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Dark Energy Radio HI Surveys

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Geometric: Baryon Acoustic Oscillations (CMB, HI, optical), lensing geometry, ... follow-up for astrometry and redshifts. Today, radio astrometry is unmatched. ... – PowerPoint PPT presentation

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Title: Dark Energy Radio HI Surveys


1
Dark Energy Radio HI Surveys
  • Ue-Li Pen
  • ???

SKA artist conception
2
Dark Energy Measurements
  • Geometric Baryon Acoustic Oscillations (CMB, HI,
    optical), lensing geometry, SNe luminosity
    distance.
  • Dynamical gravity dark matter (lensing
    tomography, cluster mass evolution)
  • Dynamical energy measure spatial perturbations
    in the dark energy field (ISW)

3
Radio vs Optical
  • Complementary approaches.
  • Historically, radio was an early window to high-z
    universe, but required optical follow-up for
    astrometry and redshifts.
  • Today, radio astrometry is unmatched. High-z
    searches dominated by optical, but redshifts are
    very challenging in range of interest (z1-2).
  • Revolution possible with billion HI redshifts

4
Image courtesy of NRAO/AUI and Chung et al.,
Columbia University
5
Existing operational cylinders
MOLONGLO 1600x12m Cost12/m2 (current dollars)
OOTY (India) 530x30m Both rotate in one dimension
6
Cylinder History
  • Popular 1960-1980
  • Lost favor with advent of cryogenically cooled
    pre-amplifiers.
  • Room temp amplifiers with 20K noise temp now
    available.

Illinois 400 ft Telescope ca. 1960
7
Indian Giant Meterwave Radio Telescope
30 dishes _at_45m ea. Operates at lt1.5 GHz
8
Traditional Radio Telescope Cost Drivers
  • High Frequency cryogenic receivers, surface,
    pointing accuracy
  • Correlation/bandwidth N2 cost
  • General purpose steerable, reconfigurable
  • HSHS target 10/m2, lt1.4 GHz, transit
  • Molonglo actual 12/m2, steerable cyl
  • GMRT actual 100/m2, lt1.4 GHz
  • SKA target 1000/m2
  • VLA actual 10000/m2

9
Hubble Sphere Hydrogen Survey
HSHS Large Area, Low Cost
  • Jeff Peterson, Uros Seljak, CEA, LAL, South
    Africa, Australia
  • Map 109 galaxy 21cm redshifts to zlt1.5 for Baryon
    acoustic oscillations, weak lensing
  • Dark energy parameters
  • Low cost, fast time scale.
  • Astro-ph/0606104

10
  • passive transit cylinder
  • Correlations FFT is N log N instead of N2
  • Astro-ph/0606104
  • Collaborators CEA, ETH, SA

Jeff Peterson Jan 2007
11
Cosmic Magnification
  • Cosmic shear has evolved as a direct way to map
    dark matter
  • Several major surveys under way or planned
    CFHTLS, LSST, SNAP
  • Anticipated limitations redshift distribution,
    PSF
  • With redshifts, these limits can be overcome, and
    magnification is measured directly
  • Measured through cross correlation in SDSS
    (Scranton et al 2005)
  • Forecasts and models by Zhang and Pen (2005,
    2006) overcomes intrinsic clustering.

12
Gravitational Lensing increase flux, decrease
density
Zwann et al
Magnification increases number of bright
galaxies, decreases faint ones.
13
Magnification Lensing
  • Bright-faintlensing
  • Brightfaintintrinsic clustering
  • Almost orthogonal measurements if distances are
    known
  • May overcome all known systematic limitations to
    shear lensing (PSF, intrinsic alignment, z-dist),
    similar sensitivity.
  • Well suited to HI radio surveys and SKA.

14
Zhang Pen 2005
15
Abdalla Rawlings, 2004
16
Dark Energy Accuracy
  • From SKA (or similar 109 redshift survey) BAO
  • Geometric Lensing (Hu Jain 2004)
  • Dynamical lensing (Hu 2003)

17
Summary
  • Radio and optical have played complementary
    roles, and the future may be for 21cm-radio as
    massive redshift machines to map Hubble Volume.
  • In cm-m wavelength, enormous growth potential in
    technology and collecting area
  • Billion redshift Hubble Volume survey will be a
    key in dark energy measurement geometric and
    dynamical (BAO, lens, ISW), and targeted by SKA
    and HSHS
  • Construction of a billion redshift survey radio
    telescope may be very economical (e.g. HSHS).
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