CosmoFit.ADE¶
- class CosmoFit.ADE(params)[source]¶
Bases:
CosmologyNew agegraphic dark energy: the holographic cutoff is the age of the universe, in conformal time.
The holographic family differs only in what length scale is put in
rho_DE = 3 c^2 M_p^2 / L^2.HDEuses the future event horizon,RDEthe Ricci scalar, and this uses the conformal age,rho_DE = 3 n^2 M_p^2 / eta^2, eta = Int dt / a = Int da / (a^2 H),
which is causal, local in time, and needs no reference to the future – the objection HDE attracts.
Like HDE there is no closed form. Writing
Omega_DE = n^2 / (eta H)^2and differentiating the definition ofetagives- d Omega_DE / d ln a
- = Omega_DE (1 - Omega_DE)
[3 - (2/n) sqrt(Omega_DE) / a],
solved and splined on every
refresh(), with the expansion rate following from flatness asE^2 = Omega_m (1+z)^3 / (1 - Omega_DE).The early-time behaviour is the model’s signature and its own consistency check: for
Omega_DE << 1the equation forcesOmega_DE -> n^2 a^2 / 4exactly, so dark energy dilutes asa^2rather than theaof HDE, and the equation of state isw = -1 + (2 / 3n) sqrt(Omega_DE) / a,
which tends to
-2/3at early times and to-1in the far future for everyn. So unlike HDE, this model cannot be phantom at anyn: the crossing HDE predicts is simply not available here, which is the sharpest observational difference between them.Caveats¶
Flat universes only, and refused by
CAMBBackend, for the same reasons asHDE.References
Wei & Cai (2008), Phys. Lett. B 660, 113, arXiv:0708.0884.
- __init__(params)¶
- Parameters:
params (CosmologyParameters)
Methods
E(z)H(z)Omega_de(z)Dark-energy density in units of today's critical density -- the term inside
E(z)^2, as every other model here returns.Omega_matter(z)Matter density at redshift
z, in units of today's critical density -- i.e. theOmega_m (1+z)^3term as it appears insideE(z)^2, before dividing byE(z)^2.__init__(params)dEdz(z)Analytic, from the ODE rather than by differencing
E.mu(a[, k])Effective-to-Newtonian gravitational coupling ratio, G_eff(a,k)/G_N, entering the linear growth equation solved by
GrowthCalculator(see that module's docstring for the equation itself).omega_de_fraction(z)The density parameter
rho_DE(z) / rho_crit(z), which is what the ODE solves for -- notOmega_de(), which is in units of today's critical density.plain_name()This model's name as plain text:
MODEL_NAMEif it declares one, else the class name.plot_label()This model's name as it should appear in a figure legend or title --
MODEL_LABEL(LaTeX) if it declares one, elseplain_name().refresh()Rebuild internal numerical tables after the underlying
paramsobject has been mutated in place (e.g. byparams.update(theta)during an MCMC step).w_de(z)w = -1 + (2 / 3n) sqrt(Omega_DE) / a.Attributes
A_planckA_sDERIVED_PARAMSParameters this model derives rather than accepts.
EXTRA_PARAMSExtra parameters this model adds beyond CosmologyParameters.
H0MBMODEL_LABELa LaTeX math string where the plain name is really a set of symbols (
LCDM->$\Lambda$CDM), None where the plain name is already what a reader should see (an acronym likeCPL).MODEL_NAMEPlain-text name for this model, for tables, JSON and log lines.
N_effOmega_bOmega_de0Omega_kOmega_mMatter density, derived from
n_aderather than sampled.alphacompute_rdWhether
rdis computed from the physical densities (rd_computed()) rather than read from the freerdparameter.derive_sigma8Whether
sigma8is derived from the Boltzmann code rather than read from the freesigma8parameter.hReduced Hubble constant,
H0 / 100.ln1e10Asm_nun_aden_somega_b_h2Physical baryon density,
Omega_b h^2-- the combination BBN and the CMB actually constrain.omega_cdm_h2Physical cold dark matter density,
Omega_c h^2-- matter less baryons.omega_m_h2Physical matter density,
Omega_m h^2.rdThe sound horizon at the drag epoch [Mpc] that the BAO likelihoods divide by.
sigma8Present-day
sigma_8, the normalization every growth prediction is built on.tau_reiow0wa- Parameters:
params (CosmologyParameters)