Neutral Current - Neutrons and Neutrinos

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SUMMARY

The discussion centers on the observation of neutral current events in particle physics, specifically the interaction involving neutrinos and neutrons. The process described is \bar{\nu}_\mu + n \longrightarrow \bar{\nu}_\mu + X, where X can include particles like \pi^0 or charged pions resulting from interactions in a bubble chamber. The Gargamelle bubble chamber at CERN is highlighted as a significant detector for neutrinos, capable of observing charged particles produced from such interactions. The conversation emphasizes the necessity of energy input for pion production and the complexities of particle identity during these interactions.

PREREQUISITES
  • Understanding of neutral current interactions in particle physics
  • Familiarity with bubble chamber technology and its limitations
  • Knowledge of particle decay processes, specifically nucleon interactions
  • Basic grasp of quantum chromodynamics (QCD) and particle production mechanisms
NEXT STEPS
  • Study the mechanics of neutral current interactions in detail
  • Explore the role of bubble chambers in particle detection, focusing on the Gargamelle detector
  • Investigate pion production mechanisms in nucleon interactions
  • Learn about quantum chromodynamics and its implications for particle interactions
USEFUL FOR

Particle physicists, students of quantum mechanics, and researchers interested in neutrino interactions and particle detection methodologies will benefit from this discussion.

Ahmes
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Hi,
We were told in a very-elementary elementary particles course, that a neutral current event was first observed in the following process:
\bar{\nu}_\mu + n \longrightarrow \bar{\nu}_\mu + X
were X is "something other than muon" (n was a neutron).

I thought about it, and I don't know how X can be something other than a n, a neutron. The interaction between the neutrino and one of the neutron's quark is second order and flavor conserving, so only the momentum changes and not the particle identity.

Yet, I've searched the internet and found that it can also be:
X=n + \pi^0[/itex]<br /> Where did the pion come from? there should be a photon or a gluon involved if it is to appear from the vacuum. How will the correct diagram look like? And what other things could X be?<br /> <br /> And maybe even a more important question - the experiment was said to be done inside of a bubble chamber - BUT WE CAN ONLY SEE CHARGED PARTICLES THERE, NOT NEUTRONS, NEUTRINOS &amp; NEUTRAL PIONS...<br /> <br /> Can someone help?<br /> Thanks!
 
Last edited:
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Re Bubble Chamber:
Wiki said:
Gargamelle was a giant particle detector at CERN, designed mostly for the detection of neutrinos. Gargamelle was a bubble chamber that held nearly 12 cubic meters of freon (CF3Br). It operated for many years at the CERN PS and SPS.

There must be energy put into the system for the pion to be there.

A really elementary introduction to the neutral current is given here at hyperphysics:
http://hyperphysics.phy-astr.gsu.edu/hbase/particles/neucur.html
 
Pions interact strongly with nucleons, so often if you hit a nucleon, a pion will be produced. The struck neutron could have produced a proton and a pi-, each of which would be seen in a bubble chamber.
 
OK, the process is detectable if the resultant particles are charged. Let's say they really are a pi- and a proton.

u ----->---- u
d ----->---- d
000000000-->-- u
gluon? ---<
000000000--<-- ubar
d ----->---- d
00000|
00000|Z
00000|
ν ----->---- ν

(Don't notice the white zeros - they are just for alignment)

If that is the diagram - then there's still the gluon or photon that comes from nowhere...
 
Ahmes said:
Hi,
We were told in a very-elementary elementary particles course, that a neutral current event was first observed in the following process:
\bar{\nu}_\mu + n \longrightarrow \bar{\nu}_\mu + X
were X is "something other than muon" (n was a neutron).
Hey,

I refer you to a post from our Elementary Particles Presented thread in which you will find ALL the necessary information you are looking for. Click on the links in the end of the page !

regards
marlon
 
The first step is nu+n-->nu_+n.
Then n-->p+ pi. Anytime you hit a nucleon it can shake off pions.
 

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