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
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
By taking the exterior derivative of (23) and using (18), we get
where we put
For a fixed value of k we multiply the above equation by
getting
or ΣρaρkΠρl ≡ 0, mod ω;.
Since the infinitesimal transformations Xρ are linearly independent, this implies that
It followo that II ρ is of the form
where ϕjρ are Pfaffian forms. Substituting these expressions into (24), we get
It follows that
Since G has the property (C), the above equations imply that
OCR based on this tiff scan