Hi everybody I thought I'd introduce myself. I have been lurking

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Hi everybody! I thought I'd introduce myself. I have been lurking around on this forum for awhile now. Yes, I am a newb.
I'm 14 and I'm doing A science fair project on particle physics. I watched a documentry on the search for the Higg's Boson particle and I thought it would be a interesting topic.
I have some understanding of particle physics. After I figured out what I was doing, I read the book " the God Particle" By Leon Lederman which gave me a very brief understanding of quarks, leptons, forces ect.
I still have a lot of questions and I only have two weeks to finish my project. I hope you can help.

James
 
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Welcome to PF, you will find a lot of people who share the same interest.
 
I read that book too.

It's a great book and Double-L is a remarkable Physicist.

If you want to go just a little bit deeper read The Theory of Almost Everything by Robert Oerter, it explains what Leon touched on (things like QED, and QCD in a more technical term) but still leaves that nasty math stuff out for 14 year olds like you :P
 
That math stuff can be confusing :biggrin: thanks for the replys
 
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}...

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