CP violation and allowed interactions

Safinaz
Messages
255
Reaction score
8
Hi,

My question about CP- violation, but it has many parts, so I appreciate any help about..

First: I know that, any complex coupling leads to CP - violation, so if for example A is a complex scalar, and H is a real scalar, interaction as: A HH will be forbidden if we considered CP conservation, but what about H A A, will it be allowed ?

Second: I read that ## ^{(1)} ## there is no coupling as : Z A A, because CP–invariance im-
plies that the two Higgs bosons must have an opposite parity. I don't understand why cp -invariance implies that ?

And what about a coupling to a gluon as: G S S ( consider S is a coloured cp- odd or cp- even scalar), will it be allowed ? I mean is there in the strong interactions CP - invariance or violation (since CP- violation observed only in the EW interactions )

Bests,
s

(1) " arXiv:hep-ph/0503173v2 ", Sec. 1.2.3,
 
Physics news on Phys.org
Hi!

Before trying to answer (I am also not an expert but I am trying to learn this stuff my self), I am confused by your question.

You say that any complex coupling generates CP violation. What do you mean? A complex coupling constant, say 'g'? Or a vertex which contains a complex field? The you say that AHH would be forbidden for this reason (because there is one complex field?), and you ask whether HAA would be forbidden. You mean HA*A I guess...

Second, you say " Z A A, because CP–invariance implies that the two Higgs bosons must have an opposite parity"

Where is the Higgs boson here? Are you assuming a CP odd Higgs boson?
 
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