PhysLean Documentation

PhysLean.Cosmology.FLRW.Basic

The Friedmann-Lemaître-Robertson-Walker metric #

Parts of this file is currently informal or semiformal.

The inductive type with three constructors:

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    noncomputable def Cosmology.SpatialGeometry.S (s : SpatialGeometry) :

    For s corresponding to

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      theorem Cosmology.SpatialGeometry.mul_sinh_as_div (r k : ) :
      k * Real.sinh (r / k) = Real.sinh (r / k) / (1 / k)

      The limit of S (Saddle k) r as k → ∞ is equal to S (Flat) r. First show that k * sinh(r / k) = sinh(r / k) / (1 / k) pointwise.

      First, show that limit of sinh(r * x) / x is r at the limit x goes to zero. Then the next theorem will address the rewrite using Filter.Tendsto.comp

      The limit of S (Sphere k) r as k → ∞ is equal to S (Flat) r.

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        The structure FLRW is defined to contain the physical parameters of the Friedmann-Lemaître-Robertson-Walker metric. That is, it contains

        Semiformal implementation note: It is possible that we should restrict a(t) to be smooth or at least twice differentiable.

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          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.

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            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.

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              The deceleration parameter is equal to - (1 + (dₜ H)/H^2).

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                The time evolution of the hubble parameter is equal to dₜ H = - H^2 (1 + q).

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                  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.

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