OAI/Analysis/CoulombIonization/Variational/TensorLp.lean
25 declarations, 0 contain sorry, 0 declared as axioms
- lemma
OAI.CoulombAtom.memLp_tensor_of_aemeasurableline 111 - lemma
OAI.CoulombAtom.memLp_tensor_of_sfinite_rightline 166 - lemma
OAI.CoulombAtom.not_aemeasurable_count_restrict_prodMkline 171 - lemma
OAI.CoulombAtom.not_memLp_tensor_count_restrict_of_choiceline 204 - lemma
OAI.CoulombAtom.volume_prod_eq_choice_of_not_aemeasurableline 233 - lemma
OAI.CoulombAtom.memLp_tensor_iff_choiceline 247 - lemma
OAI.CoulombAtom.memLp_tensorline 271Source documentation
Right s-finiteness makes the product kernel measurable, so L² factors have an L² tensor. Without an a.e. measurable kernel, Mathlib's product uses an arbitrary chosen measure, whose integrability is characterized by
memLp_tensor_iff_choice, not guaranteed by the factors. The finite-dimensional Haar hypotheses in the applications imply right s-finiteness.lemma memLp_tensor {f : E → ℂ} {g : F → ℂ} (hf : MemLp f 2) (hg : MemLp g 2) : MemLp (fun point : E × F => f point.1 * g point.2) 2 := … - lemma
OAI.CoulombAtom.integral_tensor_sqline 275 - lemma
OAI.CoulombAtom.lineDeriv_slice_leftline 294 - lemma
OAI.CoulombAtom.IsWeakDerivative.tensor_leftline 305 - lemma
OAI.CoulombAtom.IsWeakDerivative.tensor_rightline 330 - def
OAI.CoulombAtom.leftListline 349 - def
OAI.CoulombAtom.rightListline 351 - lemma
OAI.CoulombAtom.leftList_joinline 354 - lemma
OAI.CoulombAtom.rightList_joinline 356 - lemma
OAI.CoulombAtom.join_list_partsline 358 - lemma
OAI.CoulombAtom.configurationJoin_symm_applyline 366 - lemma
OAI.CoulombAtom.configurationJoin_symm_preservingline 371 - lemma
OAI.CoulombAtom.configurationJoin_direction_rightline 376 - def
OAI.CoulombAtom.tensorFormline 389 - lemma
OAI.CoulombAtom.tensorForm_value_joinline 396 - lemma
OAI.CoulombAtom.tensorForm_gradient_leftline 401 - lemma
OAI.CoulombAtom.tensorForm_gradient_rightline 408 - lemma
OAI.CoulombAtom.SobolevVector.tensorline 415 - lemma
OAI.CoulombAtom.formMass_tensorline 452