openAI-math-dataset / lean /OAI /Probability /ClassicalON /CylindricalFiber.lean
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Add lean source and binary files (part 119)
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import OAI.Probability.ClassicalON.CylindricalGeometry
namespace OAI
noncomputable section
open MeasureTheory
namespace ClassicalON
def firstAmplitude (s : Spin 3) : Amplitude := ⟨|s.val 0|,abs_nonneg _,by
simpa only [Real.norm_eq_abs,spin_norm] using PiLp.norm_apply_le s.val 0⟩
theorem continuous_firstAmplitude : Continuous firstAmplitude := by
apply Continuous.subtype_mk
exact ((PiLp.continuous_apply 2 _ 0).comp continuous_subtype_val).abs
@[simp] theorem firstAmplitude_cylindricalSpin (r : Amplitude) (τ : Bool) (θ : PlanarAngle) :
firstAmplitude (cylindricalSpin r τ θ)=r := by
apply Subtype.ext
change |(r:ℝ)*signValue τ|=(r:ℝ)
cases τ <;> simp [signValue,abs_of_nonneg r.property.1]
theorem planarAngle_exists (a b : ℝ) (hab : a^2+b^2=1) :
∃ θ : PlanarAngle,planarCos θ=a ∧ planarSin θ=b := by
let z : Circle := ⟨⟨a,b⟩,by
change (⟨a,b⟩ : ℂ) ∈ Metric.sphere 0 1
rw [mem_sphere_zero_iff_norm]
apply (sq_eq_sq₀ (norm_nonneg _) (by norm_num : (0:ℝ)≤1)).mp
rw [← Complex.normSq_eq_norm_sq]
simpa [Complex.normSq_apply,pow_two] using hab⟩
obtain ⟨θ,hθ⟩ := (AddCircle.homeomorphCircle (T := (1:ℝ)) (by norm_num)).surjective z
rw [AddCircle.homeomorphCircle_apply] at hθ
exact ⟨θ,congrArg (fun z : Circle => (z:ℂ).re) hθ,congrArg (fun z : Circle => (z:ℂ).im) hθ⟩
theorem cylindricalSpin_surjective_fiber (s : Spin 3) :
∃ τ θ,cylindricalSpin (firstAmplitude s) τ θ=s := by
let r := firstAmplitude s
let q := transverseAmplitude r
have hq : q^2=s.val 1^2+s.val 2^2 := by
have hh := normSq_three s.val
rw [spin_norm] at hh
have hr : (r:ℝ)^2=s.val 0^2 := sq_abs _
dsimp only [q]
rw [transverseAmplitude_sq,hr]
nlinarith
obtain ⟨τ,hτ⟩ : ∃ τ,(r:ℝ)*signValue τ=s.val 0 := by
by_cases hs : 0 ≤ s.val 0
· exact ⟨true,by simp [r,firstAmplitude,signValue,abs_of_nonneg hs]⟩
· exact ⟨false,by simp [r,firstAmplitude,signValue,abs_of_neg (lt_of_not_ge hs)]⟩
by_cases hzero : q=0
· refine ⟨τ,0,Subtype.ext ?_⟩
ext i
have h1 : s.val 1=0 := by nlinarith [sq_nonneg (s.val 2)]
have h2 : s.val 2=0 := by nlinarith [sq_nonneg (s.val 1)]
fin_cases i
· exact hτ
· change q*planarCos 0=s.val 1
rw [hzero,h1,zero_mul]
· change q*planarSin 0=s.val 2
rw [hzero,h2,zero_mul]
· have hab : (s.val 1/q)^2+(s.val 2/q)^2=1 := by
field_simp
nlinarith
obtain ⟨θ,hc,hs⟩ := planarAngle_exists _ _ hab
refine ⟨τ,θ,Subtype.ext ?_⟩
ext i
fin_cases i
· exact hτ
· change q*planarCos θ=s.val 1
rw [hc,mul_div_cancel₀ _ hzero]
· change q*planarSin θ=s.val 2
rw [hs,mul_div_cancel₀ _ hzero]
theorem cylinderRotation_cylindricalSpin (τ υ : Bool) (θ φ : PlanarAngle) (r : Amplitude) :
spinRotation (cylinderRotation τ θ) (cylindricalSpin r υ φ)=
cylindricalSpin r (τ==υ) (θ+φ) := by
apply Subtype.ext
ext i
fin_cases i
· change signValue τ*((r:ℝ)*signValue υ)=(r:ℝ)*signValue (τ==υ)
cases τ <;> cases υ <;> simp [signValue]
· change planarCos θ*(transverseAmplitude r*planarCos φ)-
planarSin θ*(transverseAmplitude r*planarSin φ)=transverseAmplitude r*planarCos (θ+φ)
rw [planarCos_add]; ring
· change planarSin θ*(transverseAmplitude r*planarCos φ)+
planarCos θ*(transverseAmplitude r*planarSin φ)=transverseAmplitude r*planarSin (θ+φ)
rw [planarSin_add]; ring
theorem continuous_cylinderSpinRotation :
Continuous (fun p : (Bool×PlanarAngle)×Spin 3 =>
spinRotation (cylinderRotation p.1.1 p.1.2) p.2) := by
apply Continuous.subtype_mk
change Continuous (fun p : (Bool×PlanarAngle)×Spin 3 => cylinderLinear p.1.1 p.1.2 p.2.val)
unfold cylinderLinear
apply (PiLp.continuous_toLp 2 _).comp
apply continuous_pi
intro i
have hc : Continuous (fun p : (Bool×PlanarAngle)×Spin 3 => planarCos p.1.2) := continuous_planarCos.comp (continuous_snd.comp continuous_fst)
have hs : Continuous (fun p : (Bool×PlanarAngle)×Spin 3 => planarSin p.1.2) := continuous_planarSin.comp (continuous_snd.comp continuous_fst)
have ht : Continuous (fun p : (Bool×PlanarAngle)×Spin 3 => signValue p.1.1) := (show Continuous signValue from continuous_of_discreteTopology).comp (continuous_fst.comp continuous_fst)
have hv (j : Fin 3) : Continuous (fun p : (Bool×PlanarAngle)×Spin 3 => p.2.val j) := (PiLp.continuous_apply 2 _ j).comp (continuous_subtype_val.comp continuous_snd)
fin_cases i
· exact ht.mul (hv 0)
· exact (hc.mul (hv 1)).sub (hs.mul (hv 2))
· exact (hs.mul (hv 1)).add (hc.mul (hv 2))
end ClassicalON
end
end OAI