PhysLean Documentation

PhysLean.Cosmology.FLRW.Basic

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)
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    For s corresponding to

    • Spherical k, S s r = k * sin (r / k)
    • Flat, S s r = r,
    • Saddle k, S s r = k * sin (r / k).

    Semiformal implementation note: There is likely a better name for this function.

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    • s.S = sorry
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      The limit of S (Saddle k) r as k → ∞ is equal to S (Flat) r.

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        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 restirct 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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