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Computational Challenges in CMB Data Analysis

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The CMB is a EM relic from the hot Big Bang. Its anisotropy traces the evolution of the LSS of the Universe ... cosmological signal is largely subdominant in the ... – PowerPoint PPT presentation

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Title: Computational Challenges in CMB Data Analysis


1
Computational Challenges in CMB Data Analysis
  • Paolo Natoli
  • Dipartimento di Fisica
  • Università Tor Vergata

Credits M. Botti, F. Massaioli (Caspur) G. de
Gasperis, A. Traficante (Tor Vergata)
2
The Cosmic Microwave Background
  • The CMB is a EM relic from the hot Big Bang
  • Its anisotropy traces the evolution of the LSS of
    the Universe
  • Target of many high precision experiments in the
    last two decades
  • O(10) balloons and ground based (BOOMERanG, CBI,
    DASI,...)
  • Two flown NASA satellites COBE (1989) and WMAP
    (2001)
  • The ultimate CMB satellite, Planck (ESA), is
    just around the corner...
  • It is widely regarded as a goldmine of
    cosmological information

3
Increasing complexity
COBE, early 1990, 10 K pixels
WMAP, early 2000, 1M pixels
Planck, launch 2008, gt 10 M pixels
4
Why is data analysis challenging?
  • Large Problem
  • Many Gb/channel/day
  • 105 to 107 pixels
  • Detectors inject noise
  • Noise is often correlated (long memory, or 1/f
    )
  • Systematics (non statistical noise) play an
    increasingly important role in high accuracy
    experiments.

5
Size of dataset is an issue
  • Need to observe large fractions of the sky to
    decrease sampling variance
  • observe up to few arcmin resolution, to gather
    most cosmological information

Maps with many resolution elements
(pixel) typically in the million range
6
But noise is the true enemy!
  • Good CMB detectors have noise sensitivities in
    the range 100 to 300
  • Experiments must spin (or chop) quickly to
    modulate the signal (exp. low modes, dipole often
    used for calibration) in the frequency range were
    amplifiers are stable enough.

cosmological signal is largely subdominant in
the timestream, have to resort to non trivial
statistical techniques to dig it out
7
Pixel Space Map Making
  • Go from Time-Ordered data to pixel values
  • Do it (reasonably) quick, without loosing (too
    much) information

8
A simple data model
sky
noise
pointing (sky reading)
signal
9
A trivial solution, in principle
But one that is computationally unfeasible!
10
A workable solution
  • First implementation, aimed at Planck
  • Natoli, de Gasperis, Gheller Vittorio, 2001,
    AA
  • Tested at CINECA
  • Polarized ROMA
  • de Gasperis, Natoli et al., 2005 AA
  • Tested at Caspur/Nersc
  • These activities evolved into ROMA (ROMA Optimal
    Map Making Algorithm) code, a suite of codes
    aimed at polarized CMB map making and noise
    estimation


11
ROMA
  • A collaboration has begun with Caspur in 2005.
  • This resulted in an almost complete rewriting of
    the code
  • Written in Fortran 95, uses MPI for message
    passing, cfitsio for I/O and FFTW3 to perform
    fast convolutions
  • Implemented on a number of architectures
  • SGI Origin, IBM SP3/SP5, Linux clusters, up to gt
    1000 PEs
  • On several supercomputing centers
  • CINECA, NERSC/LBL, Caspur, LFI DPC

12
Scalings 1/2
13
Scalings 2/2
100 Msamples
1.9 GHz Pwr5
2.4 GHz Opteron
14
The Hybrid code
  • ROMA requires a substantial amount of PE to work
    on a year long dataset, mostly because of the
    need to store the timeline in memory
  • However, long term correlations are weak and they
    mostly pollute the common mode (monopole) of a
    map
  • Hence the Hybrid code (Traficante et al. in
    preparation)
  • Divide the dataset in many submaps, each of which
    is porcessed by ROMA
  • Estimate the comon modes and subtract them from
    the maps
  • Co-add the maps weighting by noise

15
Planck 30 GHz dataset ( 4 Gsamples)
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