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Sure, and the effective models are governed by chiral symmetry and thus take the form they take. Pions are a bound state with the specific quark content. Already these quarks are constituent quarks of course!
You would draw both diagrams, and you have to calculate both diagrams for the decay and add their amplitudes.ChrisVer said:OK, draw the Feynman Diagram of the linear combination for me
Everything is a superposition - in most bases. Saying "this is not a superposition" without specifying a basis is meaningless. Superpositions are much more natural than the special case of pure states.ChrisVer said:afterall superpositions aren't natural.
in any case in the 1st diagram you would end up with a ddbar or with a uubar... so according to the OP, this wouldn't be a neutral pion.mfb said:You would draw both diagrams, and you have to calculate both diagrams for the decay and add their amplitudes.
The point is that you have to draw all the other diagrams as well and take the appropriate linear combination when you actually compute the decay amplitude. Indeed the uubar state is not a neutral pion, but the neutral pion projection onto the uubar direction (or vice versa) is non-zero so you have to include it when you compute the amplitude.ChrisVer said:in any case in the 1st diagram you would end up with a ddbar or with a uubar... so according to the OP, this wouldn't be a neutral pion.
Somebody should tell the ##K-\bar K## oscillations ...ChrisVer said:afterall superpositions aren't natural.
I disagree...mfb said:Everything is a superposition
Before the measurement an electron may very well be in a superposition of spin up and down. It is your measurement process that forces it to select either by singling out a basis. After your measurement each individual electron is in an eigenstate - in your chosen direction. If you change from the z to the x direction each electron is in an equal parts linear conbination so whether it is a linear combination of seceral states really is a question of your choice of basis.ChrisVer said:I disagree...
The fact that you can have an electron with spin up or spin down, doesn't mean that a single electron would have both... A collection of electrons would of course have 50% up and 50% down (given that the orientation symmetry is preserved), the single electron would have either up or down (you'd need to measure it).
Sorry Chris, but you are wrong, and repeating wrong statements won't improve them.ChrisVer said:I disagree...
The fact that you can have an electron with spin up or spin down, doesn't mean that a single electron would have both... A collection of electrons would of course have 50% up and 50% down (given that the orientation symmetry is preserved), the single electron would have either up or down (you'd need to measure it).
A superposition can be a pure state as well. I believe you mean "a measurement eigenstate".mfb said:A pure state is a very special case, in general you have superpositions.
vanhees71 said:How do you come to that conclusion? According to the particle data booklet the decay indeed happens (although quite rarely):
http://pdglive-temp.lbl.gov/BranchingRatio.action?desig=4&parCode=S008
But it's not wrong, as you can see from the particle data booklet (the branching ratio is only about ##10^{-8}##, but it's a measured decay of the charged pions). I still don't understand, why you come to the conclusion that this decay cannot exist, only because the pion is the given superposition?ChrisVer said:because I couldn't produce a neutral pion according to the definition I am getting: I either end up with processes resulting to u\bar{u} or to d\bar{d} (so projections of the neutral pion, as well as the sigma mesons)... I originally said that the decay was possible (like a semileptonic meson decay), since those were actually neutral pions but I was wrong.
There is no such thing, and a W cannot decay to a single meson anyway.ChrisVer said:Also what's the meson that has the state: u\bar{d} \pm u\bar{s} \pm u \bar{b} \pm c \bar{s}\pm c \bar{d} \pm c \bar{b} (that would come from the W hadronic decay addition of Feynman Diagrams)?
Because that decay ends up with u\bar{u} or d\bar{d} and not in a superposition of the two... and that is not a neutral pion (as I was repeatedly told in this discussion)...vanhees71 said:I still don't understand, why you come to the conclusion that this decay cannot exist, only because the pion is the given superposition?
This is self contradictory. If it can end up in uubar and ddbar, clearly it can end up in a linear combination of those states. It is a question of what the amplitude is.ChrisVer said:Because that decay ends up with u¯uuu¯u\bar{u} or d¯ddd¯d\bar{d} and not in a superposition of the two...
What makes you think it doesn't decay to both linear combinations? The only difference is that the s quark is heavy enough for the mass eigenstates to be essentially equivalent to the flavour states, which does not happen in the pion system.ChrisVer said:my question would then be why do we get a ρ+ρ+\rho^+ (with the u¯dud¯u\bar{d} decay of a W ) and not a αu¯d+βu¯sαud¯+βus¯ \alpha u\bar{d} + \beta u \bar{s} (forgetting the bottoms due to energy).