
#1
May2107, 02:37 PM

P: 603

First off, what is a mass eigenstate?! Is there a (hermitian) operator associated to mass? What should I picture when discussing a nonmasseigenstate?! The same goes for a 'weak eigenstate' as the CKM matrix is supposed to be the basis transformation between these two...
The I read that 'a linear transformation which diagonalizes the mass terms of the utype quarks does not necessarily diagonalize those of the dtype quarks.' What does this mean, and why not?! Finally, I rwill be very much helped by any insight on the meaning of this matrix and its properties, e.g. why its unitary...? Sorry, the more I learn the less I seem to know... 



#2
May2207, 02:21 AM

Sci Advisor
P: 1,732

eigenstate is an eigenstate of this operator. Such a state has a determinate mass value. superposition of more than one mass eigenstate. It's mass is therefore indeterminate (i.e: there's some probability of measuring any of the mass values of the masseigenstates that have been superposed). in general, but a superposition of mass eigenstates. (u,d,etc) does not commute with the operator corresponding to the mass property. So if you choose a Hilbert space basis corresponding to the flavor eigenstates, they are in general a nontrivial superposition of mass eigenstates. unitary to preserve inner products between states in the Hilbert space.  strangerep 



#3
May2207, 01:47 PM

P: 603

Thanks very much for that! I guess that for any observable there is an operator, so also for (quark) mass and flavour. I just never came across (explicit representations of) such operators, so find them weird, rather than just an extension of what I know within the quantum formalism. Thanks very much again, for just showing that even in the standard model things are just like the hermitian operators and unitary transformations of ordinary quantum mechanics!




#4
May2307, 06:36 PM

Sci Advisor
P: 1,732

CKM Matrix and mass eigenstatesHilbert space operators. Or more precisely, it's all about relativistic QFT: unitary operators in a multiparticle Hilbert space (aka Fock space) which has been explicitly constructed so as to carry a (tensor product of) irreducible representations of the Poincare group and the various internal symmetry groups of the standard model.  strangerep. 


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