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b1
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IndisputableMonolith.Physics.QCDRGE.TwoLoopAlphaS on GitHub at line 50.
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47def b0 (N_f : ℕ) : ℝ := (11 * (N_c : ℝ) - 2 * (N_f : ℝ)) / (12 * Real.pi)
48
49/-- Two-loop beta coefficient in MS-bar (canonical SU(3) form). -/
50def b1 (N_f : ℕ) : ℝ :=
51 (102 - 38 * (N_f : ℝ) / 3) / (8 * Real.pi ^ 2)
52
53/-- For N_f <= 8 the two-loop coefficient is positive. -/
54theorem b1_pos_lowNf (N_f : ℕ) (hNf : N_f ≤ 8) : 0 < b1 N_f := by
55 unfold b1
56 apply div_pos _ (by positivity : (0 : ℝ) < 8 * Real.pi ^ 2)
57 have hNf_real : (N_f : ℝ) ≤ 8 := by exact_mod_cast hNf
58 linarith
59
60/-- At N_f = 5 (canonical between bottom and top thresholds): b1 > 0. -/
61theorem b1_at_Nf5_pos : 0 < b1 5 := b1_pos_lowNf 5 (by norm_num)
62
63/-- One-loop coefficient at N_f = 5 is positive (asymptotic freedom). -/
64theorem b0_at_Nf5_pos : 0 < b0 5 := by
65 unfold b0 N_c
66 apply div_pos _ (by positivity : (0 : ℝ) < 12 * Real.pi)
67 norm_num
68
69/-- The two-loop running closed form. -/
70def alpha_s_two_loop (alpha_0 : ℝ) (N_f : ℕ) (mu_GeV mu_0_GeV : ℝ) : ℝ :=
71 let L := Real.log (mu_GeV ^ 2 / mu_0_GeV ^ 2)
72 let denom := 1 + b0 N_f * alpha_0 * L +
73 (b1 N_f / b0 N_f) * alpha_0 *
74 Real.log (1 + b0 N_f * alpha_0 * L)
75 alpha_0 / denom
76
77/-- The two-loop denominator collapses to the one-loop denominator when the
78 `b1`-induced correction term vanishes. -/
79theorem alpha_s_two_loop_b1_zero_eq_one_loop
80 (alpha_0 : ℝ) (mu_GeV mu_0_GeV : ℝ) :