CosmoFit.DGP¶
- class CosmoFit.DGP(params)[source]¶
Bases:
CosmologyDvali-Gabadadze-Porrati braneworld gravity, self-accelerating branch.
E(z) = sqrt(Omega_rc + Omega_m (1+z)^3) + sqrt(Omega_rc) E(z)^2 -> that, plus Omega_k (1+z)^2 for a curved brane
Gravity leaks into a fifth dimension above a crossover scale
r_c, weakening it at large distances. The universe then accelerates with no dark energy at all – there is noOmega_determ in the Friedmann equation above, and none in the theory. That is what distinguishes DGP from every dark-energy parametrization in this library: those add a fluid, this changes gravity.Omega_rc = 1/(4 r_c^2 H0^2)is not free. The Friedmann constraintE(0) = 1fixes it:Omega_rc = (1 - Omega_k - Omega_m)^2 / (4 (1 - Omega_k))
so DGP, like
PEDE, has exactly LCDM’s parameter count and a completely different expansion history – a fair comparison with no free parameter absorbing the difference.Growth of structure¶
This model overrides
mu(a, k)with the standard sub-horizon DGP result (Lue, Scoccimarro & Starkman 2004; Koyama & Maartens 2006):mu = 1 + 1 / (3 beta), beta(a) = 1 - 2 H r_c [1 + Hdot / (3 H^2)]
On the self-accelerating branch
beta < 0, somu < 1– gravity is weaker than in GR and structure grows more slowly. Today, forOmega_m = 0.3,mu ~ 0.72. This is the model’s real observational signature and the reason it is strongly disfavoured by growth data even where it can be tuned to fit distances: no dark-energy parametrization can suppress growth this way while keeping the same background.Hdot / H^2 = -(1+z) E'(z) / E(z), built from this model’s ownE/dEdzrather than from an LCDM approximation.Caveats¶
The self-accelerating branch is known to carry a ghost instability in its scalar sector. It is implemented here as the historically and observationally important benchmark it is – the reference case against which “modified gravity can mimic dark energy” is tested – not as a viable theory. Its perturbations are also outside what a standard Boltzmann code solves, so it is refused by
CAMBBackend; use the compressed distance priors for its CMB constraint.References
Dvali, Gabadadze & Porrati (2000), Phys. Lett. B 485, 208, arXiv:hep-th/0005016.
Deffayet (2001), Phys. Lett. B 502, 199, arXiv:hep-th/0010186 (the cosmological solution).
Koyama & Maartens (2006), JCAP 01 (2006) 016, arXiv:astro-ph/0511634 (the growth of structure).
- __init__(params)¶
- Parameters:
params (CosmologyParameters)
Methods
E(z)H(z)Omega_de(z)The effective dark-energy density this model's expansion history would be attributed to, if one insisted on writing it as GR plus a fluid:
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)mu(a[, k])Effective gravitational coupling
G_eff/G_Non the self-accelerating branch,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).Attributes
A_planckA_sEXTRA_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_mOmega_rcThe crossover-scale density parameter,
Omega_rc = 1/(4 r_c^2 H0^2), fixed byE(0) = 1.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_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)