Attractive nature of nuclear forces

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Discussion Overview

The discussion centers on the nature of nuclear forces, specifically the transition from attractive to repulsive forces at short distances between nucleons, with a focus on the underlying mechanisms and theoretical explanations. The scope includes theoretical considerations, particle exchange models, and quantum mechanics implications.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants note that the nuclear force is attractive at distances around 1.5 fermi but becomes repulsive at approximately 0.5 fermi, questioning the reasons behind this transition.
  • One participant suggests that a full explanation requires lattice QCD calculations, while qualitatively relating the nuclear force to meson exchange, particularly the pion and ω meson, which have different mass implications for the range of the force.
  • Another participant seeks clarification on how the properties of exchanged particles determine whether the force is attractive or repulsive, referencing discussions from quantum field theory literature.
  • A participant mentions that while the Pauli exclusion principle can provide insight into repulsion, it does not fully explain the underlying reasons for the observed nuclear force characteristics.
  • One participant introduces the concept of quantum degeneracy pressure as a potential explanation for repulsion, particularly in the context of neutron stars, but acknowledges limitations in applying this to all nucleon interactions.
  • Another participant counters that Pauli degeneracy cannot solely explain the repulsive core, as it also exists in proton-neutron interactions and highlights the role of spin states in determining the effects of the exclusion principle.

Areas of Agreement / Disagreement

Participants express differing views on the mechanisms behind the nuclear force's attractive and repulsive nature, with no consensus reached on a singular explanation. The discussion remains unresolved regarding the precise reasons for the observed behavior of nuclear forces at short distances.

Contextual Notes

Participants acknowledge that the explanations involve complex interactions and theoretical frameworks, with some aspects remaining beyond current understanding. The discussion highlights the dependence on definitions and the need for further exploration in quantum chromodynamics and particle physics.

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"At a distance of 1.5 fermi, the nuclear force becomes maximum and remains attractive in nature. However, at a distance of 0.5 fermi, the nuclear force suddenly becomes repulsive. "

Revered Members,
Nuclear force is a short range force, so naturally when the distance between the nucleons decrease, there should be more attractive force. I can't understand why repulsive force becomes predominant when the distance between the nucleons is of the order of 0.5 fermi.
 
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To really answer this question is quite difficult, since nucleons are made of quarks and gluons, and a full explanation must be sought in lattice QCD calculations. However you can understand it qualitatively the old-fashioned way, in terms of meson exchange. The original idea by Yukawa was that the nuclear force was caused by exchange of an as yet unknown particle. The range of the force would be inversely related to the particle's mass. Sure enough the pion was discovered, with a mass of 140 MeV, implying a range of 197.5/140 = 1.4f.

But is the exchange force attractive or repulsive? That depends on the properties of the particle, namely its behavior under charge conjugation. Pion exchange, it turns out, is attractive. The repulsive part has been sometimes explained by exchange of another particle, the ω meson with spin one and a mass of 780 MeV. The range this time is 197.5/780 = 0.25 f.

There are more elaborate explanations floating around. My main point is that particle exchange does not have to imply an attractive potential, it can be either.
 
Bill_K said:
But is the exchange force attractive or repulsive? That depends on the properties of the particle, namely its behavior under charge conjugation.

Could you please elaborate more on this?
I also have no real understanding as how to read of from the characteristics of the particle exchanged whether it will lead to attraction or repulsion. I remember Zee discussing it in his QFT book and linking it to the spin of the particle although I found his argument still quite involved.
 
I can't understand why repulsive force becomes predominant when the distance between the nucleons is of the order of 0.5 fermi.


'why' questions ultimately have very few good answers. 'what' happens we are better at describing because we have observational evidence.

As easy way to think about the replusion is Pauli exclusion...but of course that doesn't
really explain 'why'...

Check this out for a description of observed characteristics,
http://en.wikipedia.org/wiki/Nuclear_force

but again exactly 'why' all this occurs is still a bit beyond our reach.
 
ok, it IS a result of 'quantum degeneracy pressure'...I've only read about the electron and neutron degeneracy in stars
version, and wikie doesn't have an article on the more general topic.


Electron degeneracy pressure is a particular manifestation of the more general phenomenon of Quantum degeneracy pressure. The Pauli Exclusion Principle disallows two half integer spin particles (fermions) from occupying the same quantum state at a given time. The resulting emergent repulsive force is manifested as a pressure against compression of matter into smaller volumes of space.

http://en.wikipedia.org/wiki/Electron_degeneracy_pressure

edit: Found this additional tidbit:
"Neutron Degeneracy Pressure: Quantum mechanics restricts the number of neutrons that can have low energy. Each neutron must occupy its own energy state. When neutrons are packed together, as they are in a neutron star, the number of available low energy states is too small and many neutrons are forced into high energy states. These high energy neutrons make up the entire pressure supporting the neutron star. Because the pressure arises from this quantum mechanical effect, it is insensitive to temperature, i.e., the pressure doesn't go down as the star cools. Similar to electron degeneracy pressure but, because the neutron is much more massive than the electron, neutron degeneracy pressure is much larger and can support stars more massive than the Chandrasekhar mass limit..."


http://www.astro.virginia.edu/~jh8h/glossary/neutrondegen.htm
 
Naty1, Pauli degeneracy cannot be the explanation, since the same repulsive core exists in the interaction between a proton and a neutron. Also between two protons, the exclusion principle needs to be taken into account in the triplet state (spins the same) but does not affect the singlet state.
 

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