The main coordinate norm is controlled by fast and stored slow coordinates
ProvedErdos390.Full.PaperBridgeFit.BridgeData.main_norm_sq_le_fastSharp_add_storedSlowanalytic-number-theoryerdos-390erdos390-source-construction
Let be bridge data, a main-space vector, raw band-gauge vectors, and . Let be the paper sharp norm, the stored slow scale, and the source's sum of squared gauge centers. Assume , , the raw gauge of is , and . Then
This finite coordinate comparison converts fast/slow variance control into main-space coercivity.
Preamble
import Mathlib import Definitions.Def_erdos390_source_bank_interface import Definitions.Def_erdos390_dickman_step_function import Theorems.Thm_MediumPNT import Definitions.Def_erdos390_analytic_foundations_001 import Theorems.Thm_Erdos390_Full_DickmanBasic_kernel_product_bound import Theorems.Thm_Erdos390_Full_DickmanBasic_rho_pos_on_zero_five import Theorems.Thm_Erdos390_Full_DickmanBasic_kernel_secondDerivative_first_bound import Definitions.Def_erdos390_analytic_foundations_002 import Definitions.Def_erdos390_analytic_foundations_004 import Definitions.Def_erdos390_analytic_foundations_005 universe u_1 u_2
Formal statement
theorem Erdos390.Full.PaperBridgeFit.BridgeData.main_norm_sq_le_fastSharp_add_storedSlow :
∀ {Head : Type u_1} {Band : Type u_2} [inst : Fintype.{u_1} Head] [inst_1 : DecidableEq.{u_1 + 1} Head]
[inst_2 : Fintype.{u_2} Band] [inst_3 : DecidableEq.{u_2 + 1} Band]
(B : Erdos390.Full.PaperBridgeFit.BridgeData.{u_1, u_2} Head Band)
(u : Erdos390.Full.PaperBridgeFit.BridgeData.MainSpace.{u_1, u_2} B)
(qFast qReg : ↥(Erdos390.Full.PaperBridgeFit.BridgeData.RawBandGauge.{u_1, u_2} B)) (lambda Creg : Real),
LE.le.{0} (0 : Real) Creg →
LE.le.{0}
(Erdos390.Full.PaperWeightedInverseExport.paperSharpNorm.{u_2}
(Erdos390.Full.PaperBridgeFit.BridgeData.harmonicMass.{u_1, u_2} B)
(Erdos390.Full.PaperBridgeFit.BridgeData.bandCenter.{u_1, u_2} B)
(Erdos390.Full.ArithmeticBandGeometry.Partition.center_ne_zero.{u_2}
(Erdos390.Full.PaperBridgeFit.BridgeData.partition.{u_1, u_2} B)
(Erdos390.Full.PaperBridgeFit.BridgeData.n_gt_one.{u_1, u_2} B))
qReg)
(HMul.hMul.{0, 0, 0} Creg (Erdos390.Full.PaperBridgeFit.BridgeData.w.{u_1, u_2} B)) →
Eq.{u_2 + 1} (Erdos390.Full.PaperBridgeFit.BridgeData.rawGaugeOfMain.{u_1, u_2} B u)
(HSub.hSub.{u_2, u_2, u_2} qFast (HSMul.hSMul.{0, u_2, u_2} lambda qReg)) →
Eq.{1} (WithLp.ofLp.{u_2} u Erdos390.Full.PaperBridgeFit.MainCoord.slow.{u_2})
(HMul.hMul.{0, 0, 0} (Erdos390.Full.PaperBridgeFit.BridgeData.w.{u_1, u_2} B) lambda) →
LE.le.{0} (HPow.hPow.{0, 0, 0} (Norm.norm.{u_2} u) (2 : Nat))
(HMul.hMul.{0, 0, 0}
(HAdd.hAdd.{0, 0, 0} (1 : Real)
(HMul.hMul.{0, 0, 0}
(HMul.hMul.{0, 0, 0} (2 : Real)
(Erdos390.Full.PaperBridgeFit.BridgeData.gaugeCenterSquareSum.{u_1, u_2} B))
(HAdd.hAdd.{0, 0, 0} (1 : Real) (HPow.hPow.{0, 0, 0} Creg (2 : Nat)))))
(HAdd.hAdd.{0, 0, 0}
(HPow.hPow.{0, 0, 0}
(Erdos390.Full.PaperWeightedInverseExport.paperSharpNorm.{u_2}
(Erdos390.Full.PaperBridgeFit.BridgeData.harmonicMass.{u_1, u_2} B)
(Erdos390.Full.PaperBridgeFit.BridgeData.bandCenter.{u_1, u_2} B)
(Erdos390.Full.ArithmeticBandGeometry.Partition.center_ne_zero.{u_2}
(Erdos390.Full.PaperBridgeFit.BridgeData.partition.{u_1, u_2} B)
(Erdos390.Full.PaperBridgeFit.BridgeData.n_gt_one.{u_1, u_2} B))
qFast)
(2 : Nat))
(HPow.hPow.{0, 0, 0}
(HMul.hMul.{0, 0, 0} (Erdos390.Full.PaperBridgeFit.BridgeData.w.{u_1, u_2} B) lambda) (2 : Nat)))) := by sorry
Source