240 GHz ~115 pointings to mosaicFull 2.2’ square of HUDF(too many for Early Science)

Arp 220 sources about30 μJy flux density

47 μJy per pointing, a 3σDetection requires 16 μJy rms

6.9 hr per pointing in Early Science (not enoughtime in Early Science)

Full Array: ~100 hoursTotal with overheads

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Continuum Science• Contiguous area survey observations of deep

fields not well suited for Early Science, good for Full Array

• Surveys to follow-up individual sources are more appealing– SCUBA, AzTEC, LABOCA, etc.– SMGs, QSOs, HzRG with flux densities of a few

mJy– Band 6 or 7 (800μm to 1.4mm)

• Band 7 to reach 0.2 mJy just 9 minutes Early Science• Resolutions of ~1” to ~0.01” (10 kpc to 100 pc)

April 18, 2011

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Individual Source Continuum Surveys

• Better positions– Single dish observations with bolometer arrays,

tens of arcseconds resolution• Prior follow-up was radio, expensive time requirement

• FIR luminosities through SED fitting– Pair with non-RJ data (Spitzer, Herschel)– SFR in absence of AGN– Dust temperatures, masses

• Other sources – GRBs?

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Spectral Line: CO

April 18, 2011

CO(J=1-0) traces totalmolecular gas mass

Higher J for warmer, densergas

Ratios give excitation properties of molecular gas

Line widths for estimate ofdynamical mass

CO correlates with FIR, hence rough SFR

Also for SF efficiency: FIRfor current SF, CO for gasreservoir

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CO Rotational Ladders

April 18, 2011

Figure from Weiss et al (2007)

Sources: Central regions of local starbursts (NGC253, M82)

SMGs (SMM16359, highly lensed)

QSOs (BR1202, SDSS J1148 at z=6.4)

BAL QSO (APM0827)

Strength: Peak flux densities of several mJy, integrated lines of a few Jy km/s

Widths of a few hundred km/s

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Spectral Line: Additional Lines

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HCN only from dense gas,stronger indicator of starformation

HCN line luminosities muchhigher in SMGs and relatedobjects than in normal spirals

[CII] strongest atomic line, cooling line for atomic gas

Also [CI]; similar critical density for excitation as CO

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Spectral Line Possibilities• Redshift search for SMGs

– Difficult to get optical (position, dust obscuration)– Look for CO lines, get 8 GHz per polarization to

cover full bands in multiple observations– Line spacing as 1/(1+z)

• Absorption lines• CO in host of object types

– High z quasars– Lensed “normal” galaxies– LAEs, LBGs?

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Possible Questions• Black hole mass from HST, dynamical mass

from CO?• SF efficiency? Pair FIR with line luminosity• Morphology – big disks or mergers for

SMGs?– Formation of present day massive ellipticals?

• AGN unification and evolutionary models?– Starburst to obscured AGN to unobscured AGN?

April 18, 2011