Group consists of a set and an operation

  • Thread starter Thread starter greatscott
  • Start date Start date
  • Tags Tags
    Group Set
greatscott
Messages
14
Reaction score
0
When physicists say "elementary particles form a group," what kind of operations and sets are in question? (I presume, a group consists of a set and an operation)
 
Last edited by a moderator:
Physics news on Phys.org
Ok, the operation for SU(n) is always matrix multiplication.
Now my next question is, what kind of matrices are concerned? What do the elements of the matrices represent?
 
Nope,u missunderstood.They do not form a group,they are irreductible representations of continuous groups...To fully understand it,u must know group theory and their representations...

Daniel.
 
So the continuous group has all the information and things like spin (SU(2)) are just "parts" of it?
 
I have written all this in my journal. Just look for the "introduction to string theory"-entry, part one. There is a paragraphe especially dedicated to how field theories are constructed using global and local symmetries...When imposing such local symmetries, gauge-particles arise...Check it out, it is all in there

regards
marlon
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
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}...
Back
Top