Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Connection (mathematics)
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
==Possible approaches== *A rather direct approach is to specify how a [[covariant derivative]] acts on elements of the [[module (mathematics)|module]] of [[vector field]]s as a [[differential operator]]. More generally, a similar approach applies for [[connection (vector bundle)|connections]] in any [[vector bundle]]. *Traditional index notation specifies the connection by components; see [[Christoffel symbols]]. (''Note'': this has three indices, but is '''''not''''' a [[tensor]]). *In [[pseudo-Riemannian]] and [[Riemannian geometry]] the [[Levi-Civita connection]] is a special connection associated to the [[metric tensor]]. *These are examples of [[affine connection]]s. There is also a concept of [[projective connection]], of which the [[Schwarzian derivative]] in [[complex analysis]] is an instance. More generally, both affine and projective connections are types of [[Cartan connection]]s. *Using [[principal bundle]]s, a connection can be realized as a [[Lie algebra]]-valued [[differential form]]. See [[connection (principal bundle)]]. *An approach to connections which makes direct use of the notion of transport of "data" (whatever that may be) is the [[Ehresmann connection]]. *The most abstract approach may be that suggested by [[Alexander Grothendieck]], where a [[Grothendieck connection]] is seen as [[descent (category theory)|descent]] data from infinitesimal neighbourhoods of the [[diagonal]]; see {{harv|Osserman|2004}}.
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)