Difference between revisions of "Cosmological Parameters"

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* PDF tables with 68% limits [[File:baseline_params_table_2015_limit68.pdf]]
 
* PDF tables with 68% limits [[File:baseline_params_table_2015_limit68.pdf]]
 
* PDF tables with 95% limits [[File:baseline_params_table_2015_limit95.pdf]]
 
* PDF tables with 95% limits [[File:baseline_params_table_2015_limit95.pdf]]
 
There are also summary comparison tables, showing how constraints for selected models vary with data used to constrain them:
 
  
  
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! Tag|| Data
 
! Tag|| Data
 
|-
 
|-
| '''planck''' || high-L Planck  temperature (CamSpec, 50 <= l <= 2500)
+
| '''plikHM''' || baseline high-$l$ Planck power spectra (plik cross half-mission, 30\ <= l\ <= 2508)
 +
|-
 +
| '''lowl''' || low-L: Planck  temperature only (2 <= l <= 29)
 +
|-
 +
| '''lowTEB''' ||  low-L temperature and LFI polarization (2 <= l <= 29)
 
|-
 
|-
| '''lowl''' || low-L: Planck temperature (2 <= l <= 49)
+
| '''lowEB''' || low-L LFI polarization only (2 <= l <= 29)
 +
|-
 +
| '''WMAPTEB''' || low-L temperature, and  LFI+WMAP polarization (2 <= l <= 29)
 
|-
 
|-
 
| '''lensing''' || Planck lensing power spectrum reconstruction
 
| '''lensing''' || Planck lensing power spectrum reconstruction
 
|-
 
|-
| '''lowLike''' || low-L WMAP 9 polarization  (WP)
+
| '''lensing''' || Planck lensing power spectrum reconstruction only; T,E fixed to best-fit spectrum + priors
 +
|-
 +
| '''zre6p5''' || A hard prior z_re > 6.5
 +
|-
 +
| '''tau07''' || A Gaussian prior on the optical depth, tau = 0.07 +- 0.02
 +
|-
 +
| '''reion''' || A hard prior z_re > 6.5, combined with Gaussian prior z_re = 7 +- 1
 
|-
 
|-
| '''tauprior''' || A Gaussian prior on the optical depth, tau = 0.09 +- 0.013
+
| '''BAO''' || Baryon oscillation data from DR11LOWZ, DR11CMASS, MGS and 6DF
 
|-
 
|-
| '''BAO''' || Baryon oscillation data from DR7, DR9 and and 6DF
+
| '''JLA''' ||   Supernova data from the SDSS-II/SNLS3 Joint Light-curve Analysis
 
|-
 
|-
| '''SNLS''' ||  Supernova data from the Supernova Legacy Survey
+
| '''H070p6''' ||  Hubble parameter constraint, H_0 = 70.6 +- 3.3
 
|-
 
|-
| '''Union2''' ||  Supernova data from the Union compilation
+
| '''theta''' ||  theta_MC fixed to 1.0408
 
|-
 
|-
| '''HST''' || Hubble parameter constraint from HST (Riess et al)
+
| '''WLonlyHeymans''' || Conservative cut of the CFHTLenS weak lensing data + priors
 
|-
 
|-
 
| '''WMAP''' || The full WMAP (temperature and polarization) 9 year data  
 
| '''WMAP''' || The full WMAP (temperature and polarization) 9 year data  
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Tags used to identify the model paramters that are varied are described in [[File:parameter_tag_definitions.pdf]]. Note that alpha1 results are not used in the parameter paper, and are separate from the isocurvature results in the inflation paper.
+
Tags used to identify the model parameters that are varied are described in [[File:parameter_tag_definitions.pdf]].  
  
 
== Parameter Chains ==
 
== Parameter Chains ==

Revision as of 17:19, 15 January 2015

Description[edit]

The cosmological parameter results explore a variety of cosmological models with combinations of Planck and other data. We provide results from MCMC exploration chains, as well as best fits, and sets of parameter tables. Definitions, conventions and reference are contained in Planck-2013-XVI[1].

Production process[edit]

Parameter chains are produced using CosmoMC, a sampling package available here. This includes the sample analysis package (and GUI) GetDist, and the scripts for managing, analysing, and plotting results from the full grid or runs. Chain products provided here have had burn in removed. Some results with additional data are produced by importance sampling.

Note that the baseline model includes one massive neutrino (0.06eV). Grid outputs include WMAP 9 results for consistent assumptions.

Caveats and known issues[edit]

  1. Confidence intervals are derived from the MCMC samples, and assume the input likelihoods are exactly correct, so there is no quantification for systematic errors other than via the covariance, foreground and beam error models assumed in the likelihood codes.
  2. Non-linear lensing modelling uses Halofit; for some extended models and CMB lensing only analyses, tails of the chains may be away from the domain of validity.
  3. The CAMB version used for most results is Dec 2014; the Jan 2015 version is used for lensing-only models with neutrinos, and only differs in the neutrino corrections to the halofit model.
  4. There is evidence of temperature-polarization leakage that may affect results including high-L polarization, use caution in the interpretation of results including polarization

Related products[edit]

Results of the parameter exploration runs should be reproducible using CosmoMC with the Planck likelihood code.

Parameter Tables[edit]

These list paramter constraints for each considered model and data combination separately


Data combination tags used to label results are as follows (see Planck-2013-XVI[1] for full description and references):


Tag Data
plikHM baseline high-$l$ Planck power spectra (plik cross half-mission, 30\ <= l\ <= 2508)
lowl low-L: Planck temperature only (2 <= l <= 29)
lowTEB low-L temperature and LFI polarization (2 <= l <= 29)
lowEB low-L LFI polarization only (2 <= l <= 29)
WMAPTEB low-L temperature, and LFI+WMAP polarization (2 <= l <= 29)
lensing Planck lensing power spectrum reconstruction
lensing Planck lensing power spectrum reconstruction only; T,E fixed to best-fit spectrum + priors
zre6p5 A hard prior z_re > 6.5
tau07 A Gaussian prior on the optical depth, tau = 0.07 +- 0.02
reion A hard prior z_re > 6.5, combined with Gaussian prior z_re = 7 +- 1
BAO Baryon oscillation data from DR11LOWZ, DR11CMASS, MGS and 6DF
JLA Supernova data from the SDSS-II/SNLS3 Joint Light-curve Analysis
H070p6 Hubble parameter constraint, H_0 = 70.6 +- 3.3
theta theta_MC fixed to 1.0408
WLonlyHeymans Conservative cut of the CFHTLenS weak lensing data + priors
WMAP The full WMAP (temperature and polarization) 9 year data


Tags used to identify the model parameters that are varied are described in File:Parameter tag definitions.pdf.

Parameter Chains[edit]

We provide the full chains and getdist outputs for our parameter results. The entire grid of results is available from as a 2.8GB compressed file:

You can also download key chains for the baseline LCDM model here:

The download contains a hierarchy of directories, with each separate chain in a separate directory. The structure for the directories is

base_AAA_BBB/XXX_YYY_.../

where AAA and BBB are any additional parameters that are varied in addition to the six parameters of the baseline model. XXX, YYY, etc encode the data combinations used. These follow the naming conventions described above under Parameter Tables. Each directory contains the main chains, 4-8 text files with one chain in each, and various other files all with names of the form

base_AAA_BBB_XXX_YYY.ext

where ext describes the type of file, and the possible values or ext are


Extension Data
.txt parameter chain file with burn in removed
.paramnames File that describes the parameters included in the chains
.minimum Best-fit parameter values, -log likelihoods and chi-square
.bestfit_cl The best-fit temperature and polarization power spectra and lensing potential (see below)
.inputparams Input parameters used when generating the chain
.minimum.inputparams Input parameters used when generating the best fit
.ranges prior ranges assumed for each parameter


In addition each directory contains any importanced sampled outputs with additional data. These have names of the form

base_AAA_BBB_XXX_YYY_post_ZZZ.ext

where ZZZ is the data likelihood that is added by importance sampling. Finally, each directory contains a dist subdirectory, containing results of chain analysis. File names follow the above convntions, with the following extensions


Extension Data
.margestats mean, variance and 68, 95 and 99% limits for each parameter (see below)
.likestats parameters of best-fitting sample in the chain (generally different from the .minmum global best-fit)
.covmat Covariance matrix for the MCMC parameters
.corr Correlation matrix for the parameters
.converge A summary of various convergence diagnostics


Python scripts for reading in chains and calculating new derived parameter constraints are available as part of CosmoMC, see the readme for details [1].

File formats[edit]

The file formats are standard March 2013 CosmoMC outputs. CosmoMC includes python scripts for generating tables, 1D, 2D and 3D plots using the provided data. The formats are summarised here:

Chain files
Each chain file is ASCII and contains one sample on each line. Each line is of the format
weight like param1 param2 param3 …
Here weight is the importance weight or multiplicity count, and like is the total -log Likelihood. param1,param2, etc are the parameter values for the sample, where the numbering is defined by the position in the accompanying.paramnames files.
Note that burn in has been removed from the cosmomc outputs, so full chains provided can be used for analysis. Importance sampled results (with _post) in the name have been thinned by a factor of 10 compared to the original chains, so the files are smaller, but this does not significantly affect the effective number of samples. Note that due to the way MCMC works, the samples in the chain outputs are not independent, but it is safe to use all the samples for estimating posterior averages.
.margestats files
Each row contains the marginalized constraint on individual parameters. The format is fairly self explanatory given the text description in the file, with each line of the form
parameter mean sddev lower1 upper1 limit1 lower2 upper2 limit2 lower3 upper3 limit3
where sddev is the standard deviation, and the limits are 1: 68%, 2: 95%, 3: 99%. The limit tags specify whether a given limit is one tail, two tail or none (if no constraint within the assumed prior boundary).
.bestfit_cl files
They contain the best-fit theoretical power spectra (without foregrounds) for each model. The columns are: [math]l[/math], [math]D^{TT}_l[/math], [math]D^{TE}_l[/math], [math]D^{EE}_l[/math], [math]D^{BB}_l[/math], and [math]D^{dd}_l[/math], were [math]D_l \equiv l(l+1) C_l / (2\pi)[/math] in [math]\mu{\rm K}^2[/math]. Also [math]D^{dd}_l= [l(l+1)]^2 C^{\phi\phi}_l/(2\pi)[/math] is the power spectrum of the lensing deflection angle, where [math]C^{\phi\phi}_l[/math] is the lensing potential power spectrum. For results not including the lensing likelihood, this is the prediction from linear theory; for lensing outputs this includes corrections due to non-linear structure growth. The [math]D_l[/math] are output to high [math]l[/math], but not actually computed above [math]l_{\rm max}=2500[/math] (Planck), [math]l_{\rm max}=4500[/math] (Planck+highL) or [math]l_{\rm max}=1500[/math] (WMAP), and [math]l[/math] values above these are fixed to a scaled fiducial template.

References[edit]

  1. 1.01.1 Planck 2013 results. XVI. Cosmological parameters, Planck Collaboration, 2014, A&A, 571, A16

Cosmic Microwave background

(Planck) Low Frequency Instrument