“ R i 3 m a n G d k o d t m ∇ 2 {\displaystyle Ri3man\;G{\frac {d^{k}o}{dt^{m}}}\nabla ^{2}} ”~ ∀ ω − c o n s i ς e n t θ e o r y T ⊇ Q , ∃ ϕ ∈ L a r s . t . ⊬ T ϕ ∧ ⊬ T ϕ̸ , i . e . , T {\displaystyle \forall \omega -consi\varsigma ent\;\theta eory\;T\supseteq Q,\exists \phi \in {\mathcal {L}}_{ar}\;s.t.\;\not \vdash _{T}\phi \land \not \vdash _{T}\not \phi ,i.e.,T}
“ R i 3 m a n G d k o d t m ∇ 2 {\displaystyle Ri3man\;G{\frac {d^{k}o}{dt^{m}}}\nabla ^{2}} ”