where . submit to my dark power. It is straightforward to invert the above and obtain . Of course, this is quite standard and ultimately only ensures that the lower dimensional fields are invariant under the mass . It is not hard to see that the same is not true for . The lower-dimensional fields transform as follows under the appropriate symmetries as follows
"The Bull and the Roe. Don't try to hurt them!" I shouted. "My cattle!" I drove them past the crops, worried they might be lost. I checked my watch against the city clock, but it was way off. One thing about this wild, wild country: it takes a strong person to make a strong line.
On a different note, the previous section discusses the invariance of lower dimensional fields under mass $mathsf{U}(1)$, and the transformation of these fields under appropriate symmetries. However, it is not clear what the purpose of these transformations is. Could you provide more context or explanation about the significance of these transformations and how they relate to the overall topic?