The Friedmann-Lemaître-Robertson-Walker metric #
Everything in this file is currently informal or semiformal.
The limit of S (Saddle k) r
as k → ∞
is equal to S (Flat) r
.
Equations
- Cosmology.SpatialGeometry.limit_S_saddle = { deps := [], tag := "6ZZ3D" }
Instances For
The limit of S (Sphere k) r
as k → ∞
is equal to S (Flat) r
.
Equations
- Cosmology.SpatialGeometry.limit_S_sphere = { deps := [], tag := "62A4R" }
Instances For
The hubble constant defined in terms of the scale factor
as (dₜ a) / a
.
The notation H
is used for the hubbleConstant
.
Semiformal implementation note: Implement also scoped notation.
Equations
- Cosmology.FLRW.hubbleConstant = { deps := [], tag := "6Z2NB" }
Instances For
The deceleration parameter defined in terms of the scale factor
as - (dₜdₜ a) a / (dₜ a)^2
.
The notation q
is used for the decelerationParameter
.
Semiformal implementation note: Implement also scoped notation.
Equations
- Cosmology.FLRW.decelerationParameter = { deps := [], tag := "6Z2UE" }
Instances For
The deceleration parameter is equal to - (1 + (dₜ H)/H^2)
.
Equations
- Cosmology.FLRW.decelerationParameter_eq_one_plus_hubbleConstant = { deps := [], tag := "6Z23H" }
Instances For
The time evolution of the hubble parameter is equal to dₜ H = - H^2 (1 + q)
.
Equations
- Cosmology.FLRW.time_evolution_hubbleConstant = { deps := [], tag := "6Z3BS" }
Instances For
There exists a time at which the hubble constant decreases if and only if
there exists a time where the deceleration parameter is less then -1
.
Equations
- Cosmology.FLRW.hubbleConstant_decrease_iff = { deps := [], tag := "6Z3FS" }