pyccl.background module
Smooth background quantities
CCL defines seven species types:
‘matter’: cold dark matter and baryons
‘dark_energy’: cosmological constant or otherwise
‘radiation’: relativistic species besides massless neutrinos (i.e., only photons)
‘curvature’: curvature density
‘neutrinos_rel’: relativistic neutrinos
‘neutrinos_massive’: massive neutrinos
These strings define the species inputs to the functions below.
- class pyccl.background.Species(value, names=None, *, module=None, qualname=None, type=None, start=1, boundary=None)[source]
Bases:
Enum
- CRITICAL = 'critical'
- MATTER = 'matter'
- DARK_ENERGY = 'dark_energy'
- RADIATION = 'radiation'
- CURVATURE = 'curvature'
- NEUTRINOS_REL = 'neutrinos_rel'
- NEUTRINOS_MASSIVE = 'neutrinos_massive'
- pyccl.background.h_over_h0(cosmo, a)[source]
Ratio of Hubble constant at a over Hubble constant today.
- pyccl.background.scale_factor_of_chi(cosmo, chi)[source]
Scale factor, a, at a comoving radial distance chi.
- pyccl.background.comoving_angular_distance(cosmo, a)[source]
Comoving angular distance.
Note
This quantity is otherwise known as the transverse comoving distance, and is NOT angular diameter distance or angular separation. The comoving angular distance is defined such that the comoving distance between two objects at a fixed scale factor separated by an angle \(\theta\) is \(\theta r_{A}(a)\) where \(r_{A}(a)\) is the comoving angular distance.
- pyccl.background.angular_diameter_distance(cosmo, a1, a2=None)[source]
Angular diameter distance.
The angular diameter distance in Mpc from scale factor a1 to scale factor a2. If a2 is not provided, it is assumed that the distance will be calculated between 1 and a1.
Note
a2 has to be smaller than a1 (i.e. a source at a2 is behind one at a1). You can compute the distance between a single lens at a1 and multiple sources at a2 by passing a scalar a1.
- pyccl.background.distance_modulus(cosmo, a)[source]
Distance Modulus, defined as
\[\mu = 5\,\log_{10}(d_L/10\,{\rm pc})\]where \(d_L\) is the luminosity distance.
Note
The distance modulus can be used to convert between apparent and absolute magnitudes via \(m = M + \mu\), where \(m\) is the apparent magnitude and \(M\) is the absolute magnitude.
- pyccl.background.hubble_distance(cosmo, a)[source]
Hubble distance in \(\rm Mpc\).
\[D_{\rm H} = \frac{cz}{H_0}\]- Parameters:
cosmo (
Cosmology
) – Cosmological parameters.a (float or (na,) array_like) – Scale factor(s) normalized to 1 today.
- Returns:
D_H – Hubble distance.
- Return type:
float or (na,)
numpy.ndarray
- pyccl.background.comoving_volume_element(cosmo, a)[source]
Comoving volume element in \(\rm Mpc^3 \, sr^{-1}\).
\[\frac{\mathrm{d}V}{\mathrm{d}a \, \mathrm{d} \Omega}\]- Parameters:
cosmo (
Cosmology
) – Cosmological parameters.a (float or (na,) array_like) – Scale factor(s) normalized to 1 today.
- Returns:
dV – Comoving volume per unit scale factor per unit solid angle.
- Return type:
float or (na,)
numpy.ndarray
See also
comoving_volume
integral of the comoving volume element
- pyccl.background.comoving_volume(cosmo, a, *, solid_angle=12.566370614359172)[source]
Comoving volume, in \(\rm Mpc^3\).
\[V_{\rm C} = \int_{\Omega} \mathrm{{d}}\Omega \int_z \mathrm{d}z D_{\rm H} \frac{(1+z)^2 D_{\mathrm{A}}^2}{E(z)}\]See Eq. 29 in Hogg 2000.
- Parameters:
- Returns:
V_C – Comoving volume at
a
.- Return type:
float or (na,) ndarray
See also
comoving_volume_element
comoving volume element
- pyccl.background.lookback_time(cosmo, a)[source]
Difference of the age of the Universe between some scale factor and today, in \(\rm Gyr\).
- pyccl.background.age_of_universe(cosmo, a)[source]
Age of the Universe at some scale factor, in \(\rm Gyr\).
- pyccl.background.sigma_critical(cosmo, *, a_lens, a_source)[source]
Returns the critical surface mass density.
\[\Sigma_{\mathrm{crit}} = \frac{c^2}{4\pi G} \frac{D_{\rm{s}}}{D_{\rm{l}}D_{\rm{ls}}},\]where \(c\) is the speed of light, \(G\) is the gravitational constant, and \(D_i\) is the angular diameter distance. The labels \(i = \{s,\,l,\,ls\}\) denote the distances to the source, lens, and between source and lens, respectively.
- pyccl.background.omega_x(cosmo, a, species)[source]
Density fraction of a given species at a redshift different than z=0.
- Parameters:
cosmo (
Cosmology
) – Cosmological parameters.a (
float
or array) – Scale factor(s), normalized to 1 today.species (
str
) –species type. Should be one of
’matter’: cold dark matter, massive neutrinos, and baryons
’dark_energy’: cosmological constant or otherwise
’radiation’: relativistic species besides massless neutrinos
’curvature’: curvature density
’neutrinos_rel’: relativistic neutrinos
’neutrinos_massive’: massive neutrinos
’critical’
- Returns:
Density fraction of a given species at a scale factor.
- Return type:
(
float
or array)
- pyccl.background.rho_x(cosmo, a, species, *, is_comoving=False)[source]
Physical or comoving density as a function of scale factor.
- Parameters:
cosmo (
Cosmology
) – Cosmological parameters.a (
float
or array) – Scale factor(s), normalized to 1 today.species (
str
) –species type. Should be one of
’matter’: cold dark matter, massive neutrinos, and baryons
’dark_energy’: cosmological constant or otherwise
’radiation’: relativistic species besides massless neutrinos
’curvature’: curvature density
’neutrinos_rel’: relativistic neutrinos
’neutrinos_massive’: massive neutrinos
’critical’
is_comoving (
bool
) – either physical (False, default) or comoving (True)
- Returns:
Physical density of a given species at a scale factor, in units of \(M_\odot / {\rm Mpc}^3\).
- Return type:
(
float
or array)
- pyccl.background.growth_factor(cosmo, a)[source]
Growth factor.
Warning
CCL is not able to compute the scale-dependent growth factor for cosmologies with massive neutrinos.
- pyccl.background.growth_factor_unnorm(cosmo, a)[source]
Unnormalized growth factor.
Warning
CCL is not able to compute the scale-dependent growth factor for cosmologies with massive neutrinos.