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DACOTA The Dense Array for COsmological Transi5ons David DeBoer 1 , Geoffrey Bower 1 , Garre> Kea5ng 1 , Richard Plambeck 1 , TzuChing Chang 2 , Paul Ho 2 , Daniel Marrone 3 , Anthony Readhead 4 1 UC Berkeley 2 Academia Sinica Ins5tute for Astronomy and Astrophysics 3 University of Arizona 4 California Ins5tute of Technology

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Page 1: ursi2013 deboer pdfVersion - National Radio Astronomy ... · • Phaseddevelopmentoftechniques/ instrumentaonforredshiedCO – piggybacktohigherz – upperlimits>detecon>stascs>imaging

DACOTA    

The  Dense  Array  for  COsmological  Transi5ons  

David  DeBoer1,  Geoffrey  Bower1,  Garre>  Kea5ng1,  Richard  Plambeck1,  Tzu-­‐Ching  Chang2,  Paul  Ho2,  Daniel  Marrone3,  Anthony  

Readhead4  1UC  Berkeley  2Academia  Sinica  Ins5tute  for  Astronomy  and  Astrophysics  3University  of  Arizona  4California  Ins5tute  of  Technology  

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Cosmic  Dawn:  How  was  the  Milky  Way  Formed?  

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Cosmic  Dawn:      Mul5-­‐Pronged  Approach  

Neutral  Hydrogen  

Massive  Galaxies  Ionized  Gas  

The  Mul5tude  of  Galaxies:  Milky  Way  Building  Blocks  

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Z  =  6   Z  =  3  Z  =  8  

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CO  Luminosity  Es5mates  

•  O-­‐O-­‐M  approach  (Carilli  2010)  •  Compute  needed  SFR  for  reioniza5on  •  Get  other  rela5onships  to  go  from  that  to  something  observable.  

•  SFR  à  LIR  à  LCO    

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Simple  Halo  Model  (essen5ally  same  assump5ons)  

•  Lidz  et  al  2011  (Ap  J  741:70)  •  Parameterized  by  the  minimum  mass  halo  hos5ng  CO  luminous  galaxies:  

Munoz  et  al  2013  

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Model  for  Lower  z  •  Pullen  et  al  2012  •  Models  with  different  CO  luminosity  assump5ons:  

–  A  :  Halo  mass  to  CO  luminosity  –  B  :  Star  forma5on  rate  to  CO  luminosity  

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Evolu5on  of  Molecular  Gas  

Z=6  

Z=3  

OMG  

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•  Phased  development  of  techniques/instrumenta5on  for  red-­‐shieed  CO  – piggy-­‐back  to  higher  z  – upper  limits  -­‐>  detec5on  -­‐>  sta5s5cs  -­‐>  imaging  

•  Leveraging  the  tremendous  amount  of  work  done  in  HI  EOR  – smaller  signal,  but  easier  foregrounds  

•  Use  exis5ng  facili5es  to  start  

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•  What  is  desired  is  the  spa5al  power  spectrum,  not  an  image  (yet)  – k  is  the  3-­‐D  wavenumber  of  the  spa5al  PS  –  Interferometric  u,v  coordinates  are  just  scaled  versions  of  k  in  the  plane  of  the  sky  (k    )  

– On  cosmological  scales,  the  frequency  axis  provides  the  “line-­‐of-­‐sight”  image  coordinate  •  Its  transform  is  the  k      coordinate  

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•  What  is  desired  is  the  spa5al  power  spectrum,  not  an  image  (yet)  – k  is  the  3-­‐D  wavenumber  of  the  spa5al  PS  –  Interferometric  u,v  coordinates  are  just  scaled  versions  of  k  in  the  plane  of  the  sky  (k    )  

– On  cosmological  scales,  the  frequency  axis  provides  the  “line-­‐of-­‐sight”  image  coordinate  •  Its  transform  is  the  k      coordinate  

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•  What  is  desired  is  the  spa5al  power  spectrum,  not  an  image  (yet)  – k  is  the  3-­‐D  wavenumber  of  the  spa5al  PS  –  Interferometric  u,v  coordinates  are  just  scaled  versions  of  k  in  the  plane  of  the  sky  (k    )  

– On  cosmological  scales,  the  frequency  axis  provides  the  “line-­‐of-­‐sight”  image  coordinate  •  Its  transform  is  the  k      coordinate  

J=2-­‐1  

J=1-­‐0  

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For  an  “imaging”  interferometer  

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CARMA  (SZA)  

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Redundant  Interferometer  

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Redundant  Interferometer  

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Unrotated  Version  

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AMIBA  

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Sensi5vity  &  Boost  Factor  

AMIBA  

AMIBA  –  no  ro

ta5on  

SZA  

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DACOTA-­‐I  Sensi5vity  @  z=6  

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Sensi5vity  @  z=3  

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Measurement  

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Frequencies  

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Diameter  

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Config  

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Technical  Overview  

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Technical  Overview  

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Technical  Overview  

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Cross-­‐correla5on  

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Cross-­‐correla5on  

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Future  

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PAPER  

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PAPER  

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