Pion+/- decay - what *Exactly* is happening?

[Asgrrr]

I have seen vague explanations and (to me) misleading diagrams, and I am still not completely sure what is supposed to be happening in pion+/- decay. This Feynman diagram is a starting point.
https://en.wikipedia.org/wiki/Pion#/media/File:PiPlus_muon_decay.svg
What is happening? What happens to the quarks? I'm not asking for the unknowable, just a reasonable description of events and the fate of particles.

Thank you.

 

[mfb]

What is happening?

A pion decays to a muon plus a neutrino. The coupling is mediated by the W field.
The quarks stop existing.

Don't take Feynman diagrams too literally.

 

[Orodruin]

To build on that, Feynman diagrams are really mathematical objects that represent different terms in a series expansion. It is easy to be misled into thinking that there are particles running around like that and physicists will often use a language that suggests that.

 

[Asgrrr]

I'm grateful for the replies I'm sure. However, I'm working on teaching materials for high school/college. I am hoping for some way to explain pion decay in the terms of already established weak interactions involving the W particle. Help with that would be much appreciated.

 

[Orodruin]

I am not sure you can explain Feynman diagrams to high school students without a significant amount of "lying to children". You need a large amount of background to just understand what a particle physicist means when (s)he says "particle", let alone what the lines in a Feynman diagram represent.

 

[ChrisVer]

Since it's for teaching matterial:
The level of the class should be considered. As a result if you, as a a teacher, can't interpret well the lines of a Feynman Diagram, you should rethink of introducing the decay through it... If Ws are already introduced (wow), then you can just tell that the udbar quarks annihilate via a virtual W boson which couples to a lepton+neutrino.
How would you answer the simpler question of "what happens to the muons" when a muon and antimuon annihilate to electron+positron?
In fact, outside the context of a quantum theory, the only way you can introduce Feynman diagrams is by giving the students a list of conservation laws (eg charge conservation) and rules (eg flavor changing happens only via Ws), and making them play with the possible Feynman Diagrams (since they are made such that all conservations laws are satisfied in every vertex). They can't be thought as what "really" happens as others mentioned, or as you can understand by the fact that you integrate over all the spacetime the vertices of the internal lines.

 

[Asgrrr]

To clarify, it was never my intention to use Feynman diagrams as the basis of the treatment. I might show one or two for curiosity. What I am after in this thread is connecting pion decay to specific, established weak interaction(s) involving quarks, that's all.

 

[ChrisVer]

as an up-quark can be transformed to a down-quark by emitting a W (eg in beta processes), an up-quark and an anti-down-quark can "decay" into a W (virtual or real depending on the available energy, for the pion decay that's virtual)... The W decays to quarks (giving birth to mesons/hadrons) or leptons (e/mu/tau+neutrino), however because the pion is the lightest meson, the only energy-conserving decays are those to leptons (and in particular to electron or muon).

 

[Asgrrr]

PS: for some reason a quote from "Fear and Loathing in Las Vegas" keeps coming to mind when looking at this thread:

"Finish the f-ing story! What happened? What about the glands?"

For "glands" insert "quarks".

Don't take it the wrong way please.

 

[mfb]

See above: They stop existing.

 

[ChrisVer]

what about them? they're are no more (before you had a pion, then you have the leptons)... if they didn't disappear we wouldn't call it a decay but radiation (or something).

How would you answer the simpler question of "what happens to the muons" when a muon and antimuon annihilate to electron+positron?

 

[Asgrrr]

Sorry I didn't see your reply earlier, ChrisVer, my silly quote was not a response to you. I feel we are getting somewhere now.

I'll express antiquarks as ~x.

We start with a let's say u~d (Pion). That decays into W, disappearing both u and ~d.

That doesn't feel right to me as the end of the story. I have a problem with two particles decaying at once in this manner.

Can we say that the established decay of u -> d + W leaves us with d and ~d which immediately annihilate each other in the established way? Photons are not produced because they are not needed. The W carries away the energy and momentum.

That sounds much better to me.

 

[ChrisVer]

That doesn't feel right to me as the end of the story. I have a problem with two particles decaying at once in this manner.

what's that problem? They don't decay at once (it's not like a double beta decay), they annihilate each other.

Can we say that the established decay of u -> d + W leaves us with d and ~d which immediately annihilate each other in the established way?

I don't understand what you mean here, is ~d a $\bar{d}$ ? And why would you need a ddbar (or where did you find it)? I also don't understand the "photons are not needed"...

 

[Asgrrr]

Yes, a ~d is as you print it, anti-d. I'm not that good with symbols here.

My problem is, what is it that gets u and ~d to annihilate each other? What allows that? They are not each other's antiparticle, and it doesn't happen inside protons for example (or does it?). This doesn't feel like a fundamental interaction, which leads me to think there's more to the story.

What I was trying to say, is that if we start out with a pion, we have a u~d. That's a pion. Now, if the u decays to d via

u → d +W

which is an established, basic decay mode, then what we are left with is d~d, or a particle and its antiparticle. THAT can reasonably decay in an established fashion (pair annihilation). Usually, pair annihilation would produce photons to carry away the energy and momentum of the destroyed particles, but when the W is forming at just about the same time, the W can carry away the energy/momentum, so there is no need for photons to be emitted. This is a much better explanation of pion decay because it only appeals to already established decay modes.

Thank you for your prompt response and your patience, ChrisVer.

PS: scratch the proton example, I was mistaken there.

 

[ChrisVer]

My problem is, what is it that gets u and ~d to annihilate each other? What allows that?

Weak interactions do (via the charged W bosons). W bosons allow transitions/couplings between up-type quarks ($u,c,t$) and down-type quarks ($d,s,b$) and generally violate the flavour conservation (it's the only Standard Model interaction which does that)...
The vertices will then have any combination depending on what is incoming/outgoing (so for the ud, you can have any vertex with $ud$, $\bar{d}\bar{u}$, $\bar{u}d$ or $u\bar{d}$ )

then what we are left with is d~d

in your $u\rightarrow d W$ where is the $\bar{d}$ ? This process has the following outcomes:
$u \rightarrow d W \rightarrow d \ell \nu$
$u \rightarrow d W \rightarrow d q q'$

Usually, pair annihilation would produce photons to carry away the energy and momentum of the destroyed particles

Pair annihilation between quark-antiquarks will preferably happen via gluons, rather than photons, because of the stronger strong interactions. The only exception would be the neutral pion because again of energy conservation (at least for its decay).
The photons can't transform an up-quark to a down-quark (this would even violate charge conservation), so there can be no $ud$, $\bar{u}d$ or $u\bar{d}$ vertices with a photon coming out of them.

 

[Asgrrr]

Thank you ChrisVer.

I think you have perhaps misunderstood some things I've said, but I'm satisfied with your explanations.

 

[Orodruin]

What I was trying to say, is that if we start out with a pion, we have a u~d. That's a pion. Now, if the u decays to d via

u → d +W

which is an established, basic decay mode, then what we are left with is d~d, or a particle and its antiparticle.

This is incorrect. What is established is the vertex between the u, d, and W with a particular fermion and boson charge flow. It certainly is no "basic decay mode" as the W is much heavier than both quarks. What is established from the theory are the Feynman rules and later you have to figure out what this means for the interactions among the asymptotic states.

 

[ChrisVer]

OK I think I see what you mean now: you are saying that a charged pion coul decay to a neutral pion and a lepton(and neutrino) like a semileptonic decay? however that's very unlikely and it's a very rare way for the charged pion to decay (because a lot of energy will be kept by the neutral pion, and the W would have only energy to transfer equal to the charged minus neutral pions' masses difference (which makes it even more off-shell W).
If that's what you meant, then the neutral pion will indeed decay to 2 photons (main decay channel for the neutral pions)...

 

[mfb]

I have a problem with two particles decaying at once in this manner.

That is the process that happens. Nature doesn't care if you have a problem with its processes.

 

[Orodruin]

That is the process that happens. Nature doesn't care if you have a problem with its processes.

There is only one decaying particle, the pion. If you look at the quark level it is a binary interaction between the bond state constituents.

 

[Asgrrr]

That is almost what I mean but not quite. A neutral pion is (u~u - d~d)/root2 or something like that. But after u decays into d in the charged pion we would have a pure d~d. I realize this is a state that would probably be impossible to detect, I'm looking for a rationalization.

 

[vanhees71]

http://pdglive-temp.lbl.gov/Particle.action?init=0&node=S009

 

[ChrisVer]

uubar or ddbar can be neutral pions... the expression you show doesn't make sense in terms of quark content (what does MINUS stand for?)...
Nevertheless, the $\pi^\pm \rightarrow \pi^0 e^\pm \nu$ exists, however the dominant decay is the fully leptonic one to muons (mostly) and electrons (less)

 

[Orodruin]

uubar or ddbar can be neutral pions... the expression you show doesn't make sense in terms of quark content (what does MINUS stand for?)...

Uhmmmm, it is the linear combination of states that makes a neutral pion. The other linear combination is not a pion.

 

[Asgrrr]

uubar or ddbar can be neutral pions... the expression you show doesn't make sense in terms of quark content (what does MINUS stand for?)...
Nevertheless, the $\pi^\pm \rightarrow \pi^0 e^\pm \nu[\itex] exists, however the dominant decay is the fully leptonic one to muons (mostly) and electrons (less)$

$<br /> <a href="https://en.wikipedia.org/wiki/Pion" target="_blank" class="link link--external" rel="nofollow ugc noopener">https://en.wikipedia.org/wiki/Pion</a><br /> <br /> See table at bottom of article.$

 

[ChrisVer]

Uhmmmm, it is the linear combination of states that makes a neutral pion. The other linear combination is not a pion.

However a neutral pion is either uubar or ddbar...

 

[mfb]

However a neutral pion is either uubar or ddbar...

No, it is the linear combination, as Orodruin said already.

 

[ChrisVer]

No, it is the linear combination, as Orodruin said already.

OK, draw the Feynman Diagram of the linear combination for me and I would really like to see how you'd represent the (-) and where the /sqrt(2) appears, try the decay $\pi \rightarrow \pi^0 e \nu$... or diagrams like in Fig.2(a,b) and the blue neutral pion (for I don't see a uubar-ddbar), neither do I know a Z decaying to both a uubar and ddbar to give a neutral pion (d) http://www2.kek.jp/en/press/2008/BellePress12e.html
The combination appears only when you want to write the neutral pion's wavefunction in flavor space... afterall superpositions aren't natural.

 

[vanhees71]

uubar or ddbar can be neutral pions... the expression you show doesn't make sense in terms of quark content (what does MINUS stand for?)...
Nevertheless, the $\pi^\pm \rightarrow \pi^0 e^\pm \nu$ exists, however the dominant decay is the fully leptonic one to muons (mostly) and electrons (less)

The mesons are grouped according to isospin (or its SO(3) generalization if you wish). Take $\psi=\binom{u}{d}$ for the first-generation quarks, forming an iso-doublet. Out of those you can build the pions by
$$\vec{\pi} = \bar{\psi} \vec{\tau} \gamma_5 \psi,$$
making them an isovector (isospin 1) triplet, the charged pions are given by $\pi^{\pm}=\pi_1 \pm \mathrm{i} \pi_2$ and the neutral pion is $\pi^0=\pi_3$. The $\vec{\tau}$ are the isospin-Pauli matrices and thus indeed $\pi^0=\bar{u} \gamma_5 u-\bar{d} \gamma_5 d$ (without caring about normalizations here). The iso-singlet is the scalar $\sigma$ meson (or $f^0$): $\sigma=\bar{\psi} \psi=\bar{u} u + \bar{d} d$, forming the other neutral combination of light quarks.

Whether or not you put factore $1/\sqrt{2}$ or $1/2$ there is a matter of convention, and there are at least three conventions for the pion-decay constant in the literature all different by factors $\sqrt{2}$ or $2$ from each other. For more details with all the factors (hopefully ;-)) in place, see theory lecture I under

http://th.physik.uni-frankfurt.de/~hees/hgs-hire-lectweek17/

 

[ChrisVer]

The mesons are grouped according to isospin (or its SO(3) generalization if you wish). Take $\psi=\binom{u}{d}$ for the first-generation quarks, forming an iso-doublet.

Whether or not you put factore $1/\sqrt{2}$ or $1/2$ there is a matter of convention, and there are at least three conventions for the pion-decay constant in the literature all different by factors $\sqrt{2}$ or $2$ from each other. For more details with all the factors (hopefully ;-)) in place, see theory lecture I under

Still I think this works only for effective field theories, since you mention the $f_\pi$ (pion's decay constant). In that case you wouldn't represent the pion as a combination of quarks but as a single line (scalar field) in a Feynman Diagram (see eg some neutral pion decay diagrams), which is exactly what you do when you try to define it as a "field".