Can we truly destroy a proton or nucleon?

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Discussion Overview

The discussion centers around the possibility of destroying a nucleon, specifically whether it can be obliterated or if it can only be transformed into other particles. Participants explore the implications of high-energy collisions, such as those at the LHC, on nucleons and the conservation of baryon number.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that while nucleons can be subjected to high-energy collisions that may "rip" them apart, this process creates new particles rather than simply destroying them.
  • Others argue that the resultant particle shower from such collisions may not always include protons or neutrons, although baryon number must be conserved overall.
  • A later reply questions whether it is possible to have a collision result in no protons or neutrons, suggesting that while they may not appear immediately, they eventually decay from other baryons present.
  • Some participants note that all free baryons eventually decay to protons, and the only way to eliminate a proton is through interactions with anti-baryons, although this is contingent on high energy and density conditions.

Areas of Agreement / Disagreement

Participants express differing views on whether nucleons can be considered destroyed in high-energy collisions, with some asserting that they are transformed rather than lost, while others emphasize the conservation of baryon number and the eventual return of nucleons through decay processes. The discussion remains unresolved regarding the implications of these interactions.

Contextual Notes

Participants highlight limitations in measuring certain outcomes of collisions due to experimental challenges, and there is an acknowledgment of the dependence on energy levels and conditions for certain processes to occur.

DiracPool
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Or, more generally, can we destroy a nucleon? I know we can convert between a proton and a neutron, but what about obliteration? If we try to separate a quark from a nucleon we cannot do so because we bud off an anti-quark and the original quark goes back in (or something like that). So we can't measure any free quarks. Does this mean that we can't bust open a nucleon? If we can, then what happens, the nucleon just become a bunch of neutrinos, lepton's, and photons? Are we removing protons from the universe's pool at the LHC?
 
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Sure, you can hit a nucleon so hard that you "rip" it apart. But the energy required to do so is so high that you actually end up CREATING new particles from the energy, resulting in a shower of new particles emerging from the collision. The higher the energy of the collision the more particles and the higher mass they generally are. There isn't a "pool" of particles we take from, they are actually created from energy. The energy doesn't disappear, it is converted into mass per E=MC2.
 
There isn't a "pool" of particles we take from, they are actually created from energy.

OK, I get that, but when we add energy through acceleration to these protons in the LHC, collide them, and get the shower of new particles, is there ever an instance where the resultant shower does NOT include a proton or neutron in the product? That is, the product of the collision is a zoo of particles that are perhaps just leptons and photons, and/or maybe heavy quarks?
 
is there ever an instance where the resultant shower does NOT include a proton or neutron in the product?
It is hard to measure this rate (due to experimental issues), but it is certainly possible to have no proton and neutron after the collision.
At the same time, you have to conserve baryon number. Those collisions have to have other baryons in the final state, and those decay to protons and/or neutrons after a while.
 
Those collisions have to have other baryons in the final state, and those decay to protons and/or neutrons after a while.

Interesting...so qualitatively you do not, in fact, lose a nucleon in the end result.
 
DiracPool said:
Interesting...so qualitatively you do not, in fact, lose a nucleon in the end result.

If it's not there after the collision, I would say you do. Even if you eventually get a few back after decays.
 
As mfb said, you have to conserve baryon number. So you need at least one baryon at all times. Nucleons (protons and neutrons) aren't the only baryons.
 
jtbell said:
As mfb said, you have to conserve baryon number. So you need at least one baryon at all times. Nucleons (protons and neutrons) aren't the only baryons.

But, every free baryon eventually decays down to a proton. The only way to get rid of a proton is with an anti-proton (or other anti-baryon). Well, that is, unless you're at sufficiently high energy (and, probably, density) that non-perturbative weak processes are accessible, in which case it's possible to have a proton (or, perhaps, more correctly, its constituents) decay in a way that produces an anti-lepton. But, that's not something that happens at any noticeable rate at ordinary scales.
 
sure.
 

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