How to intuitively understand parallel transport

In the article I’ve referenced below, and many other articles for that matter, the notion of parallel transport along a line of latitude θ=θ0 on the unit 2-sphere is spoken about. What I can’t understand is, intuitively, how there is any “rotation” after circuiting the full line-of-latitude path.

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The above illustration is my understanding of what is meant by “parallel transport of a vector along the θ or ϕ direction”. Clearly, after completing a full path, the rotation of the vectors is always exactly 2π, and hence the parallely transported vectors are left unchanged. What have I misunderstood? My understanding doesn’t seem to match with the results derived in the article below.



I was also having trouble with this for a long time. The explanation which finally worked for me was the following:

For the purposes of parallel transport along a particular circle of latitude, the sphere can be replaced by the cone which is tangent to the sphere along that circle, since a “flatlander” living on the surface and travelling along the circle would experience the same “twisting of the tangent plane in the ambient space” regardless of whether the surface is a sphere or a cone.

And for the cone, there’s an easy way of seeing that there is indeed a rotation of the transported vector with respect to the tangent vector of the curve: just cut the cone open and lay it flat on the table, so that parallel transport becomes simply ordinary parallel transport on the plane.

A picture says more than a thousand words, and I found a good one here:
A simple discussion of the Berry Phase (N. P. Ong, Physics, Princeton Univ.).

Source : Link , Question Author : Arturo don Juan , Answer Author : Hans Lundmark

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