Contravariant vs Covariant components - misprint?

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SUMMARY

The discussion centers on the terminology used in the article "Integrals in the theory of electron correlations" by L. Onsager et al., specifically regarding the use of "contravariant components" versus "covariant components" in the context of vector \(\vec{s}\) in an oblique coordinate system defined by vectors \(\vec{q}\) and \(\vec{Q}\). The components \(s_1\) and \(s_2\) are derived from the definitions of \(\vec{s}\) projected onto the basis formed by \(\vec{q}\) and \(\vec{Q}\). The consensus leans towards the term "contravariant" due to the nature of tangent vectors in manifold theory, although the terminology is criticized for its complexity and potential confusion.

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In their article [Integrals in the theory of electron correlations, Annalen der Physik 7, 71] L.Onsager at el. write:

By resolving the vector \vec{s} into its contravariant components in the oblique coordinate system formed by the vectors \vec{q} and \vec{Q} it is possible to reduce the region of integration (3.11) to a rectangle. The contravariant components of \vec{s} are defined by:

s_1 = \frac{\vec{s}\vec{q}}{|q|}, \quad s_2 = \frac{\vec{s}\vec{Q}}{|Q|}

Shouldn't they write "covariant components"?

PDF of the article can be found here: http://zs.thulb.uni-jena.de/receive/jportal_jparticle_00133463

Thank you.
 
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Why should it be "covariant"? I don't see a reason to mention either of those words. ##s_1## and ##s_2## are just the components of ##\vec s## in the ordered basis ##\Big\langle\frac{\vec q}{|\vec q|},\frac{\vec Q}{|\vec Q|}\Big\rangle##.

However, if I had to choose one of those words, I'd go with "contravariant", because when ##\{e_i\}## is a basis for the tangent space of a manifold, a tangent vector v can be expressed as ##v=v^i e_i##, and the ##v^i## are said to define a contravariant vector. (I strongly dislike this terminology, and don't understand why people are still using it). The "covariant components of ##\vec v##" in this (horrible) terminology would be components of the 1-form ##g(\vec v,\cdot)## in the dual basis for the cotangent space that's the dual basis of ##\{e_i\}##.

Also note that if the manifold is Euclidean, the contravariant and covariant components are the same.
 

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