CosmoFit.FQExponential¶
- class CosmoFit.FQExponential(params)[source]¶
Bases:
Cosmologyf(Q) gravity, exponential model.
f(Q) modified gravity replaces the Ricci scalar R in the Einstein-Hilbert action with an arbitrary function f of the non-metricity scalar Q (symmetric teleparallel gravity; GR is recovered exactly at f(Q)=Q). This is a genuine modification of the gravitational field equations, not a dark-energy fluid bolted onto standard GR the way LCDM/wCDM/CPL/JBP/BA/GCG all are.
This implements the specific model of Anagnostopoulos, Basilakos & Saridakis (2021):
f(Q) = Q * exp(lambda * Q0 / Q), Q = 6 H^2, Q0 = 6 H0^2
with lambda the model’s only new quantity. Crucially, lambda is not an independent free parameter: their eq. (10) fixes it from Omega_m via the Lambert W function, so this model has exactly as many free parameters as flat LCDM (H0, Omega_m) – only
Omega_mneeds to be given/fit; lambda is derived automatically. Flat only –Omega_kis ignored, since the Q=6H^2 identity this model is built on is itself a flat-FLRW result (see the reference below for the curved-space case, not implemented here).The Friedmann equation (their eq. 9, radiation dropped – as with every other model in this library) is transcendental, not closed-form:
(E^2 - 2*lambda) * exp(lambda / E^2) = Omega_m * (1+z)^3
E(z)solves this via a fixed number of vectorized Newton iterations (the function is smooth and monotonic in E^2 over the physical range, so this converges to machine precision well before the iteration budget is used).dEdzcomes from implicit differentiation of the same relation – closed-form, no extra root-finding – sobackground.q()/plots.deceleration()work exactly like every other model, not as some numerical-fallback special case.Omega_de(z)is presented, as is standard for this model class, as an effective/geometric dark-energy densityE(z)^2 - Omega_m*(1+z)^3– there is no actual second fluid here, the accelerated expansion comes entirely from the modified gravitational sector.Growth of structure.
mu(a, k)implements the standard sub-horizon, quasi-static result for f(Q) gravity’s effective gravitational coupling, G_eff/G_N = 1/f_Q where f_Q = df/dQ (Barros, Barreiro, Koivisto & Nunes 2020, arXiv:2004.07867, “Testing F(Q) gravity with redshift space distortions” – the same growth-rate observable this feeds into here). For this model, f_Q = exp(lambda/E^2) (1 - lambda/E^2) (derived by differentiating f(Q) above and using Q0/Q = 1/E(z)^2), scale-independent (kis accepted for interface consistency withCosmology.mu()but ignored). lambda=0 gives f_Q=1, i.e. mu=1 exactly – by this model’s own closure condition (see_lamabove), that is the Omega_m -> 1 limit (matter-only, EdS), not Omega_m -> 0.References
Anagnostopoulos, Basilakos & Saridakis (2021), “First evidence that non-metricity f(Q) gravity could challenge LCDM”, Phys. Lett. B 822, 136634, arXiv:2104.15123.
Barros, Barreiro, Koivisto & Nunes (2020), “Testing F(Q) gravity with redshift space distortions”, Phys. Dark Univ. 30, 100616, arXiv:2004.07867.
- Parameters:
params (CosmologyParameters)
- __init__(params)¶
- Parameters:
params (CosmologyParameters)
Methods
E(z)Dimensionless Hubble parameter (solves the transcendental Friedmann equation -- see the class docstring).
H(z)Omega_de(z)Effective/geometric dark-energy density -- see the class docstring for why this isn't a real second fluid here.
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)Derivative of E(z), by implicit differentiation of the Friedmann relation (closed-form given E(z), no extra root-finding).
mu(a[, k])Effective gravitational coupling G_eff/G_N = 1/f_Q -- see the class docstring for the derivation.
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_malphacompute_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