The Planck view of CMB Contamination from Diffuse Foregrounds

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Presentation transcript:

The Planck view of CMB Contamination from Diffuse Foregrounds Carlo Baccigalupi On Behalf of the Planck Collaboration KITP Conference, April 2013

Outline Component Separation for Planck CMB solutions Consistency and Robustness Cosmology from Component Separation Diffuse Foregrounds Conclusions The Planck Collaboration XII

Outline Component Separation for Planck CMB solutions Consistency and Robustness Cosmology from Component Separation Diffuse Foregrounds Conclusions Contribution from Jean-Francois Cardoso The Planck Collaboration XII

Outline Component Separation for Planck CMB solutions Consistency and Robustness Cosmology from Component Separation Diffuse Foregrounds Conclusions See Graca's talk The Planck Collaboration XII

Outline Component Separation for Planck CMB solutions Consistency and Robustness Cosmology from Component Separation Diffuse Foregrounds Conclusions Thanx to Ingunn and the C-R team The Planck Collaboration XII

Outline Component Separation for Planck CMB solutions Consistency and Robustness Cosmology from Component Separation Diffuse Foregrounds Conclusions The Planck Component Separation Group The Planck Collaboration XII

Component separation for Planck The Planck Collaboration XII

Component Separation for Planck d = A s + n The Planck Collaboration XII

Component Separation for Planck Your data The mixing matrix CMB and foregrounds d = A s + n Noise The Planck Collaboration XII

Component Separation for Planck resolution elements components d = A s + n resolution elements resolution elements frequencies frequencies components frequencies The Planck Collaboration XII

On foregrounds you... Know nothing Know something The Planck Collaboration XII

Thus you... Look for minimum variance Model and fit The Planck Collaboration XII

And you... Look for minimum variance in the needlet (spherical wavelet) domain – NILC in the pixel domain – SEVEM Model and fit semi-parametrically in the harmonic domain – SMICA physical parameters in the pixel domain – C-R The Planck Collaboration XII

And you... Look for minimum variance in the needlet (spherical wavelet) domain in the pixel domain Model and fit semi-parametrically in the harmonic domain physical parameters in the pixel domain The Planck Collaboration XII

CMB solutions The Planck Collaboration XII

Characterization of the CMB solutions Parallel runs on data and Full Focal Plane (FFP6) simulations, including the best in flight knowledge of instrumental behavior Instrumental error is propagated through noise variance (and covariance at low l for C-R for use in the likelihood) as well as through half-ring differences The beam is evaluated through ... Quantitative claims on: auto-spectra, cosmological parameter estimation Primordial Non-Gaussianity Lensing The Planck Collaboration XII

CMB solutions and Planck papers 2013 paper where component separation products were used for quantitative statements: Planck 2013, I, overview Planck 2013, XI, consistency Planck 2013 XIII, CO Planck 2013 XV, likelihood Planck 2013 XVI, cosmological parameters Planck 2013 XVII, lensing Planck 2013 XIX, ISW Planck 2013 XXIII, Isotropy Planck 2013 XXIV, non-Gaussianity Planck 2013 XXV, cosmic strings Planck 2013 XXVI, topology ... The Planck Collaboration XII

CMB solutions differences The Planck Collaboration XII

CMB standard deviation evaluated over methodology The Planck Collaboration XII

The Planck Collaboration XII; Courtesy of Jean-Francois Cardoso

Highlights on Component Separation: Spectral Matching The Planck Collaboration XII; Courtesy of Jean-Francois Cardoso

Highlights on Component Separation: Spectral Matching The Planck Collaboration XII; Courtesy of Jean-Francois Cardoso

Highlights on Component Separation: Spectral Matching The Planck Collaboration XII; Courtesy of Jean-Francois Cardoso

Highlights on Component Separation: Spectral Matching The Planck Collaboration XII; Courtesy of Jean-Francois Cardoso

Highlights on Component Separation: Spatial and Spectral Localization Localization in the pixel and harmonic domain (needlets) allows to treat foregrounds differently depending on their intensity in different regions of the sky and the angular domain Reducing to channel coaddition when they are absent, typically at small angular scales The Planck Collaboration XII; Courtesy of Jean-Francois Cardoso

Consistency and Robustness The Planck Collaboration XII

Sky masks The Planck Collaboration XII

Sky masks Threshold maskings is made by combining 30 and 353 Ghz flux thresholding for achieving a given sky fraction Confidence masks are method dependent: C-R NILC SEVEM SMICA The Planck Collaboration XII

Pseudo-spectra The Planck Collaboration XII

Pseudo-spectra The Planck Collaboration XII; Courtesy of Jean-Francois Cardoso

Null tests on FFP6: foreground residuals The Planck Collaboration XII

Null tests on FFP6: lensing The Planck Collaboration XII

Cosmology from Component Separation The Planck Collaboration XII

Cosmology with Component Separation See forthcoming Graca's talk on power spectra and cosmological parameter estimation Paul and Ben's talks on primordial non- Gaussianity Duncan's talk on lensing extraction Full list: Planck 2013 XV, likelihood Planck 2013 XVI, cosmological parameters Planck 2013 XVII, lensing Planck 2013 XIX, ISW Planck 2013 XXIII, Isotropy Planck 2013 XXIV, non-Gaussianity Planck 2013 XXV, cosmic strings Planck 2013 XXVI, topology The Planck Collaboration XII

Conclusions: CMB A leap forward for Component Separation in Planck Likely to split from now on into specialized foreground cleaning for CMB extraction, and foreground reconstruction for astrophysical studies CMB solutions from a complete set of approaches are consistent on a large sky fraction, at the level of the two and three point statistics Cosmological parameters from auto-spectra are consistent with the cross-spectra likelihood (see Graca's talk) Primordial non-Gaussianity and lensing results are consistent (see Paul's, Ben's and Duncan's talks monday) At low latitudes, relevant differences persist Simulations enable us to isolate the solution with the lowest residual contamination from diffuse foregrounds The Planck Collaboration XII

Diffuse Foregrounds The Planck Collaboration XII

Recovery of diffuse foregrounds with Planck Planck adopts a pixel based parametric approach for separating diffuse foregrounds Parameters in the pixel domain: spatially varying spectral indices and amplitudes of foreground components Fitting procedure: Markov Chains Monte Carlo over the multi- frequency datasets Main references: Brandt et al. 1994 (main idea), Eriksen et al. 2006 (efficient fitting through Gibbs sampling), Eriksen et al. 2008 (Jeffrey’s prior is introduced), Stompor et al. 2009 (high resolution fitting on the basis of chains conducted at low resolution) Implementation in the Commander-Ruler code which was used for all results presented in the Planck XII paper The Planck Collaboration XII

Foreground model Low frequency amplitude at 30 GHz and spectral index, effectively describing a mixture of various astrophysical effects, as Brehmsstrahlung (free-free), Anomalous Dust Emission (AME), Synchrotron CO amplitude at 100 GHz Thermal Dust amplitude at 353 GHz and grey body temperature and emissivity Monopoles and dipoles over the frequency channels which are considered for separation, to be estimated separately, at low resolution (Wehus et al. 2013) The Planck Collaboration XII

Methodology Inputs: Planck sky maps, 30-353 GHz, total and half-ring datasets along with their characterization Spectral indices estimation at low resolution takes as inputs the maps are smoothed to 40 arcminutes common resolution, re-pixelized at Nside=256 Mixing matrices are applied to the Ruler resolution dataset corresponding to 7.1 arcminutes The Planck Collaboration XII

From Commander to Ruler The Planck Collaboration XII

The Planck low frequency foregrounds Amplitude and spectral index of the low frequency component as seen by Planck Different emission mechanism, such as Brehmstraalung, synchrotron and low frequency dust emission are reflected in the sky distribution of the spectral index The Planck Collaboration XII

CO emission as seen by Planck Planck is sensitive to 9 CO transition lines in its frequency range Fit is done by modeling the emission is modelled as a constant line ratio over the full sky for increasing signal to noise ratio, isolate regions heavily affected by this emission The Planck Collaboration XII

The Planck view of thermal dust Planck provides an exquisite mapping of the Galactic thermal from 100 to 857 Ghz Planck resolves the sky pattern of dust emissivity, reflecting different phases in the interstellar gas The Planck Collaboration XII

The Planck view of thermal dust A comparison is made between the dust solution in the frequency interval where the fit is done and the dust dominated channels at 545, 857 Ghz A scatter plot reveals substantial agreement in the common 353 Ghz channel The Planck Collaboration XII

Validating on FFP6... The Planck Collaboration XII

Validating on FFP6... The Planck Collaboration XII

Validating on FFP6... The Planck Collaboration XII

Conclusions: foregrounds Planck is able to separate diffuse Galactic foregrounds on 87% of the sky, quantifying uncertainties from the separation procedure as well as instrumental noise Planck resolves a single low frequency component amplitude and effective spectral index, CO line ratio, and a thermal dust amplitude and emissivity An extensive study involving other datasets is necessary for fully exploit the Planck capability of studying the astrophysical properties of foregrounds, in particular at low frequencies The Planck Collaboration XII

What's next Over the next year we plan to... Say goodbye to Component Separation doing everything, welcome specialization for CMB extraction and foreground recovery Extracting Foregrounds using Ancillary Datasets Use more data, 2.5 years versus 1 Continuing to study systematics, beam effect at arcminute resolution in particular Polarization... ... The Planck Collaboration XII

The Planck Collaboration XII

Beams Beams transfer functions are provided NILC, SEVEM, SMICA adopt a Gaussian representation of the beam with 5 arcminutes FWHM C-R esimates the beam transfer function though FFP6 Mcs adopting in flight main beam measurements The Planck Collaboration XII