synthetic differential geometry
Introductions
from point-set topology to differentiable manifolds
geometry of physics: coordinate systems, smooth spaces, manifolds, smooth homotopy types, supergeometry
Differentials
Tangency
The magic algebraic facts
Theorems
Axiomatics
(shape modality $\dashv$ flat modality $\dashv$ sharp modality)
$(ʃ \dashv \flat \dashv \sharp )$
dR-shape modality$\dashv$ dR-flat modality
$ʃ_{dR} \dashv \flat_{dR}$
(reduction modality $\dashv$ infinitesimal shape modality $\dashv$ infinitesimal flat modality)
$(\Re \dashv \Im \dashv \&)$
fermionic modality$\dashv$ bosonic modality $\dashv$ rheonomy modality
$(\rightrightarrows \dashv \rightsquigarrow \dashv Rh)$
Models
Models for Smooth Infinitesimal Analysis
smooth algebra ($C^\infty$-ring)
differential equations, variational calculus
Euler-Lagrange equation, de Donder-Weyl formalism?,
Chern-Weil theory, ∞-Chern-Weil theory
Cartan geometry (super, higher)
There are two different meanings of horizontal differential form
Given a bundle $\pi \colon P \to X$ of smooth manifolds,
then a differential form on the total space $P$ is horizontal if it vanishes on vertical vector fields:
in the context of variational calculus:
a differential form on the the total space $J^\infty_X(E)$ of the jet bundle of $E$ is horizontal if it is in the horizontal compoent of the variational bicomplex of $J^\infty(E)$.
Last revised on June 27, 2019 at 12:13:13. See the history of this page for a list of all contributions to it.