Subatomic rotations in a plane Abelian group

genloz
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Hi.. I recently stumbled across a question that seemed a little bit odd "Show that the set of rotations in a plane form a SO(2) Abelian group." for a subatomic physics course. I know how to obtain the answer showing that A^TA=AA^T=1... what I don't understand is what the relevance to subatomic physics is and what type of physics process it's modelling...
Thanks!
 
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genloz said:
Hi.. I recently stumbled across a question that seemed a little bit odd "Show that the set of rotations in a plane form a SO(2) Abelian group." for a subatomic physics course. I know how to obtain the answer showing that A^TA=AA^T=1... what I don't understand is what the relevance to subatomic physics is and what type of physics process it's modelling...
Thanks!

just to give a verbal example; neutral meson states, by quark content, fluctuate. The amplitudes of quark content in mesons can be modeled in a unitary matrix that follows the same condition as your example, but has a dimension for each quark type. The amplitudes are related to mixing angles that mix the masses of related mesons in the "mass squared matrix" for a given quantum number.
 
You should take a look at Noether's theorem and the relationship between symmetries of a group and conservation laws.
 
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I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
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