What is U(1) Lie Group? | Abelian Lie Group | Unit Circle

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U(1) is defined as the 1-parameter Abelian Lie group represented by the unit circle, specifically characterized by the equation e^{iθ}. It is isomorphic to rotations about the unit circle and can be understood as the group of 1x1 unitary matrices where x* = x^-1. In the context of gauge theories, U(1) signifies invariance under local U(1) gauge transformations, contrasting with global transformations. This foundational concept is crucial for establishing more complex theories involving SU(2) and SU(3) gauge transformations relevant to weak and strong force physics.

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Matterwave
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I keep hearing statements like "XXX theory is based on U(1)" or some such, but I haven't heard what this group actually is. If U(N) are the NxN unitary matrices, then U(1) are the 1x1 matrices such that x*=x^-1. So, I just want to confirm then, that U(1) is simply the 1 parameter Abelian Lie group given by e^{i\theta}? This is simply the unit circle right, and should be isomorphic to rotations about a unit circle?
 
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Matterwave said:
U(1) … is simply the unit circle right, and should be isomorphic to rotations about a unit circle?

Yup! :smile:
 
Matterwave said:
I keep hearing statements like "XXX theory is based on U(1)" or some such, but I haven't heard what this group actually is. If U(N) are the NxN unitary matrices, then U(1) are the 1x1 matrices such that x*=x^-1. So, I just want to confirm then, that U(1) is simply the 1 parameter Abelian Lie group given by e^{i\theta}? This is simply the unit circle right, and should be isomorphic to rotations about a unit circle?

Yes, it's not very impressive. Though when we say a U(1) gauge theory we mean the physics is invariant to a LOCAL U(1) gauge transformation (i.e exp(i theta(x)), not just a global one (i.e. exp(i* constant)). However, the reason we label such a simple thing is because we also then establish theories which are invariant under SU(2) and SU(3) local gauge transformations which gives us the weak and strong force physics.
 
Ok, last question. Is U(1) identical (homomorphic or diffeomorphic?) to SO(2) then?
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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