Inner product of parallel transported vectors along a curve

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SUMMARY

The discussion centers on the relationship between the covariant derivative of the inner product of parallel transported vectors \( A \) and \( B \) along a curve. It is established that if the covariant derivative \( \nabla_{\mathbf{l}}(g(A,B)) = 0 \), then the inner product \( g(A,B) \) remains constant along the curve. The participants confirm that the condition of zero covariant derivatives for both vectors implies that their inner product does not change, reinforcing the concept of parallel transport in differential geometry.

PREREQUISITES
  • Understanding of covariant derivatives in differential geometry
  • Familiarity with inner products and their properties
  • Knowledge of parallel transport concepts
  • Basic grasp of tensor notation and operations
NEXT STEPS
  • Study the properties of covariant derivatives in Riemannian geometry
  • Explore the implications of parallel transport on curvature
  • Learn about the role of inner products in the context of differential forms
  • Investigate the relationship between geodesics and parallel transport
USEFUL FOR

This discussion is beneficial for students and researchers in differential geometry, particularly those studying Riemannian manifolds, as well as mathematicians interested in the applications of parallel transport and covariant derivatives.

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Homework Statement


Given that the vectors [tex]\underset{A}{\rightarrow}[/tex] and [tex]\underset{B}{\rightarrow}[/tex] are parallel transported along a curve:
[tex]\triangledown _{\underset{l}{\rightarrow}}A = 0[/tex]
[tex]\triangledown _{\underset{l}{\rightarrow}}B = 0[/tex]

Show that g(A,B) = constant along the curve

Homework Equations


The Attempt at a Solution


I just have one major question for this problem: can one say that if the covariant derivative of g(A,B) = 0 then g(A,B) = constant i.e. if
[tex]\triangledown _{\underset{l}{\rightarrow}}(g(A,B)) = \triangledown _{\underset{l}{\rightarrow}}(g_{\alpha \beta }A^{\alpha }B^{\beta }) = A^{\alpha }B^{\beta }\triangledown _{\underset{l}{\rightarrow}}g_{\alpha \beta } + g_{\alpha \beta }B^{\beta }\triangledown _{\underset{l}{\rightarrow}}A^{\alpha} + g_{\alpha \beta }A^{\alpha }\triangledown _{\underset{l}{\rightarrow}}B^{\beta } = 0[/tex]

then g(A,B) = const. for the curve?
 
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Sure, that's right. Now what's the covariant derivative of g?
 

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