Nuclear Isospin: Questions on u & d Quarks and Proton & Neutron

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    Isospin
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Discussion Overview

The discussion revolves around the concept of nuclear isospin, specifically focusing on the properties of up (u) and down (d) quarks, as well as protons and neutrons. Participants explore the assignment of isospin values and the implications of quark composition on these values, including inquiries about anti-protons and anti-neutrons.

Discussion Character

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

Main Points Raised

  • Some participants confirm that u and d quarks have isospin I = ½, with u having I_3 = ½ and d having I_3 = -½.
  • There is a question regarding why protons and neutrons also have I = ½, with protons having I_3 = ½ and neutrons having I_3 = -½.
  • One participant suggests that the addition of isospin at the quark level does not lead to simple arithmetic sums due to the nature of angular momentum addition.
  • Another participant mentions that the spin of a proton is ½, despite it containing three quarks, and references the existence of the Δ+ particle with the same quark content but a spin of 3/2.
  • There are inquiries about the isospin assignments for anti-protons and anti-neutrons, with some participants expressing uncertainty and seeking confirmation.
  • Participants discuss the use of Clebsch-Gordan coefficients in quantum mechanics to calculate angular momentum combinations.

Areas of Agreement / Disagreement

Participants generally agree on the isospin values for u and d quarks, as well as protons and neutrons. However, there is uncertainty regarding the isospin assignments for anti-protons and anti-neutrons, with some participants seeking confirmation of their assumptions.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about angular momentum addition and the definitions of isospin, which are not fully resolved. The complexity of the mathematical treatment involving Clebsch-Gordan coefficients is acknowledged but not deeply explored.

malawi_glenn
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Hi you guys!

I am a little bit confused about nuclear isospin.

u and d quarks have I = ½

u has I_3 = ½ , d has I_3 = -½ (third component)

right so far?

Now why does the proton have I = ½ and I_3 = 1/2, and
neutron I = ½ and I_3 = -1/2 ??

but when you add upp the I on the quark level , you might get things like 3/2 etc, has that something to do with the strong intreaction?

And how do one assign I and I_3 to p-bar and n-bar? [anti-proton, anti-neutron]

please help dear Nuclear and Particle lovers :)
 
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malawi_glenn said:
Hi you guys!

I am a little bit confused about nuclear isospin.

u and d quarks have I = ½

u has I_3 = ½ , d has I_3 = -½ (third component)

right so far?

Now why does the proton have I = ½ and I_3 = 1/2, and
neutron I = ½ and I_3 = -1/2 ??

but when you add upp the I on the quark level , you might get things like 3/2 etc, has that something to do with the strong intreaction?

And how do one assign I and I_3 to p-bar and n-bar? [anti-proton, anti-neutron]

please help dear Nuclear and Particle lovers :)

AHH, this is a classic one. The answer goes like this :

Angular momentum doesn't add up linearly, as you were suggesting to do. That is, a proton contains three quarks, but its spin is not 3/2, but 1/2. When you add angular momentum, you have a range of possible results, which goes from the maximum (the arithmetic sum) down to the minimum (the larger minus the smaller) with possible values at unit steps in between.

If you add two spin-1/2 fermions, you get either spin 0 or spin 1 (a boson). If you add 5 units of angular momentum to 2 units, you get 3, 4, 5, 6, or 7 units of angular momentum. If you add 3/2 units and 2 units, you get 1/2, 3/2, 5/2, or 7/2 units. A proton has spin 1/2. As you should expect, there's another particle with the same quark content as the proton, but spin 3/2, the Δ+.

In QM, one can calculate all of this using the Clebsch Gordon coefficients. Do you know this technique ? If not, THIS is what you need to be studying then.

marlon
 
aha ok its "just" vector summation?

This is overcourse right now :) I will have courses in advanced QM in the autuum =) thanks!
 
malawi_glenn said:
aha ok its "just" vector summation?
No, this is slightly more elaborated :smile:
Something like "Decomposition in a direct sum of a tensor product of irreductible representations of Lie groups"
It is actually not as complicated as it might seem. You can check wikipedia about Clebsch-Gordan coefficients[/color]
 
humanino said:
No, this is slightly more elaborated :smile:
Something like "Decomposition in a direct sum of a tensor product of irreductible representations of Lie groups"
It is actually not as complicated as it might seem. You can check wikipedia about Clebsch-Gordan coefficients[/color]

hehe ****! =)
 
So does the anti-neutron have I = 1/2 and I_3 = 1/2
and anti-proton have I= 1/2 and I_3 = -1/2 ??
 
malawi_glenn said:
So does the anti-neutron have I = 1/2 and I_3 = 1/2
and anti-proton have I= 1/2 and I_3 = -1/2 ??

Sorry to raise a dead thread but I have the same question, I think that the answer is yes, but not sure. Can anyone confirm or disconfirm?

EDIT: Nevermind, it's yes.
 
Last edited:

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