Deflecting high energy proton beam

GCyrille
Messages
1
Reaction score
0
hi everyone,

I have a question concerning the magnets physics more precisely about the Kickers/Dipoles.

For my work, I need to design an optical system capable of deflecting a proton beam (4 GeV) switching between to 2 angles (+ 118 mard and -118 mrad) in a raw.

Can a pulsed magnet (or a kicker) do this if it receives alternatively a negative/positive intensity? (If no intensity, the angle would be then 0 mrad).

do you know any experiment that uses this kind of deflector in the world?

best regards
 
Physics news on Phys.org
Particle accelerators use these kicker magnets for injection and extraction - switching between a configuration where the beam can orbit in cycles and a configuration where new particles can enter or stored particles can leave.
Key parameters are the necessary strength and size of the magnetic field and the time between the two field configurations.
 
  • Like
Likes geoelectronics
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