Can Left Handed Up Quarks Transform Into Right Handed Ones?

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The discussion centers on the possibility of left-handed up quarks transforming into right-handed ones, suggesting that such transformations require additional bosons and a proper formulation within the standard model Lagrangian. Participants explore the role of the Higgs field in facilitating these transformations, drawing parallels to how left-handed electrons can become right-handed through Higgs coupling. The conversation emphasizes the importance of gauge symmetries in these transformations, highlighting that one component must be conjugated to maintain these symmetries. The interaction between the Higgs and the electroweak fields is compared to the quark transformations, illustrating the complexity of mass generation in particle physics. Overall, the dialogue delves into the intricate relationships between particle properties and the mechanisms of symmetry breaking in the standard model.
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Homework Statement
Can Left Handed Up Quarks Transform Into Right Handed Ones?
Relevant Equations
u(i) = 1/2
Isospin must be transformable if it is the case. In which case there must be additional Bosons for doing the transformation.
 
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Can you write down a term in the standard model lagrangian where you have ##\bar u_R## and ##u_L##?
 
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It's uR and uL.

No, but I can write down a formula containing a new particle, with the particle's properties (for the case of an electron, not u-quark).
 
talanum52 said:
It's uR and uL.

No, but I can write down a formula containing a new particle, with the particle's properties (for the case of an electron, not u-quark).
Hint: Look at the Higgs sector.

-Dan
 
topsquark said:
Hint: Look at the Higgs sector.

-Dan
Doesn't, for example, a left-handed electron change into a right-handed one by coupling to the Higgs field? Which is why the neutrino has no Higgs-induced mass?

So, a left-handed quark can change into a right-handed one indeed?
 
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talanum52 said:
It's uR and uL.
You need a bar above one of them to preserve gauge symmetries...
 
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malawi_glenn said:
You need a bar above one of them to preserve gauge symmetries...
I thought the same. Loosely speaking, before the SU(2)LxU(1)Y symmetry is broken, Higgs couples the ##\phi _l## and ##\bar{\phi} _r##: ##\bar{\phi} _l h {\phi} _r##. When the symmetry is broken this becomes ##m\bar{\phi} \phi##, where the ##\phi##'s are superpositions of l and r.

It's comparable to the Higgs interacting with the three W's and B of the unbroken electroweak field. After this interaction, the interaction vertex term becomes a mass term, the Z0 and W+/- being superpositions of the three W's and B (like the l and r in the previous paragraph).
 
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