Namespace

NumCosmo – 1.0

NumCosmo Library

Version0.27.0
AuthorsNumCosmo Developers
LicenseLGPL-2.1-or-later
Websitehttps://numcosmo.github.io/
Sourcehttps://github.com/NumCosmo/NumCosmo

Build

C headersnumcosmo/numcosmo.h
pkg-config filesnumcosmo

Dependencies

GObject—2.0 The base type system library
Browse documentation
NumCosmoMath—1.0 NumCosmo Math Library
Browse documentation

Additional documentation

Classes

CBE

CLASS (Cosmic Linear Anisotropy Solving System) backend.

CBEPrecision

CLASS (Cosmic Linear Anisotropy Solving System) backend for perturbations.

ClusterAbundance

Cluster abundance distribution.

ClusterMass

Abstract class for cluster mass distributions.

ClusterMassAscaso

Cluster mass-richness distribution model based on Ascaso et al.

ClusterMassBenson

Sunyaev-Zel’dovich cluster mass distribution.

ClusterMassBensonXRay

Sunyaev-Zel’dovich and x-ray cluster abundance mass distribution.

ClusterMassExt

Extended cluster mass-richness distribution model.

ClusterMassLnnormal

Cluster mass ln-normal distribution.

ClusterMassNodist

Cluster mass real mass distribution.

ClusterMassPlCL

Planck-CLASH Cluster Mass Distribution.

ClusterMassRichness

Abstract class for cluster mass-richness observable relations.

ClusterMassSelection

Cluster mass distribution model based on Selection et al.

ClusterMassVanderlinde

Sunyaev-Zel’dovich cluster mass distribution.

ClusterPhotozGauss

Individual gaussian photometric distribution for clusters.

ClusterPhotozGaussGlobal

Global gaussian photometric distribution for clusters.

ClusterPseudoCounts

Model for the pseudo number counts of galaxy clusters.

ClusterRedshift

Abstract class for cluster redshift distributions.

ClusterRedshiftNodist

Cluster abundance redshift real redshift distribution.

CorClusterCmbLensLimber

Cluster and CMB lensing correlation using halo model and Limber approximation.

DataBaoA

Baryon oscillation data — acoustic scale $A$.

DataBaoDHrDAr

Baryon Oscillation Data — $(D_H/r,\; D_A/r)$ data.

DataBaoDMrHr

Baryon Oscillation Data — $(D_M/r,\; H/r)$ data.

DataBaoDtrDHr

Baryon Oscillation Data — $(D_H/r,\; D_t/r)$ data.

DataBaoDV

Baryon oscillation data — volume mean $D_V$.

DataBaoDVDV

Baryon oscillation data — $D_V / D_V$ ratio.

DataBaoDvrDtDh

DataBaoEmpiricalFit

Baryon oscillation data — $D_V / r_s$ empirical likelihood.

DataBaoEmpiricalFit2d

Baryon oscillation data — $D_H / r_d$ and $D_t / r_d$ empirical likelihood.

DataBaoRDV

Baryon Oscillation Data — $r_s / D_V$ ratio.

DataClusterMassRich

Cluster mass richness data object.

DataClusterNCount

Cluster number count data.

DataClusterNCountsGauss

Cluster number count data gaussian likelihood.

DataClusterPseudoCounts

Galaxy clusters data — pseudo number counts likelihood.

DataClusterWL

Cluster weak lensing likelihood.

DataCMBDistPriors

Cosmic microwave background data — distance priors.

DataCMBShiftParam

Cosmic microwave background data — shift parameter.

DataDistMu

Likelihood object for distance modulus data.

DataHubble

Hubble function data.

DataHubbleBao

Hubble function data from BAO.

DataPlanckLKL

Planck Likelihood interface.

DataSNIACov

Type Ia supernovae data with covariance error matrix.

DataXcor

Cross-correlation data object.

DECont

Dark energy contraction perturbations model.

Distance

Cosmological distance and time related quantities.

GalaxyAcf

Galaxy angular correlation function.

GalaxySDObsRedshift

Class describing galaxy sample observed redshift distribution.

GalaxySDObsRedshiftGauss

Class describing photometric redshift observations with gaussian errors.

GalaxySDObsRedshiftPz

GalaxySDObsRedshiftSpec

Class describing spectroscopic redshift observations.

GalaxySDPosition

Class describing galaxy sample position distributions.

GalaxySDPositionFlat

Class describing galaxy sample position distributions with flat distribution.

GalaxySDShape

Class describing galaxy sample shape distribution.

GalaxySDShapeGauss

Class describing a galaxy sample shape distribution with a truncated gaussian p.d.f. convoluted with gaussian noise.

GalaxySDShapeGaussHSC

Class describing a galaxy sample shape distribution with a truncated gaussian p.d.f. convoluted with gaussian noise and accounting for bias. Compatible with Subaru’s Hyper Suprime-Cam (HSC) survey data.

GalaxySDTrueRedshift

Class describing galaxy sample redshift distributions.

GalaxySDTrueRedshiftLSSTSRD

Class describing galaxy sample redshift distributions as in LSST-SRD.

GalaxySelfunc

Galaxy phenomelogical selection function.

GalaxyWLObs

Galaxy weak lensing observation data.

GrowthFunc

Growth function of linear perturbations.

HaloBias

Abstract class for halo bias function type.

HaloBiasDespali

Despali halo bias function type.

HaloBiasPS

Press-Schechter halo bias function type.

HaloBiasSTEllip

Sheth-Tormen elliptical halo bias function type.

HaloBiasSTSpher

Sheth-Tormen spherical halo bias function type.

HaloBiasTinker

Tinker halo bias function type.

HaloCMBhattacharya13

Class defining the Bhattacharya et al. 2013 concentration-mass relation.

HaloCMDiemer15

Class defining the Diemer & Kravtsov 2015 concentration-mass relation. FIXME include reference and equation.

HaloCMDuffy08

Class defining the Duffy et al. 2008 concentration-mass relation. The concentration parameter $c_\Delta$ is given by: $$c_\Delta = A \left(\frac{M_\Delta}{M_\mathrm{pivot}}\right)^B (1+z)^C,$$ where $M_\mathrm{pivot} = 2 \times 10^{12} h^{-1} M_\odot$ and the parameters $(A, B, C)$ depend on the mass definition (mean, critical, or virial).

HaloCMDutton14

Class defining the Dutton et al. 2014 concentration-mass relation.

HaloCMKlypin11

Class defining the Klypin et al. 2011 concentration-mass relation. FIXME Include reference, equation and ranges of mass and reshift.

HaloCMParam

Class defining mass and concentration as parameters.

HaloCMPrada12

Class defining the Prada et al. 2012 concentration-mass relation.

HaloDensityProfile

Abstract class for density profile functions.

HaloDensityProfileDK14

Density profile of Diemer \& Kravtsov type.

HaloDensityProfileEinasto

Density profile of Einasto type.

HaloDensityProfileHernquist

Density profile of Hernquist type.

HaloDensityProfileNFW

Density profile of Navarro-Frenk-White type.

HaloMassFunction

Clusters mass function.

HaloMassSummary

Class describing halo mass summary.

HaloPosition

A class to represent the center of a halo.

HICosmo

Abstract class for implementing homogeneous and isotropic cosmological models.

HICosmoDE

Base class for implementing dark energy models.

HICosmoDECpl

Dark Energy — Chevallier–Polarski–Linder equation of state.

HICosmoDEJbp

Dark Energy — Jassal-Bagla-Padmanabhan equation of state.

HICosmoDEReparamCMB

Dark Energy — CMB reparametrization.

HICosmoDEReparamOk

Dark Energy — reparametrization $\Omega_{x0} \to \Omega_{k0}$.

HICosmoDEWSpline

Dark Energy — spline equation of state.

HICosmoDEXcdm

Dark Energy — constant equation of state.

HICosmoGCG

Generalized Chaplygin Gas.

HICosmoGCGReparamCMB

HICosmoGCGReparamOk

HICosmoIDEM2

Interacting Dark Energy Model.

HICosmoIDEM2ReparamCMB

HICosmoIDEM2ReparamOk

HICosmoLCDM

$\Lambda$CDM model.

HICosmoQConst

Kinetic model — Constant deceleration function.

HICosmoQGRW

Radiation plus $w$-fluid model with a quantum generated bounce phase model.

HICosmoQGW

The $w$-fluid model with a quantum generated bounce phase model.

HICosmoQLinear

Kinetic model — Linear deceleration function.

HICosmoQRBF

Kinetic model — Radial basis function deceleration function.

HICosmoQRBFRprior

HICosmoQSpline

Kinetic model — Spline deceleration function.

HICosmoQSplineContPrior

HICosmoVexp

Single scalar field with an exponential potential.

HIPert

Base class for perturbation in homogeneous and isotropic cosmologies.

HIPertAdiab

Perturbation object for adiabatic mode only.

HIPertBGVar

Perturbation background variables transport object.

HIPertBoltzmann

Base class for perturbative Boltzmann hierarchy.

HIPertBoltzmannCBE

CLASS (Cosmic Linear Anisotropy Solving System) backend for perturbations.

HIPertBoltzmannStd

Perturbations object for standard Boltzmann hierarchy model.

HIPertComp

Base class describing a general perturbation component.

HIPertCompPB

Photon-Baryon plasma compoment.

HIPertEM

Perturbation object for electromagnetic mode.

HIPertFirstOrder

Base class for implementing first order perturbation in a Friedmann background.

HIPertGrav

Base class describing a general first order gravitation theory.

HIPertGravEinstein

First order Einstein equations on a Friedmann background.

HIPertGW

Perturbation object for gravitational wave mode.

HIPertTwoFluids

Perturbation object for a two fluids system.

HIPrim

Abstract class for implementing homogeneous and isotropic primordial cosmological models.

HIPrimAtan

Arctangent modification of the power law primordial spectrum.

HIPrimBPL

Broken power law modification of the power law primordial spectrum.

HIPrimExpc

Exponential cutoff modification of the power law primordial spectrum.

HIPrimPowerLaw

Power law implementation for primordial spectra.

HIPrimSBPL

Smooth Broken power law modification of the power law primordial spectrum.

HIPrimTwoFluids

Two Fluids implementation for primordial spectra.

HIQG1D

Minisuperspace 1D quantum gravity models.

HIReion

Abstract class for implementing homogeneous and isotropic reionization models.

HIReionCamb

CAMB-like reionization object.

HIReionCambReparamTau

CAMB reionization reparametrization $z_\mathrm{reion} \to \tau_\mathrm{reion}$.

MultiplicityFunc

Dark matter halo multiplicity function.

MultiplicityFuncBocquet

Dark matter halo — Bocquet multiplicity function.

MultiplicityFuncCrocce

Dark matter halo — Crocce multiplicity function.

MultiplicityFuncDespali

Dark matter halo — Despali multiplicity function.

MultiplicityFuncJenkins

Dark matter halo — Jenkins multiplicity function.

MultiplicityFuncPS

Dark matter halo — Press-Schechter multiplicity function.

MultiplicityFuncST

Dark matter halo — Sheth-Tormen multiplicity function.

MultiplicityFuncTinker

Dark matter halo — Tinker multiplicity function.

MultiplicityFuncTinkerMeanNormalized

Dark matter halo — Tinker normalized multiplicity function mean matter density.

MultiplicityFuncWarren

Dark matter halo — Warren multiplicity function.

MultiplicityFuncWatson

Dark matter halo — Watson multiplicity function.

PlanckFI

Abstract class for Planck Foreground and Instrument models.

PlanckFICorTT

Planck Foreground and Instrument model for TT correlation maps.

PlanckFICorTTTEEE

Planck Foreground and Instrument model for TT correlation maps.

PowspecML

Abstract class for linear matter power spectrum implementation.

PowspecMLCBE

Linear matter power spectrum from CLASS backend.

PowspecMLSpline

Class for linear matter power spectrum from a 1d-spline.

PowspecMLTransfer

Class for linear matter power spectrum from a transfer function.

PowspecMNL

Abstrac class for non-linear matter power spectrum implementation.

PowspecMNLHaloFit

Nonlinear matter power spectrum from Halofit model.

PriorQSplineCont

Recomb

Abstract class for cosmic recombination.

RecombCBE

Cosmic recombination by Class.

RecombSeager

Cosmic recombination implementing Seager (1999).

ReducedShearCalib

Reduced Shear Calibration.

ReducedShearCalibWtg

Reduced Shear Calibration.

ReducedShearClusterMass

Cluster mass estimation via reduced shear observable.

Scalefactor

Scale factor as a function of the conformal time.

SNIADistCov

Supernovae distance covariance between distance estimates.

TransferFunc

Abstrac class for perturbation transfer function.

TransferFuncBBKS

Bardeen, Bond, Kaiser and Szalay (BBKS) transfer function.

TransferFuncCAMB

Transfer function using CAMB as backend.

TransferFuncEH

Eisenstein-Hu fitting function for the transfer function.

TransferFuncEHNoBaryon

Eisenstein-Hu fitting function for the transfer function with no baryons.

Window

Abstract class for window functions.

WindowGaussian

A gaussian window function.

WindowTophat

A top-hat window function.

WLSurfaceMassDensity

Weak lensing surface mass density.

Xcor

XcorAB

Cross-correlations data storage object.

XcorKernel

Base object for the kernels of projected observables used in cross-correlations.

XcorKernelCluster

Base class for cluster kernels in cross-correlations.

XcorKernelClusterTophat

Implementation of cluster kernel using a top-hat redshift distribution.

XcorKernelCMBISW

Implementation of NcXcorKernel for integrated Sachs-Wolfe (ISW).

XcorKernelCMBLensing

Implementation of NcXcorKernel for CMB lensing.

XcorKernelComponent

Abstract base class for kernel components in cross-correlation calculations.

XcorKernelGal

Implementation of NcXcorKernel for galaxy density.

XcorKerneltSZ

Thermal Sunyaev Zel’dovich effect kernel.

XcorKernelWeakLensing

Implementation of NcXcorKernel for galaxy weak lensing.

XcorLensingEfficiency

Abstract class for computing lensing efficiency.

Interfaces

HIPertIAdiab

HIPertIEM

HIPertIGW

HIPertITwoFluids

Perturbation interface for two fluids system.

Structs

_HaloPositionClass

ClusterAbundanceDataBin

ClusterAbundanceDataBinM

ClusterAbundanceDataBinZ

ClusterAbundanceDataP

DistanceFunc

DistanceFuncZ

GalaxySDObsRedshiftData

GalaxySDObsRedshiftIntegrand

GalaxySDPositionData

GalaxySDPositionIntegrand

GalaxySDShapeData

GalaxySDShapeIntegrand

HICosmoFunc

HICosmoFuncZ

HIPertBGVarDesc

HIPertBGVarYDY

Boxed object containing the current status of the ode system.

HIPertGravInfo

Gravitation section info.

HIPertGravScalar

Boxed object describing scalar modes of the gravitational perturbations.

HIPertGravTensor

Boxed object describing tensor modes of the gravitational perturbations.

HIPertGravTScalar

Boxed object describing scalar modes of the energy-momentum tensor perturbations.

HIPertGravTScalarInfo

Boxed object describing the dependencies of the scalar modes of the gravitational perturbations.

HIPertGravTTensor

Boxed object describing tensor modes of the energy-momentum tensor perturbations.

HIPertGravTVector

Boxed object describing vector modes of the energy-momentum tensor perturbations.

HIPertGravVector

Boxed object describing vector modes of the gravitational perturbations.

HIPertITwoFluidsEOM

Structure used to store the perturbations’ equations of motion coefficients for the two-fluid model.

HIPertITwoFluidsState

Structure used to store the perturbations’ state for the two-fluid model.

HIPertITwoFluidsTV

Structure used to store the perturbations’ transfer functions for the two-fluid model.

HIPertITwoFluidsWKB

Structure representing the WKB approximations of perturbations in the two-fluid model. Stores two approximations, one for each eigenmode, along with their corresponding estimated WKB scales.

HIPertTwoFluidsStateInterp

HIQG1DExp

Exponential wave-function.

HIQG1DGauss

Gaussian wave-function.

HIQG1DSQ

Semi-Quantum approximation fiducial wave-function.

WLSurfaceMassDensityOptzs

Optimization structure.

XcorKernelIntegrand

A reference-counted closure for computing kernel integrands. The eval_func function should fill len values in the W array for the given wavenumber k.

XcorKinetic

A boxed type for the kinetic quantities necessary to compute the kernels.

Aliases

Enumerations

ClusterMassAscasoSParams

Parameters for the Ascaso cluster mass-richness relation.

ClusterMassBensonSParams

Parameters for the Benson cluster mass-SZ relation.

ClusterMassBensonXRaySParams

Parameters for the Benson cluster mass-X-ray relation.

ClusterMassExtSParams

Parameters for the extended cluster mass-richness relation.

ClusterMassImpl

ClusterMassLnnormalSParams

Parameters for the log-normal cluster mass-observable relation.

ClusterMassPlCLSParams

Parameters for the Planck cluster mass relation combining SZ and lensing.

ClusterMassRichnessSParams

Scalar parameters for the cluster mass-richness relation.

ClusterMassSelectionSParams

FIXME.

ClusterMassVanderlindeSParams

Parameters for the Vanderlinde cluster mass-SZ relation.

ClusterPhotozGaussGlobalSParams

Parameters for the global Gaussian photometric redshift distribution.

ClusterPseudoCountsSParams

FIXME.

ClusterRedshiftImpl

DataBaoId

Enumeration of available BAO (Baryon Acoustic Oscillations) datasets.

DataClusterAbundanceId

Cluster abundance data input modes. These specify how the cluster number count data is initialized or used.

DataClusterPseudoCountsObs

DataCMBId

Wilkinson Microwave Anisotropy Probe (WMAP) distance priors and shift parameter estimates.

DataHubbleBaoId

Available BAO samples for Hubble function measurements. These identifiers select specific datasets for the Hubble parameter derived from Baryon Acoustic Oscillation observations.

DataHubbleId

Identifiers for different Hubble parameter observational datasets.

DataPlanckLKLType

The Planck likelihood types.

DataSNIACovOrder

Data ordering for covariance.

DataSNIAId

Supernovae data sets.

DistanceComovingMethod

Enumeration to define which method to be applied in order to compute the cosmological distances.

GalaxySDShapeGaussParams

Gaussian galaxy shape distribution model parameters.

GalaxySDTrueRedshiftLSSTSRDSParams

LSST SRD galaxy redshift distribution model parameters.

GalaxySDTrueRedshiftLSSTSRDType

LSST SRD galaxy redshift distribution types.

GalaxyWLObsCoord

Coordinate system for the galaxy weak lensing ellipticity data.

GalaxyWLObsEllipConv

Method used to compute the ellipticity from the quadrupole moment matrix. The quadrupole matrix can be normalized either by its trace or by a combination of trace and determinant. In both cases, the shape can be described by an ellipse parameterized as $$ \left(\frac{x\cos\theta + y\sin\theta}{a}\right)^2 + \left(\frac{y\cos\theta - x\sin\theta}{b}\right)^2 = 1, $$ where $a$ and $b$ are the semi-major and semi-minor axes, and $\theta$ is the orientation angle.

HaloCMBhattacharya13SParams

Fundamental parametrization of the profile $\rho(r)$. The halo mass is a paremeter while the concentration is given by the Bhattacharya et al. (2013) concentration-mass relation.

HaloCMDiemer15SParams

Fundamental parametrization of the profile $\rho(r)$. The halo mass is a paremeter while the concentration is given by the Diemer & Kravtsov (2015) concentration-mass relation.

HaloCMDuffy08SParams

Fundamental parametrization of the profile $\rho(r)$. The halo mass is a paremeter while the concentration is given by the Duffy et al. (2008) concentration-mass relation.

HaloCMDutton14SParams

Fundamental parametrization of the profile $\rho(r)$. The halo mass is a paremeter while the concentration is given by the Dutton & Macciò (2014) concentration-mass relation.

HaloCMKlypin11SParams

Fundamental parametrization of the profile $\rho(r)$. The halo mass is a paremeter while the concentration is given by the Klypin et al. (2011) concentration-mass relation.

HaloCMParamSParams

Fundamental parametrization of the profile $\rho(r)$. Both mass and concentration are parameters.

HaloCMPrada12SParams

Fundamental parametrization of the profile $\rho(r)$. The halo mass is a paremeter while the concentration is given by the Prada et al. (2012) concentration-mass relation.

HaloDensityProfileDK14MethodParams

Methods for parametrizing the DK14 halo density profile.

HaloDensityProfileDK14Params

The first three parameters, $\rho_s$, $r_s$ and $\alpha$, are the Einasto profile’s parameters. The transition term $f_{trans}$ is a function parametrized by $r_t$, $beta$ and $\gamma$. These two functions determine the inner profile, whereas the outer profile is parametrized br $b_e$ and $s_e$.

HaloDensityProfileEinastoParams

Parameters for the Einasto halo density profile.

HaloMassFunctionSplineOptimize

Options for optimizing spline interpolation in halo mass function calculations.

HaloMassSummaryMassDef

Spherical overdensity halo mass: $$M_\Delta = \frac{4\pi}{3} \Delta \rho_\mathrm{bg} r_\Delta^3,$$ where $\rho_\mathrm{bg}$ is the background density of the universe at redshift z, $\rho_\mathrm{bg} (z)$. For NC_HALO_MASS_SUMMARY_MASS_DEF_VIRIAL the virial overdensity is defined as: \begin{equation}\label{def:DVir} \Delta_\mathrm{Vir} = 18 \pi^2 + 82 x - 39 x^2, \quad x \equiv \Omega_m(z) - 1. \end{equation}.

HaloPositionSParams

Halo center model parameters.

HICosmoDECplSParams

Dark Energy equation of state: $w(z) = w_0 + w_1 \frac{z}{1.0 + z}$.

HICosmoDEJbpSParams

Dark Energy equation of state: $w(z) = w_0 + w_1 \frac{z}{(1.0 + z)^2}$.

HICosmoDESParams

Scalar parameters for dark energy cosmological models. These are the standard cosmological parameters extended to include dark energy contributions.

HICosmoDEVParams

Vector parameters for dark energy cosmological models. These arrays specify properties of massive neutrino species, allowing for multiple neutrino families with different masses and temperatures.

HICosmoDEWSplineVParams

HICosmoDEXCDMSParams

Dark Energy equation of state: $w(z) = w$.

HICosmoGCGSParams

Scalar parameters for the generalized Chaplygin gas cosmological model.

HICosmoGCGVParams

Vector parameters for massive neutrinos in the generalized Chaplygin gas model.

HICosmoIDEM2SParams

Scalar parameters for interacting dark energy-matter cosmology models (IDEM2).

HICosmoIDEM2VParams

Vector parameters for interacting dark energy-matter cosmology models (IDEM2).

HICosmoQConstSParams

HICosmoQGRWSParams

Parameter of the Quantum Gravity Radiation W model.

HICosmoQGWSParams

Parameter of the Quantum Gravity Radiation W model.

HICosmoQLinearSParams

HICosmoQRBFSParams

HICosmoQRBFVParams

HICosmoQSplineSParams

Scalar parameters for Q-spline cosmological model. This parametrization uses splines for the deceleration parameter q(z).

HICosmoQSplineVParams

Vector parameters for Q-spline cosmological model. The deceleration parameter spline knots define the evolution of $q(z)$.

HICosmoVexpEMCoupling

Electromagnetic coupling enumerator.

HICosmoVexpSParams

Scalar field parameters enumerator. This enumerator is used to access the scalar field parameters in the NcHICosmoVexp object.

HIPertAdiabVars

Perturbation variables enumerator.

HIPertBoltzmannVars

Variables for the Boltzmann perturbation equations.

HIPertCompPBVar

Photon-baryon component variables.

HIPertEMVars

Perturbation variables enumerator.

HIPertFirstOrderInteg

ODE integrators.

HIPertGravGauge

Gravitation gauges.

HIPertGravSElem

Elements present in the scalar equations.

HIPertGWVars

Perturbation variables enumerator.

HIPertITwoFluidsObs

Enumeration of physical observables computed from the two-fluid perturbation state.

HIPertITwoFluidsObsMode

Specifies which quantized mode(s) to include when computing two-point observables such as power spectra and correlations.

HIPertITwoFluidsVars

Enumeration of variables used in the two-fluid model.

HIPertTwoFluidsError

Error domain for NcHIPertTwoFluids.

HIPrimAtanSParams

Primordial adiabatic scalar power spectrum: $$ \mathcal{P}{SA}(k) = \xi\mathrm{neq}(k)\mathcal{P}{\mathrm{F}}(k),$$ where $$ \mathcal{P}{\mathrm{F}}(k) \equiv \mathcal{A}\mathrm{s}\left(\frac{k}{k\star}\right)^{n_s -1 } $$ and $$ \xi_\mathrm{neq}(k) = \arctan \left[ \left(\frac{k}{k_\mathrm{c}}\right)^\lambda + c_2\right] - \frac{\pi}{2} + c_3. $$.

HIPrimBPLSParams

Broken power-law primordial power spectrum parameters. These parameters define a primordial power spectrum with a break, useful for modeling features in the inflationary potential.

HIPrimExpcSParams

Parameters for the exponential cutoff primordial spectrum model.

HIPrimPowerLawSParams

Primordial adiabatic scalar power spectrum: $$ \mathcal{P}{SA}(k) = \mathcal{A}\mathrm{s}\left(\frac{k}{k_\star}\right)^{n_s -1 }.$$.

HIPrimSBPLSParams

Parameters for the smooth broken power law primordial spectrum model.

HIPrimTwoFluidsSParams

Parameters for the two fluids primordial power spectrum.

HIReionCambSParams

FIXME.

MultiplicityFuncBocquetSim

MultiplicityFuncMassDef

Spherical overdensity halo mass: $$M_\Delta = \frac{4\pi}{3} \Delta \rho_\mathrm{bg} r_\Delta^3,$$ where $\rho_\mathrm{bg}$ is the background density of the universe at redshift z, $\rho_\mathrm{bg} (z)$. For NC_HALO_DENSITY_PROFILE_MASS_DEF_VIRIAL the virial overdensity is defined as: \begin{equation}\label{def:DVir} \Delta_\mathrm{Vir} = 18 \pi^2 + 82 x - 39 x^2, \quad x \equiv \Omega_m(z) - 1. \end{equation}.

PlanckFICorTTSParams

Planck Foregound and Instrument parameters, compatible with 2013, 2015 and 2018 releases (see [Planck 2015 results XI (2015)][XPlanckCollaboration2015a] and [Planck 2018 results V (2019)][XPlanckCollaboration2019]).

PlanckFICorTTTEEESParams

Planck Foregound and Instrument parameters, compatible with 2013, 2015 and 2018 releases (see [Planck 2015 results XI (2015)][XPlanckCollaboration2015a] and [Planck 2018 results V (2019)][XPlanckCollaboration2019]).

ReducedShearCalibWtgSParams

WtG calibration parameters.

ReducedShearClusterMassParams

These parameters refers to the shear calibration, and the Voigt profile.

SNIADistCovSParams

SN Ia distance covariance model parameters.

SNIADistCovVParams

SN Ia distance covariance model parameters.

TransferFuncBBKSType

BBKS transfer function variant.

WLSurfaceMassDensityParams

FIXME.

XcorKernelCMBLensingSParams

Scalar parameters for CMB lensing kernel (currently none defined).

XcorKernelGalSParams

XcorKernelGalVParams

XcorKernelImpl

XcorKerneltSZSParams

Enum values for the tSZ kernel parameters.

XcorKernelWeakLensingSParams

XcorKernelWeakLensingVParams

XcorMethod

Methods to compute integrals.

Bitfields

DataClusterWLResampleFlag

DataCMBDataType

Each type corresponds to one CMB two-point correlation function data to be used: TT (temperature only), EE (E-mode only), BB (B-mode only), TE (temperature and E-mode polarization), TB (temperature and B-mode polarization), EB (E- and B-mode polarization) and $\phi\phi$ (CMB lensing). The last option `ALL’ selects all data listed above.

HICosmoDEImpl

Implementation flags for dark energy models. These flags indicate which virtual methods are implemented by a specific dark energy model subclass.

HICosmoImpl

Flags defining the implementation options of the NcHICosmo abstract object.

HIPrimImpl

Methods to be implementd by every primordial model.

RecombSeagerOpt

FIXME.

Error Domains

DataSNIACovError

NcDataSNIACov error messages.

Callbacks

CBECall

CBEFree

ClusterAbundanceIntPd2N

ClusterAbundanceIntPd2NBias

ClusterAbundanceN

DistanceFunc0

DistanceFunc1

GalaxySDObsRedshiftIntegrandCopyData

GalaxySDObsRedshiftIntegrandFreeData

GalaxySDObsRedshiftIntegrandFunc

GalaxySDObsRedshiftIntegrandPrepareData

GalaxySDPositionIntegrandCopyData

GalaxySDPositionIntegrandFreeData

GalaxySDPositionIntegrandFunc

GalaxySDPositionIntegrandPrepareData

GalaxySDShapeIntegrandCopyData

GalaxySDShapeIntegrandFreeData

GalaxySDShapeIntegrandFunc

GalaxySDShapeIntegrandPrepareData

HICosmoDEFunc1

HICosmoFunc0

HICosmoFunc1K

HICosmoFunc1Z

HICosmoFuncMassNuInfo

HICosmoFuncNMassNu

HICosmoGCGFunc1

HICosmoGetBGVar

HICosmoIDEM2Func1

HICosmoVFunc0

HICosmoVFunc1K

HICosmoVFunc1Z

HIPertBoltzmannConf

HIPertBoltzmannCreate

HIPertBoltzmannEvol

HIPertBoltzmannGet

HIPertBoltzmannGetCl

HIPertBoltzmannGetN

HIPertBoltzmannPrepare

HIPertBoltzmannSources

HIPertBoltzmannTest

HIPertCompDeps

HIPertCompGetDYScalar

HIPertCompGetGauge

HIPertCompGetTScalar

HIPertCompGetTScalarInfo

HIPertCompGetTTensor

HIPertCompGetTVector

HIPertCompNDynVar

HIPertCompSetGauge

HIPertGravDeps

HIPertGravGetDYScalar

HIPertGravGetGauge

HIPertGravGetScalar

HIPertGravGetScalarInfo

HIPertGravNDynVar

HIPertGravSetGauge

HIPertITwoFluidsFuncEOM

HIPertITwoFluidsFuncTV

HIPertITwoFluidsFuncWKB

HIPertTwoFluidsLogger

HIPrimFunc1

HIQG1DPsi

Wave-function.

RecombSeagerKHeI2p

RecombSeagerKHeI2pGrad

RecombSeagerKHI2p2Pmean

XcorKernelComponentEvalKernel

Evaluates the kernel function K(k, xi) at the given comoving distance and wave number.

XcorKernelComponentEvalPrefactor

Evaluates the prefactor that may depend on k and â„“.

XcorKernelComponentGetLimits

Gets the valid integration ranges for this component.

XcorKernelIntegrandEval

Function type for evaluating kernel integrands.

XcorKernelIntegrandGetRange

Function type for getting the valid k range.

XcorLensingEfficiencyEvalSource

Evaluates the source weight function $W_{\mathrm{src}}(z)$ for the lensing efficiency computation. This is used in the integral: \begin{equation} g(z) = \int_z^{z_{\max}} dz’ \left(1 - \frac{\chi(z)}{\chi(z’)}\right) W_{\mathrm{src}}(z’) \end{equation}.

XcorLensingEfficiencyGetZRange

Returns the redshift range for the source distribution used in lensing efficiency computation.

Function Macros

CBE_CLASS

CBE_PRECISION

CBE_PRECISION_CLASS

cluster_abundance_d2NdzdlnM_val

cluster_abundance_dNdlnM_val

cluster_abundance_dNdz_val

cluster_abundance_N_val

CLUSTER_MASS_BENSON_XRAY

CLUSTER_MASS_BENSON_XRAY_CLASS

CLUSTER_MASS_PLCL

CLUSTER_MASS_PLCL_CLASS

DATA_CLUSTER_NCOUNT

DATA_CLUSTER_NCOUNT_CLASS

DATA_CLUSTER_NCOUNTS_GAUSS

DATA_CLUSTER_NCOUNTS_GAUSS_CLASS

DATA_CMB_DIST_PRIORS

DATA_CMB_DIST_PRIORS_CLASS

DATA_CMB_SHIFT_PARAM

DATA_CMB_SHIFT_PARAM_CLASS

DATA_DIST_MU

DATA_DIST_MU_CLASS

HALO_DENSITY_PROFILE_DK14

HALO_DENSITY_PROFILE_DK14_CLASS

HICOSMO

HICOSMO_CLASS

HICOSMO_DE

HICOSMO_DE_CLASS

HICOSMO_DE_CPL

HICOSMO_DE_CPL_CLASS

HICOSMO_DE_JBP

HICOSMO_DE_JBP_CLASS

HICOSMO_DE_REPARAM_CMB

HICOSMO_DE_REPARAM_CMB_CLASS

HICOSMO_DE_REPARAM_OK

HICOSMO_DE_REPARAM_OK_CLASS

HICOSMO_DE_WSPLINE

HICOSMO_DE_WSPLINE_CLASS

HICOSMO_DE_XCDM

HICOSMO_DE_XCDM_CLASS

HICOSMO_GCG

HICOSMO_GCG_CLASS

HICOSMO_GCG_REPARAM_CMB

HICOSMO_GCG_REPARAM_CMB_CLASS

HICOSMO_GCG_REPARAM_OK

HICOSMO_GCG_REPARAM_OK_CLASS

HICOSMO_IDEM2

HICOSMO_IDEM2_CLASS

HICOSMO_IDEM2_REPARAM_CMB

HICOSMO_IDEM2_REPARAM_CMB_CLASS

HICOSMO_IDEM2_REPARAM_OK

HICOSMO_IDEM2_REPARAM_OK_CLASS

HICOSMO_LCDM

HICOSMO_LCDM_CLASS

HICOSMO_QCONST

HICOSMO_QCONST_CLASS

HICOSMO_QGRW

HICOSMO_QGRW_CLASS

HICOSMO_QGW

HICOSMO_QGW_CLASS

HICOSMO_QLINEAR

HICOSMO_QLINEAR_CLASS

HICOSMO_QRBF

HICOSMO_QRBF_CLASS

HICOSMO_QRBF_RPRIOR

HICOSMO_QRBF_RPRIOR_CLASS

HICOSMO_QSPLINE

HICOSMO_QSPLINE_CLASS

HICOSMO_QSPLINE_CONT_PRIOR

HICOSMO_QSPLINE_CONT_PRIOR_CLASS

HICOSMO_VEXP

HICOSMO_VEXP_CLASS

HIPERT_BG_VAR

HIPERT_BG_VAR_CLASS

HIPERT_BG_VAR_ID_FUNC

Macro to generate the id function name for a background variable.

HIPERT_BG_VAR_ID_FUNC_DECL

Declare the id function associated with obj_ns.

HIPERT_BG_VAR_ID_FUNC_IMPL

The implementation of the id function associated with obj_ns.

HIPERT_BOLTZMANN

HIPERT_BOLTZMANN_CBE

HIPERT_BOLTZMANN_CBE_CLASS

HIPERT_BOLTZMANN_CLASS

HIPERT_BOLTZMANN_LAMBDA2X

HIPERT_BOLTZMANN_STD

HIPERT_BOLTZMANN_STD_CLASS

HIPERT_BOLTZMANN_THETA

HIPERT_BOLTZMANN_THETA_P

HIPERT_BOLTZMANN_X2LAMBDA

HIPERT_COMP

HIPERT_COMP_CLASS

HIPERT_COMP_PB

HIPERT_COMP_PB_CLASS

HIPERT_COMP_PB_VAR_F_G

HIPERT_FIRST_ORDER

HIPERT_FIRST_ORDER_CLASS

HIPERT_GRAV

HIPERT_GRAV_CLASS

HIPERT_GRAV_DYN_VAR

HIPERT_GRAV_EINSTEIN

HIPERT_GRAV_EINSTEIN_CLASS

HIPERT_TWO_FLUIDS_A2P

HIPERT_TWO_FLUIDS_A2Q

HIPERT_TWO_FLUIDS_QP2A

HIPRIM

HIPRIM_ATAN

HIPRIM_ATAN_CLASS

HIPRIM_BPL

HIPRIM_BPL_CLASS

HIPRIM_CLASS

HIPRIM_EXPC

HIPRIM_EXPC_CLASS

HIPRIM_POWER_LAW

HIPRIM_POWER_LAW_CLASS

HIPRIM_SBPL

HIPRIM_SBPL_CLASS

HIPRIM_TWO_FLUIDS

HIPRIM_TWO_FLUIDS_CLASS

HIQG_1D

HIQG_1D_CLASS

HIREION

HIREION_CAMB

HIREION_CAMB_CLASS

HIREION_CAMB_REPARAM_TAU

HIREION_CAMB_REPARAM_TAU_CLASS

HIREION_CLASS

PLANCK_FI_COR_TTTEEE

PLANCK_FI_COR_TTTEEE_CLASS

POWSPEC_ML_CBE

POWSPEC_ML_CBE_CLASS

POWSPEC_MNL

POWSPEC_MNL_CLASS

POWSPEC_MNL_HALOFIT

POWSPEC_MNL_HALOFIT_CLASS

PRIOR_QSPLINE_CONT

PRIOR_QSPLINE_CONT_CLASS

RECOMB_CBE

RECOMB_CBE_CLASS

SNIA_DIST_COV

SNIA_DIST_COV_CLASS

XCOR_KERNEL_COMPONENT_DEFINE_TYPE

A convenience macro to define a subclass of NcXcorKernelComponent with a custom user data type.

XCOR_LENSING_EFFICIENCY_DEFINE_TYPE

A convenience macro to define a subclass of NcXcorLensingEfficiency with a custom user data type. This follows the same pattern as NcmIntegralND for inline type definition.

Constants

CLUSTER_MASS_ASCASO_DEFAULT_MU_P0

CLUSTER_MASS_ASCASO_DEFAULT_MU_P1

CLUSTER_MASS_ASCASO_DEFAULT_MU_P2

CLUSTER_MASS_ASCASO_DEFAULT_PARAMS_ABSTOL

CLUSTER_MASS_ASCASO_DEFAULT_SIGMA_P0

CLUSTER_MASS_ASCASO_DEFAULT_SIGMA_P1

CLUSTER_MASS_ASCASO_DEFAULT_SIGMA_P2

CLUSTER_MASS_BENSON_DEFAULT_A_SZ

CLUSTER_MASS_BENSON_DEFAULT_B_SZ

CLUSTER_MASS_BENSON_DEFAULT_C_SZ

CLUSTER_MASS_BENSON_DEFAULT_D_SZ

CLUSTER_MASS_BENSON_DEFAULT_PARAMS_ABSTOL

CLUSTER_MASS_BENSON_M_LOWER_BOUND

CLUSTER_MASS_BENSON_XI_ZETA_DIST_CUT

CLUSTER_MASS_BENSON_XRAY_DEFAULT_A_X

CLUSTER_MASS_BENSON_XRAY_DEFAULT_B_X

CLUSTER_MASS_BENSON_XRAY_DEFAULT_C_X

CLUSTER_MASS_BENSON_XRAY_DEFAULT_D_X

CLUSTER_MASS_BENSON_XRAY_DEFAULT_PARAMS_ABSTOL

CLUSTER_MASS_EXT_DEFAULT_MU_P0

CLUSTER_MASS_EXT_DEFAULT_MU_P1

CLUSTER_MASS_EXT_DEFAULT_MU_P2

CLUSTER_MASS_EXT_DEFAULT_MU_P3

CLUSTER_MASS_EXT_DEFAULT_PARAMS_ABSTOL

CLUSTER_MASS_EXT_DEFAULT_SIGMA_P0

CLUSTER_MASS_EXT_DEFAULT_SIGMA_P1

CLUSTER_MASS_EXT_DEFAULT_SIGMA_P2

CLUSTER_MASS_LNNORMAL_DEFAULT_BIAS

CLUSTER_MASS_LNNORMAL_DEFAULT_PARAMS_ABSTOL

CLUSTER_MASS_LNNORMAL_DEFAULT_SIGMA

CLUSTER_MASS_PLCL_DEFAULT_A_L

CLUSTER_MASS_PLCL_DEFAULT_A_SZ

CLUSTER_MASS_PLCL_DEFAULT_B_L

CLUSTER_MASS_PLCL_DEFAULT_B_SZ

CLUSTER_MASS_PLCL_DEFAULT_COR

CLUSTER_MASS_PLCL_DEFAULT_PARAMS_ABSTOL

CLUSTER_MASS_PLCL_DEFAULT_SD_L

CLUSTER_MASS_PLCL_DEFAULT_SD_SZ

CLUSTER_MASS_PLCL_MCL

CLUSTER_MASS_PLCL_MPL

CLUSTER_MASS_PLCL_SD_CL

CLUSTER_MASS_PLCL_SD_PL

CLUSTER_MASS_RICHNESS_DEFAULT_CUT

CLUSTER_MASS_RICHNESS_DEFAULT_PARAMS_ABSTOL

CLUSTER_MASS_SELECTION_DEFAULT_CUT

CLUSTER_MASS_SELECTION_DEFAULT_MU_P0

CLUSTER_MASS_SELECTION_DEFAULT_MU_P1

CLUSTER_MASS_SELECTION_DEFAULT_MU_P2

CLUSTER_MASS_SELECTION_DEFAULT_PARAMS_ABSTOL

CLUSTER_MASS_SELECTION_DEFAULT_SIGMA_P0

CLUSTER_MASS_SELECTION_DEFAULT_SIGMA_P1

CLUSTER_MASS_SELECTION_DEFAULT_SIGMA_P2

CLUSTER_MASS_VANDERLINDE_DEFAULT_A_SZ

CLUSTER_MASS_VANDERLINDE_DEFAULT_B_SZ

CLUSTER_MASS_VANDERLINDE_DEFAULT_C_SZ

CLUSTER_MASS_VANDERLINDE_DEFAULT_D_SZ

CLUSTER_MASS_VANDERLINDE_DEFAULT_PARAMS_ABSTOL

CLUSTER_PHOTOZ_GAUSS_BIAS

CLUSTER_PHOTOZ_GAUSS_SIGMA

CLUSTER_PSEUDO_COUNTS_DEFAULT_DELTAZ

CLUSTER_PSEUDO_COUNTS_DEFAULT_LNMCUT

CLUSTER_PSEUDO_COUNTS_DEFAULT_PARAMS_ABSTOL

CLUSTER_PSEUDO_COUNTS_DEFAULT_SD_MCUT

CLUSTER_PSEUDO_COUNTS_DEFAULT_ZMIN

CLUSTER_REDSHIFT_PHOTOZ_GAUSS_GLOBAL_DEFAULT_BIAS

CLUSTER_REDSHIFT_PHOTOZ_GAUSS_GLOBAL_DEFAULT_PARAMS_ABSTOL

CLUSTER_REDSHIFT_PHOTOZ_GAUSS_GLOBAL_DEFAULT_SIGMA0

DATA_BAO_RDV_LEN

DATA_CLUSTER_PSEUDO_COUNTS_RESAMPLE_MAX_TRIES

DATA_SNIA_COV_LEN

DATA_SNIA_SIMPLE_LEN

DATA_XCOR_DL

DATA_XCOR_MAX

GALAXY_SD_OBS_REDSHIFT_COL_Z

GALAXY_SD_OBS_REDSHIFT_GAUSS_COL_SIGMA

GALAXY_SD_OBS_REDSHIFT_GAUSS_COL_SIGMA0

GALAXY_SD_OBS_REDSHIFT_GAUSS_COL_ZP

GALAXY_SD_POSITION_COL_DEC

GALAXY_SD_POSITION_COL_RA

GALAXY_SD_SHAPE_COL_COORD

GALAXY_SD_SHAPE_COL_EPSILON_INT_1

GALAXY_SD_SHAPE_COL_EPSILON_INT_2

GALAXY_SD_SHAPE_GAUSS_COL_EPSILON_OBS_1

GALAXY_SD_SHAPE_GAUSS_COL_EPSILON_OBS_2

GALAXY_SD_SHAPE_GAUSS_COL_STD_NOISE

GALAXY_SD_SHAPE_GAUSS_DEFAULT_PARAMS_ABSTOL

GALAXY_SD_SHAPE_GAUSS_DEFAULT_SIGMA

GALAXY_SD_SHAPE_GAUSS_HSC_COL_C1

GALAXY_SD_SHAPE_GAUSS_HSC_COL_C2

GALAXY_SD_SHAPE_GAUSS_HSC_COL_EPSILON_OBS_1

GALAXY_SD_SHAPE_GAUSS_HSC_COL_EPSILON_OBS_2

GALAXY_SD_SHAPE_GAUSS_HSC_COL_M

GALAXY_SD_SHAPE_GAUSS_HSC_COL_STD_NOISE

GALAXY_SD_SHAPE_GAUSS_HSC_COL_STD_SHAPE

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_DEFAULT_PARAMS_ABSTOL

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_DEFAULT_Z_HIGH

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_DEFAULT_Z_LOW

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y10_LENS_ALPHA

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y10_LENS_BETA

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y10_LENS_Z0

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y10_SOURCE_ALPHA

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y10_SOURCE_BETA

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y10_SOURCE_Z0

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y1_LENS_ALPHA

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y1_LENS_BETA

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y1_LENS_Z0

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y1_SOURCE_ALPHA

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y1_SOURCE_BETA

GALAXY_SD_TRUE_REDSHIFT_LSST_SRD_Y1_SOURCE_Z0

HALO_CM_BHATTACHARYA13_DEFAULT_PARAMS_ABSTOL

HALO_CM_BHATTACHARYA13_LOCAL_SPARAM_LEN

HALO_CM_DIEMER15_DEFAULT_PARAMS_ABSTOL

HALO_CM_DIEMER15_LOCAL_SPARAM_LEN

HALO_CM_DUFFY08_DEFAULT_PARAMS_ABSTOL

HALO_CM_DUFFY08_LOCAL_SPARAM_LEN

HALO_CM_DUTTON14_DEFAULT_PARAMS_ABSTOL

HALO_CM_DUTTON14_LOCAL_SPARAM_LEN

HALO_CM_KLYPIN11_DEFAULT_PARAMS_ABSTOL

HALO_CM_KLYPIN11_LOCAL_SPARAM_LEN

HALO_CM_PARAM_DEFAULT_C_DELTA

HALO_CM_PARAM_DEFAULT_PARAMS_ABSTOL

HALO_CM_PARAM_LOCAL_SPARAM_LEN

HALO_CM_PRADA12_DEFAULT_PARAMS_ABSTOL

HALO_CM_PRADA12_LOCAL_SPARAM_LEN

HALO_DENSITY_PROFILE_DK14_DEFAULT_BETA

HALO_DENSITY_PROFILE_DK14_DEFAULT_PARAMS_ABSTOL

HALO_DENSITY_PROFILE_DK14_DEFAULT_RT

HALO_DENSITY_PROFILE_EINASTO_DEFAULT_ALPHA

HALO_DENSITY_PROFILE_EINASTO_DEFAULT_PARAMS_ABSTOL

HALO_DENSITY_PROFILE_EINASTO_LOCAL_SPARAM_LEN

HALO_POSITION_DEFAULT_DEC

HALO_POSITION_DEFAULT_PARAMS_ABSTOL

HALO_POSITION_DEFAULT_RA

HALO_POSITION_DEFAULT_Z

HICOSMO_DE_CPL_DEFAULT_W0

HICOSMO_DE_CPL_DEFAULT_W1

HICOSMO_DE_CPL_N

HICOSMO_DE_DEFAULT_ENNU

HICOSMO_DE_DEFAULT_HE_YP

HICOSMO_DE_DEFAULT_NU_G

HICOSMO_DE_DEFAULT_NU_MASS

HICOSMO_DE_DEFAULT_NU_MU

HICOSMO_DE_DEFAULT_NU_T

HICOSMO_DE_DEFAULT_OMEGA_B

HICOSMO_DE_DEFAULT_OMEGA_C

HICOSMO_DE_DEFAULT_OMEGA_X

HICOSMO_DE_DEFAULT_T_GAMMA0

HICOSMO_DE_JBP_DEFAULT_W0

HICOSMO_DE_JBP_DEFAULT_W1

HICOSMO_DE_WSPLINE_DEFAULT_W0

HICOSMO_DE_WSPLINE_N

HICOSMO_DE_XCDM_DEFAULT_W0

HICOSMO_DE_XCDM_N

HICOSMO_DEFAULT_PARAMS_ABSTOL

HICOSMO_DEFAULT_PARAMS_RELTOL

HICOSMO_GCG_DEFAULT_ENNU

HICOSMO_GCG_DEFAULT_GAMMA

HICOSMO_GCG_DEFAULT_HE_YP

HICOSMO_GCG_DEFAULT_NU_G

HICOSMO_GCG_DEFAULT_NU_MASS

HICOSMO_GCG_DEFAULT_NU_MU

HICOSMO_GCG_DEFAULT_NU_T

HICOSMO_GCG_DEFAULT_OMEGA_B

HICOSMO_GCG_DEFAULT_OMEGA_C

HICOSMO_GCG_DEFAULT_OMEGA_X

HICOSMO_GCG_DEFAULT_T_GAMMA0

HICOSMO_IDEM2_DEFAULT_ENNU

HICOSMO_IDEM2_DEFAULT_GAMMA

HICOSMO_IDEM2_DEFAULT_HE_YP

HICOSMO_IDEM2_DEFAULT_NU_G

HICOSMO_IDEM2_DEFAULT_NU_MASS

HICOSMO_IDEM2_DEFAULT_NU_MU

HICOSMO_IDEM2_DEFAULT_NU_T

HICOSMO_IDEM2_DEFAULT_OMEGA_B

HICOSMO_IDEM2_DEFAULT_OMEGA_C

HICOSMO_IDEM2_DEFAULT_OMEGA_X

HICOSMO_IDEM2_DEFAULT_T_GAMMA0

HICOSMO_OMEGA_K0_LIMIT

HICOSMO_QCONST_DEFAULT_CD

HICOSMO_QCONST_DEFAULT_E

HICOSMO_QCONST_DEFAULT_OMEGA_T

HICOSMO_QCONST_DEFAULT_Q

HICOSMO_QCONST_DEFAULT_Z1

HICOSMO_QGRW_DEFAULT_OMEGA_R

Default $\Omega_{r0}$.

HICOSMO_QGRW_DEFAULT_OMEGA_W

Default $\Omega_{w0}$.

HICOSMO_QGRW_DEFAULT_W

Default $w$.

HICOSMO_QGRW_DEFAULT_X_B

HICOSMO_QGW_DEFAULT_OMEGA_W

Default $\Omega_{w0}$.

HICOSMO_QGW_DEFAULT_W

Default $w$.

HICOSMO_QGW_DEFAULT_X_B

HICOSMO_QLINEAR_DEFAULT_CD

HICOSMO_QLINEAR_DEFAULT_E

HICOSMO_QLINEAR_DEFAULT_OMEGA_T

HICOSMO_QLINEAR_DEFAULT_Q

HICOSMO_QLINEAR_DEFAULT_QP

HICOSMO_QLINEAR_DEFAULT_Z1

HICOSMO_QRBF_DEFAULT_AS_DRAG

HICOSMO_QRBF_DEFAULT_H0

HICOSMO_QRBF_DEFAULT_OMEGA_T

HICOSMO_QRBF_DEFAULT_RBF_CENTERS

HICOSMO_QRBF_DEFAULT_RBF_CENTERS_LEN

HICOSMO_QRBF_DEFAULT_RBF_COEFFS

HICOSMO_QRBF_DEFAULT_RBF_COEFFS_LEN

HICOSMO_QRBF_DEFAULT_RBF_H

HICOSMO_QSPLINE_CONT_PRIOR_ABSTOL

HICOSMO_QSPLINE_CONT_PRIOR_LNSIGMA

HICOSMO_QSPLINE_DEFAULT_AS_DRAG

HICOSMO_QSPLINE_DEFAULT_OMEGA_T

HICOSMO_QSPLINE_DEFAULT_Q

HICOSMO_QSPLINE_DEFAULT_Q_LEN

HICOSMO_VEXP_DEBUG_EVOL_CL

HICOSMO_VEXP_DEBUG_EVOL_QT

HICOSMO_VEXP_DEFAULT_ALPHA_B

HICOSMO_VEXP_DEFAULT_D_PHI

HICOSMO_VEXP_DEFAULT_EM_ALPHA

HICOSMO_VEXP_DEFAULT_EM_BETA

HICOSMO_VEXP_DEFAULT_H0

HICOSMO_VEXP_DEFAULT_OMEGA_C

HICOSMO_VEXP_DEFAULT_OMEGA_L

HICOSMO_VEXP_DEFAULT_SIGMA_PHI

HICOSMO_VEXP_DEFAULT_X_B

HIPERT_BG_VAR_DEFAULT_ZF

HIPERT_BOLTZMANN_BASE_SIZE

HIPRIM_ATAN_DEFAULT_C2

HIPRIM_ATAN_DEFAULT_C3

HIPRIM_ATAN_DEFAULT_LAMBDA

HIPRIM_ATAN_DEFAULT_LN10E10ASA

HIPRIM_ATAN_DEFAULT_LNKC

HIPRIM_ATAN_DEFAULT_N_SA

HIPRIM_ATAN_DEFAULT_N_T

HIPRIM_ATAN_DEFAULT_T_SA_RATIO

HIPRIM_BPL_DEFAULT_DELTA

HIPRIM_BPL_DEFAULT_LN10E10ASA

HIPRIM_BPL_DEFAULT_LNKB

HIPRIM_BPL_DEFAULT_N_SA

HIPRIM_BPL_DEFAULT_N_T

HIPRIM_BPL_DEFAULT_T_SA_RATIO

HIPRIM_DEFAULT_K_PIVOT

HIPRIM_DEFAULT_PARAMS_ABSTOL

HIPRIM_DEFAULT_PARAMS_RELTOL

HIPRIM_EXPC_DEFAULT_C

HIPRIM_EXPC_DEFAULT_LAMBDAC

HIPRIM_EXPC_DEFAULT_LN10E10ASA

HIPRIM_EXPC_DEFAULT_LNKC

HIPRIM_EXPC_DEFAULT_N_SA

HIPRIM_EXPC_DEFAULT_N_T

HIPRIM_EXPC_DEFAULT_T_SA_RATIO

HIPRIM_POWER_LAW_DEFAULT_LN10E10ASA

HIPRIM_POWER_LAW_DEFAULT_N_SA

HIPRIM_POWER_LAW_DEFAULT_N_T

HIPRIM_POWER_LAW_DEFAULT_T_SA_RATIO

HIPRIM_SBPL_DEFAULT_DELTA

HIPRIM_SBPL_DEFAULT_LAMBDA

HIPRIM_SBPL_DEFAULT_LN10E10ASA

HIPRIM_SBPL_DEFAULT_LNKB

HIPRIM_SBPL_DEFAULT_N_SA

HIPRIM_SBPL_DEFAULT_N_T

HIPRIM_SBPL_DEFAULT_RA

HIPRIM_SBPL_DEFAULT_T_SA_RATIO

HIPRIM_TWO_FLUIDS_DEFAULT_LN10E10ASA

HIPRIM_TWO_FLUIDS_DEFAULT_LNK0

HIPRIM_TWO_FLUIDS_DEFAULT_LNW

HIPRIM_TWO_FLUIDS_DEFAULT_N_T

HIPRIM_TWO_FLUIDS_DEFAULT_T_SA_RATIO

HIREION_CAMB_DEFAULT_HEIII_REION_DELTA

HIREION_CAMB_DEFAULT_HEIII_Z

HIREION_CAMB_DEFAULT_HII_HEII_REION_DELTA

HIREION_CAMB_DEFAULT_HII_HEII_REION_EXPO

HIREION_CAMB_DEFAULT_HII_HEII_Z

HIREION_DEFAULT_PARAMS_ABSTOL

MULTIPLICITY_FUNC_DELTA_C0

PLANCK_FI_COR_TT_DEFAULT_A_cib_217

PLANCK_FI_COR_TT_DEFAULT_A_planck

PLANCK_FI_COR_TT_DEFAULT_A_sbpx_100_100_TT

PLANCK_FI_COR_TT_DEFAULT_A_sbpx_143_143_TT

PLANCK_FI_COR_TT_DEFAULT_A_sbpx_143_217_TT

PLANCK_FI_COR_TT_DEFAULT_A_sbpx_217_217_TT

PLANCK_FI_COR_TT_DEFAULT_A_sz

PLANCK_FI_COR_TT_DEFAULT_calib_100T

PLANCK_FI_COR_TT_DEFAULT_calib_217T

PLANCK_FI_COR_TT_DEFAULT_cib_index

PLANCK_FI_COR_TT_DEFAULT_gal545_A_100

PLANCK_FI_COR_TT_DEFAULT_gal545_A_143

PLANCK_FI_COR_TT_DEFAULT_gal545_A_143_217

PLANCK_FI_COR_TT_DEFAULT_gal545_A_217

PLANCK_FI_COR_TT_DEFAULT_ksz_norm

PLANCK_FI_COR_TT_DEFAULT_ps_A_100_100

PLANCK_FI_COR_TT_DEFAULT_ps_A_143_143

PLANCK_FI_COR_TT_DEFAULT_ps_A_143_217

PLANCK_FI_COR_TT_DEFAULT_ps_A_217_217

PLANCK_FI_COR_TT_DEFAULT_xi_sz_cib

PLANCK_FI_COR_TTTEEE_DEFAULT_A_cnoise_e2e_100_100_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_A_cnoise_e2e_143_143_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_A_cnoise_e2e_217_217_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_A_pol

PLANCK_FI_COR_TTTEEE_DEFAULT_A_sbpx_100_100_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_A_sbpx_100_143_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_A_sbpx_100_217_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_A_sbpx_143_143_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_A_sbpx_143_217_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_A_sbpx_217_217_EE

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_0E_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_0E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_0E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_0T_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_0T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_0T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_1E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_1E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_1T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_1T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_2E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_0_2T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_0E_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_0E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_0E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_0T_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_0T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_0T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_1E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_1E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_1T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_1T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_2E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_1_2T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_0E_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_0E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_0E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_0T_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_0T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_0T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_1E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_1E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_1T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_1T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_2E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_2_2T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_0E_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_0E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_0E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_0T_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_0T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_0T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_1E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_1E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_1T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_1T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_2E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_3_2T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_0E_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_0E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_0E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_0T_0E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_0T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_0T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_1E_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_1E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_1T_1E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_1T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_2E_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_bleak_epsilon_4_2T_2E

PLANCK_FI_COR_TTTEEE_DEFAULT_calib_100P

PLANCK_FI_COR_TTTEEE_DEFAULT_calib_143P

PLANCK_FI_COR_TTTEEE_DEFAULT_calib_217P

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_EE_A_100

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_EE_A_100_143

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_EE_A_100_217

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_EE_A_143

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_EE_A_143_217

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_EE_A_217

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_EE_index

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_TE_A_100

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_TE_A_100_143

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_TE_A_100_217

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_TE_A_143

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_TE_A_143_217

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_TE_A_217

PLANCK_FI_COR_TTTEEE_DEFAULT_galf_TE_index

PLANCK_FI_DEFAULT_PARAMS_ABSTOL

POWSPEC_ML_CBE_INTERN_KMAX

POWSPEC_ML_CBE_INTERN_KMIN

POWSPEC_MNL_HALOFIT_F1aPOW

POWSPEC_MNL_HALOFIT_F1bPOW

POWSPEC_MNL_HALOFIT_F2aPOW

POWSPEC_MNL_HALOFIT_F2bPOW

POWSPEC_MNL_HALOFIT_F3aPOW

POWSPEC_MNL_HALOFIT_F3bPOW

POWSPEC_MNL_HALOFIT_LOGRMIN

RECOMB_SEAGER_HUMMER_HEI_CASE_B_P

RECOMB_SEAGER_HUMMER_HEI_CASE_B_P_TRIP

RECOMB_STARTING_X

REDUCED_SHEAR_CLUSTER_MASS_DEFAULT_A

REDUCED_SHEAR_CLUSTER_MASS_DEFAULT_B

REDUCED_SHEAR_CLUSTER_MASS_DEFAULT_C

REDUCED_SHEAR_CLUSTER_MASS_DEFAULT_PARAMS_ABSTOL

REDUCED_SHEAR_CLUSTER_MASS_DEFAULT_VGAMMA

REDUCED_SHEAR_CLUSTER_MASS_DEFAULT_VSIGMA

REDUCED_SHEAR_CLUSTER_MASS_DEFAULT_XP

SCALEFACTOR_DEFAULT_A0

SCALEFACTOR_DEFAULT_ABSTOL

SCALEFACTOR_DEFAULT_RELTOL

SCALEFACTOR_DEFAULT_ZF

SCALEFACTOR_MIN_ETA_STEP

SCALEFACTOR_OMEGA_K_ZERO

SNIA_DIST_COV_DEFAULT_ALPHA

SNIA_DIST_COV_DEFAULT_BETA

SNIA_DIST_COV_DEFAULT_M1

SNIA_DIST_COV_DEFAULT_M2

SNIA_DIST_COV_DEFAULT_MU

SNIA_DIST_COV_DEFAULT_PARAMS_ABSTOL

SNIA_DIST_COV_LNSIGMA_INT_DEFAULT_LEN

SNIA_DIST_COV_MU_DEFAULT_LEN

WINDOW_VOLUME_GAUSSIAN

WINDOW_VOLUME_TOPHAT

WL_SURFACE_MASS_DENSITY_DEFAULT_PARAMS_ABSTOL

WL_SURFACE_MASS_DENSITY_DEFAULT_PCC

WL_SURFACE_MASS_DENSITY_DEFAULT_ROFF

XCOR_KERNEL_CMB_ISW_DEFAULT_PARAMS_ABSTOL

XCOR_KERNEL_CMB_LENSING_DEFAULT_PARAMS_ABSTOL

XCOR_KERNEL_COMPONENT_DEFAULT_EPSILON

XCOR_KERNEL_GAL_BIAS_DEFAULT_LEN

XCOR_KERNEL_GAL_DEFAULT_BIAS

XCOR_KERNEL_GAL_DEFAULT_MAG_BIAS

XCOR_KERNEL_GAL_DEFAULT_NOISE_BIAS

XCOR_KERNEL_GAL_DEFAULT_PARAMS_ABSTOL

XCOR_KERNEL_GAL_G_FUNC_LEN

XCOR_KERNEL_WEAK_LENSING_DEFAULT_PARAMS_ABSTOL

XCOR_LENSING_EFFICIENCY_DEFAULT_ABSTOL

XCOR_LENSING_EFFICIENCY_DEFAULT_RELTOL

XCOR_PRECISION