def
definition
QuarkAbsoluteMassResidual
show as:
view math explainer →
open explainer
Generate a durable explainer page for this declaration.
open lean source
IndisputableMonolith.Masses.QuarkScoreCard on GitHub at line 172.
browse module
All declarations in this module, on Recognition.
explainer page
depends on
-
of -
rung -
Constants -
rung -
of -
A -
of -
of -
gap -
Phase -
of -
A -
Sector -
gap -
rung -
Fermion -
gap -
M0 -
rung -
Sector -
sectorOf -
ZOf -
Sector -
sectorOf -
Fermion -
rs_mass_MeV -
A -
RSBridge -
Phase -
Fermion -
gap -
M0 -
rung -
Sector -
sectorOf -
ZOf -
row
used by
formal source
169 formula and the gap-corrected `massAtAnchor` formula on a chosen
170 quark sector. A proof of this proposition would close the absolute
171 quark-mass row of the scorecard. -/
172def QuarkAbsoluteMassResidual : Prop :=
173 ∀ (f : Fermion),
174 sectorOf f = Sector.up →
175 Verification.rs_mass_MeV Anchor.Sector.UpQuark (RSBridge.rung f)
176 = M0 * Real.exp (((RSBridge.rung f : ℝ) - 8 + gap (ZOf f)) *
177 Real.log Constants.phi)
178
179/-! ## ScoreCard certificate
180
181A single record bundling every theorem-grade row of this Phase 0
182deliverable. -/
183
184structure QuarkScoreCardCert where
185 ZOf_up : ZOf .u = 276 ∧ ZOf .c = 276 ∧ ZOf .t = 276
186 ZOf_down : ZOf .d = 24 ∧ ZOf .s = 24 ∧ ZOf .b = 24
187 ZOf_lep : ZOf .e = 1332 ∧ ZOf .mu = 1332 ∧ ZOf .tau = 1332
188 charm_up_ratio_eq :
189 Verification.charm_quark_pred / Verification.up_quark_pred =
190 Constants.phi ^ (11 : ℕ)
191 top_charm_ratio_eq :
192 Verification.top_quark_pred / Verification.charm_quark_pred =
193 Constants.phi ^ (6 : ℕ)
194 top_in_band : (10000 : ℝ) < Verification.top_quark_pred ∧
195 Verification.top_quark_pred < 1000000
196 quark_preds_pos : 0 < Verification.up_quark_pred ∧
197 0 < Verification.charm_quark_pred ∧ 0 < Verification.top_quark_pred
198 electron_pct :
199 |Verification.rs_mass_MeV .Lepton 2 - Verification.m_e_exp| /
200 Verification.m_e_exp < 0.003
201 muon_pct :
202 |Verification.rs_mass_MeV .Lepton 13 - Verification.m_mu_exp| /