The Friedmann-Lemaître-Robertson-Walker metric #
Everything in this file is currently informal or semiformal.
The inductive type with three constructors:
Spherical (k : ℝ)
Flat
Saddle (k : ℝ)
Equations
- Cosmology.SpatialGeometry = sorry
Instances For
For s
corresponding to
Semiformal implementation note: There is likely a better name for this function.
Instances For
The structure FLRW is defined to contain the physical parameters of the Friedmann-Lemaître-Robertson-Walker metric. That is, it contains
- The scale factor
a(t)
- An element of
SpatialGeometry
.
Semiformal implementation note: It is possible that we should restirct
a(t)
to be smooth or at least twice differentiable.
Equations
- Cosmology.FLRW = sorry
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.
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.
Instances For
The deceleration parameter is equal to - (1 + (dₜ H)/H^2)
.
Equations
Instances For
The time evolution of the hubble parameter is equal to dₜ H = - H^2 (1 + q)
.
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
.