Transformations of a vector in the active viewpoint

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The discussion focuses on the transformations of vector fields under active transformations as described in Peskin and Schroeder. It highlights that under 3-dimensional rotations, the vector field transforms as ##V^{i}(x) \rightarrow R^{ij}V^{j}(R^{-1}x)##, and under Lorentz transformations, it transforms as ##V^{\mu}(x) \rightarrow \Lambda^{\mu}_{\nu}V^{\nu}(R^{-1}x)##. The key point is that while the vector field is actively rotated, the coordinate system remains fixed, leading to a distinction between rotating the vector field and merely changing its components. The discussion clarifies the importance of applying the transformation matrix to the vector field while using the inverse transformation matrix on the coordinates.

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In Peskin and Schroeder page 37,

a diagram illustrates how, under the active transformation, the orientation of a vector field must be rotated forward as the point of evaluation of the field is changed.

I understand that the change of the orientation of the vector field is the same idea as that of the transformation matrix mixing up the vector field components to form the new vector field components.

Now, the textbook goes on to mention that:

under 3-dimensional rotations, ##V^{i}(x) \rightarrow R^{ij}V^{j}(R^{-1}x)##
under Lorentz transformations, ##V^{\mu}(x) \rightarrow \Lambda^{\mu}_{\nu}V^{\nu}(R^{-1}x)##

I understand that because we are working in the active transformation, the vector field itself is rotated (or boosted) in space(time) and the coordinate system (or reference system) is held fixed.

Can someone explain to me in simple layman terms why we are applying the a transformation matrix on the vector field when we are using the inverse transformation matrix on the coordinates?
 
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A vector field is a map with vector domain and range. Think about the classic ##\mathbb{R}^2 \rightarrow \mathbb{R}^2## map. If you just do ##V^i(x) \mapsto R^{ij} V^j(x)## you are rotating the range vector while keeping it in the same position. That means you don't get a rotated vector field, but a completely different field. Think about the classic curling field:

300px-Irrotationalfield.svg.png


If you do ##V^i(x) \mapsto R^{ij} V^j(x)## with a 90° rotation matrix, you obtain a central vector field! While if you actively rotate the whole field, sure the resulting vector is rotated 90° but referred to the old vector function in the old position.

Edit: maybe I see where your doubt lies. For instance, you don't do ##V^i(x) \mapsto R^{ij} V^j(R x)## because the right hand side V would have to be a different function from the left hand side V to be the actively rotated field. Also, don't see in the correct formula ##V^i(x) \mapsto R^{ij} V^j(R^{-1} x)## the resulting field as a function of ##R^{-1}x##, see it as a function of ##x##. Then it will make sense.
 
Last edited:
Thanks! I get it! :smile:
 

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