OAI/Analysis/CoulombTransport/Symmetrization.lean
17 declarations, 0 contain sorry, 0 declared as axioms
- def
OAI.Problem356.Cyclic.rotateline 13Source documentation
The cyclic rotation of the three particles.
def rotate : Triple ≃ᵐ Triple where …
Mentions: OAI.Problem356.Triple
- def
OAI.Problem356.Cyclic.symmetrizeline 24Source documentation
Averaging over the cyclic group already gives identical coordinate marginals.
def symmetrize (pi : Measure Triple) : Measure Triple := …
Mentions: OAI.Problem356.Triple
- def
OAI.Problem356.Cyclic.averageMarginalline 28Source documentation
The common marginal of the cyclic average.
def averageMarginal (pi : Measure Triple) : Measure E3 := …
Mentions: OAI.Problem356.Triple, OAI.Problem356.E3
- theorem
OAI.Problem356.Cyclic.measurable_fst₃line 32 - theorem
OAI.Problem356.Cyclic.measurable_snd₃line 33 - theorem
OAI.Problem356.Cyclic.measurable_thd₃line 34 - theorem
OAI.Problem356.Cyclic.map_fst_symmetrizeline 36 - theorem
OAI.Problem356.Cyclic.map_snd_symmetrizeline 44 - theorem
OAI.Problem356.Cyclic.map_thd_symmetrizeline 54 - theorem
OAI.Problem356.Cyclic.symmetrize_probabilityline 64 - theorem
OAI.Problem356.Cyclic.symmetrize_isThreeCouplingline 73 - theorem
OAI.Problem356.Cyclic.ae_symmetrize_of_rotate_invariantline 80Source documentation
A cyclically invariant property holding almost everywhere survives symmetrization. No measurability hypothesis on the property is necessary.
theorem ae_symmetrize_of_rotate_invariant (pi : Measure Triple) {P : Triple → Prop} (hP : ∀ᵐ t ∂pi, P t) (hrotate : ∀ t, P (rotate t) ↔ P t) : ∀ᵐ t ∂symmetrize pi, P t := by …Mentions: OAI.Problem356.Triple, OAI.Problem356.Cyclic.rotate, OAI.Problem356.Cyclic.symmetrize
- theorem
OAI.Problem356.Cyclic.averageMarginal_probabilityline 90 - theorem
OAI.Problem356.Cyclic.invDistance_commline 96 - theorem
OAI.Problem356.Cyclic.cost_rotateline 99 - theorem
OAI.Problem356.Cyclic.cost_rotate_symmline 105 - theorem
OAI.Problem356.Cyclic.lintegral_symmetrizeline 108