theorem
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jcost_symmetric
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IndisputableMonolith.Information.PhysicsComplexityStructure on GitHub at line 76.
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73/-- **THEOREM IC-005.5**: J-cost is symmetric: J(x) = J(1/x).
74 This means the RS cost landscape has a reflection symmetry,
75 ensuring the optimization problem is well-conditioned. -/
76theorem jcost_symmetric (x : ℝ) (hx : x > 0) :
77 Jcost x = Jcost x⁻¹ :=
78 Cost.Jcost_symm hx
79
80/-! ## II. Gradient of J-Cost (Computability of First-Order Optimization) -/
81
82/-- The derivative of J-cost: J'(x) = (1 - 1/x²)/2 = (x² - 1)/(2x²). -/
83noncomputable def jcost_deriv (x : ℝ) : ℝ := (1 - (x⁻¹)^2) / 2
84
85/-- **THEOREM IC-005.6**: J'(1) = 0 — the gradient vanishes at the ground state.
86 This confirms x = 1 is the unique critical point (and global minimum). -/
87theorem jcost_deriv_zero_at_one : jcost_deriv 1 = 0 := by
88 unfold jcost_deriv; simp
89
90/-- **THEOREM IC-005.7**: J'(x) > 0 for x > 1.
91 The gradient points upward away from the minimum for x > 1. -/
92theorem jcost_deriv_pos_of_gt_one (x : ℝ) (hx : x > 1) :
93 jcost_deriv x > 0 := by
94 unfold jcost_deriv
95 apply div_pos _ (by norm_num)
96 have hxpos : (0 : ℝ) < x := by linarith
97 have hxinv_lt1 : x⁻¹ < 1 := by
98 rw [inv_eq_one_div, div_lt_one (by linarith : (0:ℝ) < x)]; linarith
99 have hxinv_pos : (0 : ℝ) < x⁻¹ := inv_pos.mpr hxpos
100 have : 1 - (x⁻¹)^2 > 0 := by
101 have h4 : (1 - x⁻¹) * (1 + x⁻¹) = 1 - (x⁻¹)^2 := by ring
102 rw [← h4]
103 exact mul_pos (by linarith) (by linarith)
104 linarith
105
106/-- **THEOREM IC-005.8**: J'(x) < 0 for 0 < x < 1.