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test ocr 2

(Definition)

necessary to consider the second bundle. The curvature form of our connection is a tensorial quadratic differential form in M, of type ad(G′) and with values in the Lie algebra L(O′) of G′. Since the Lie algebra L(O) of G is a subalgebra of L(G′), there is a natural projection of L(O′) into the quotient space L(G′)∕L(G). The image of the cur- vature form under this proiection will be called the torsion form or the torsion tensor. If the forms πρ in (13) define a G-connection, the vanishing of the torsion form is expressed analytically by the con- ditions

        i′′
(22)   cf′′k′′ = 0.

We proceed to derive the analytical formulas for the theory of a G-connection without torsion in the tangent bundle. In general we will consider such formulas in BG. The fact that the O-connection has no torsion simplifies (13) into the form

(23 )   dωi = Σρ,kaiρkπρ ∧ ωk.

By taking the exterior derivative of (23) and using (18), we get

            i
(24)   Σ ρ,kaρkΠ ρAωk=0;

where we put

               ρ          ρ  σ    τ
(25)   Π ρ = dπ  + # Σ σ.τγστπ A π .

For a fixed value of k we multiply the above equation by

ω1 A. . . A ωk− 1 A ωk+1Λ ... A ωn,

getting

∑
    ai ∏ρ A ω1 A. . . A ωn =  0,
 ρ   ρk

or ΣρaρkΠρl ≡ 0, mod ω;.

Since the infinitesimal transformations Xρ are linearly independent, this implies that

                j
Π ρ ≡ 0, mod  ω .

It followo that II ρ is of the form

IA  ρ=ΣjϕρJAωf

where ϕjρ are Pfaffian forms. Substituting these expressions into (24), we get

Σ ρ,j,k(aiϕρ−ai ϕρ)AωjAωk=0.
       ρk j  ρj k

It follows that

     i  ρ    1  ρ             ′
Σ ρ(a ρkϕ f − aρjϕ k) ≡ 0, mod  ω .

Since G has the property (C), the above equations imply that

  ρ
ϕ f ≡ 0, mod  ωk.

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Cross-references: formulas, tensor, Lie algebra, type

This is version 2 of test ocr 2, born on 2009-02-07, modified 2009-02-07.
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Classification:
Physics Classification: 00. (GENERAL)

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