Relativistic Heavy Ion Collider: Difference between revisions

From formulasearchengine
Jump to navigation Jump to search
 
en>Dewritech
→‎The experiments: clean up, typo(s) fixed: so called → so-called using AWB
Line 1: Line 1:
Alyson is what my husband enjoys to call me but I don't like when people use my complete name. Office supervising is where her main income comes from. I've always loved residing in Kentucky but now I'm considering other options. To perform lacross is the factor I adore most of all.<br><br>Feel free to visit my homepage :: [http://www.edusharer.com/members/profile/311291/CeWebster psychic readings]
In [[mathematics]], the '''exterior covariant derivative''', sometimes also '''covariant exterior derivative''', is a very useful notion for [[calculus on manifolds]], which makes it possible to simplify formulas which use a [[Connection (principal bundle)|principal connection]].
 
==Definition==
Let ''P'' &rarr; ''M'' be a [[principal bundle|principal ''G''-bundle]] on a [[smooth manifold]] ''M''. If ϕ is a [[tensorial form|tensorial ''k''-form]] on ''P'', then its exterior covariant derivative is defined by
:<math>D\phi(X_0,X_1,\dots,X_k)=\mathrm{d}\phi(h(X_0),h(X_1),\dots,h(X_k))</math>
where ''h'' denotes the projection to the [[Horizontal space|horizontal subspace]], ''H<sub>x</sub>'' defined by the connection, with kernel ''V<sub>x</sub>'' (the [[vertical subspace]]) of the tangent bundle of the [[total space]] of the [[fiber bundle]]. Here ''X<sub>i</sub>'' are any vector fields on ''P''. ''D''ϕ is a tensorial (''k'' + 1)-form on ''P''.
 
==Properties==
Unlike the usual [[exterior derivative]], which squares to 0 (that is d<sup>2</sup> = 0), we have
 
:<math>D^2\phi=\Omega\wedge\phi</math>
 
where Ω denotes the [[curvature form]]. In particular ''D''<sup>2</sup> vanishes for a [[flat connection]].
 
==See also==
*[[Connection_form#Exterior_connections|Exterior connections]]
 
==References==
*{{cite book | author=Kobayashi, Shoshichi and Nomizu, Katsumi | title = [[Foundations of Differential Geometry]], Vol. 1 | publisher=Wiley-Interscience | year=1996 (New edition) |isbn = 0-471-15733-3}}
 
{{tensor}}
 
[[Category:Connection (mathematics)]]
[[Category:Differential geometry]]
[[Category:Fiber bundles]]
 
{{differential-geometry-stub}}

Revision as of 16:16, 29 November 2013

In mathematics, the exterior covariant derivative, sometimes also covariant exterior derivative, is a very useful notion for calculus on manifolds, which makes it possible to simplify formulas which use a principal connection.

Definition

Let PM be a principal G-bundle on a smooth manifold M. If ϕ is a tensorial k-form on P, then its exterior covariant derivative is defined by

where h denotes the projection to the horizontal subspace, Hx defined by the connection, with kernel Vx (the vertical subspace) of the tangent bundle of the total space of the fiber bundle. Here Xi are any vector fields on P. Dϕ is a tensorial (k + 1)-form on P.

Properties

Unlike the usual exterior derivative, which squares to 0 (that is d2 = 0), we have

where Ω denotes the curvature form. In particular D2 vanishes for a flat connection.

See also

References

  • 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

    My blog: http://www.primaboinca.com/view_profile.php?userid=5889534

Template:Tensor

Template:Differential-geometry-stub