Linear connection: Difference between revisions

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===Definition part (pointwise form)===
===Definition part (pointwise form)===


A '''linear connection''' is a smooth choice <math>\nabla</math> of the following: at each point <math>p \in M</math>, there is a map <math>{}^p\nabla: T_p(M) \times \Gamma(TM) \to T_p(M)</math>, satisfying some conditions. The map is written as <math>{}^p\nabla_X(v)</math> where <math>X \in T_p(M)</math> and <math>v \in \Gamma(E)</math>.
A '''linear connection''' is a smooth choice <math>\nabla</math> of the following: at each point <math>p \in M</math>, there is a map <math>{}^p\nabla: T_p(M) \times \Gamma(TM) \to T_p(M)</math>, satisfying some conditions. The map is written as <math>{}^p\nabla_X(v)</math> where <math>X \in T_p(M)</math> and <math>v \in \Gamma(TM)</math>.


* It is <math>C^\infty</math>-linear in <math>X</math> (that is, in the <math>T_p(M)</math> coordinate).
* It is <math>\R</math>-linear in <math>X</math> (that is, in the <math>T_p(M)</math> coordinate).
* It is <math>\mathbb{R}</math>-linear in <math>\Gamma(TM)</math> (viz the space of sections on <math>E</math>).
* It is <math>\R</math>-linear in <math>\Gamma(TM)</math> (viz the space of sections on <math>TM</math>).
* It satisfies the following relation called the Leibniz rule:
* It satisfies the following relation called the Leibniz rule:


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===Definition part (global form)===
===Definition part (global form)===


A '''connection''' is a map <math>\nabla:\Gamma(TM) \times \Gamma(TM) \to \Gamma(TM)</math>, satisfying the following:
A '''linear connection''' is a map <math>\nabla:\Gamma(TM) \times \Gamma(TM) \to \Gamma(TM)</math>, satisfying the following:


* It is <math>C^\infty</math>-linear in the first <math>\Gamma(TM)</math>
* It is <math>C^\infty</math>-linear in the first <math>\Gamma(TM)</math>
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* It satisfies the following relation called the Leibniz rule:
* It satisfies the following relation called the Leibniz rule:


<math>\nabla_X(fv) = (Xf) (v) f \nabla_X(v) </math>
<math>\nabla_X(fv) = (Xf) (v) + f \nabla_X(v) </math>


where <math>f</math> is a scalar function on the manifold and <math>fv</math> denotes scalar multiplication of <math>v</math> by <math>f</math>.
where <math>f</math> is a scalar function on the manifold and <math>fv</math> denotes scalar multiplication of <math>v</math> by <math>f</math>.
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===Generalizations===
===Generalizations===


The notion of linear connection can be generalized to the more general notion of a [[connection]].
The notion of linear connection can be generalized to the more general notion of a [[connection]], where the second <math>TM</math> is replaced by an arbitrary [[vector bundle]] <math>E</math> over <math>M</math>.


==Operations on a linear connection==
==Operations on a linear connection==
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===Torsion of a linear connection===
===Torsion of a linear connection===


The torsion of a linear connection <math>\nabla</math> is denoted as <math>\tau(\nabla)</math>. It is a <math.(1,2)</math>-tensor defined as:
{{further|[[torsion of a linear connection]]}}
 
The torsion of a linear connection <math>\nabla</math> is denoted as <math>\tau(\nabla)</math>. It is a <math>(1,2)</math>-tensor defined as:


<math>\tau(\nabla)(X,Y)= \nabla_XY - \nabla_YX - [X,Y]</math>.
<math>\tau(\nabla)(X,Y)= \nabla_XY - \nabla_YX - [X,Y]</math>.


A connection whose torsion is zero is termed a [[torsion-free linear connection]].
A connection whose torsion is zero is termed a [[torsion-free linear connection]].
Note that torsion makes sense ''only'' for linear connections.


===Curvature of a linear connection===
===Curvature of a linear connection===
{{further|[[Riemann curvature tensor]]}}


The curvature of a linear connection <math>\nabla</math> is denoted as <math>R_\nabla</math>. It is defined as:
The curvature of a linear connection <math>\nabla</math> is denoted as <math>R_\nabla</math>. It is defined as:
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<math>R_\nabla(X,Y) = \nabla_X\nabla_Y - \nabla_Y\nabla_X - \nabla_{[X,Y]}</math>
<math>R_\nabla(X,Y) = \nabla_X\nabla_Y - \nabla_Y\nabla_X - \nabla_{[X,Y]}</math>


The notion of curvature actually makes sense for any connection. In the case of a linear connection, it is tensorial, with lots of nice properties. It is in fact a (1,3)-tensor called the [[Riemann curvature tensor]].
The notion of curvature actually makes sense for any connection.

Latest revision as of 16:03, 26 May 2025

This lives as an element of: the space of -bilinear maps

Definition

Given data

  • A connected differential manifold with tangent bundle denoted by

Definition part (pointwise form)

A linear connection is a smooth choice of the following: at each point , there is a map , satisfying some conditions. The map is written as where and .

  • It is -linear in (that is, in the coordinate).
  • It is -linear in (viz the space of sections on ).
  • It satisfies the following relation called the Leibniz rule:

Definition part (global form)

A linear connection is a map , satisfying the following:

  • It is -linear in the first
  • it is -linear in the second
  • It satisfies the following relation called the Leibniz rule:

where is a scalar function on the manifold and denotes scalar multiplication of by .

Generalizations

The notion of linear connection can be generalized to the more general notion of a connection, where the second is replaced by an arbitrary vector bundle over .

Operations on a linear connection

Torsion of a linear connection

Further information: torsion of a linear connection

The torsion of a linear connection is denoted as . It is a -tensor defined as:

.

A connection whose torsion is zero is termed a torsion-free linear connection.

Note that torsion makes sense only for linear connections.

Curvature of a linear connection

Further information: Riemann curvature tensor

The curvature of a linear connection is denoted as . It is defined as:

The notion of curvature actually makes sense for any connection.