feat: Add Quarks#1328
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nateabr
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Overall everything looks great, just some comments on how we could make this approach standard for other particle fields.
I hope they help :)
| @[ext] | ||
| structure Quark where | ||
| /-- The underlying value of the quark field in the tensor product space. -/ | ||
| val : Fermion.LeftHandedWeyl ⊗[ℂ] EuclideanSpace ℂ (Fin 3) ⊗[ℂ] EuclideanSpace ℂ (Fin 2) |
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I'm assuming that we would add more fermions in successsive PR's, so would this being called Quark help with the naming?
Maybe LeftDoublet so if assume the namespace is Quark, the naming would be Quark.LeftDoublet ?
| one_smul := by intros; ext; simp [one_smul] | ||
| smul_zero := by intros; ext; simp [smul_zero] | ||
| zero_smul := by intros; ext; simp [zero_smul] | ||
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Regarding the above, would it be possible to define an equivalence between the Quark and its tensor product space? Something like valEquiv : Quark ≃ WrappedSpace.
Im thinking since the tensor product space already carries the necessary group and module structures, we can use Equiv.addCommGroup valEquiv and Equiv.module ℂ valEquiv to derive the group/module instances automatically.
This would then allow the valLinEquiv to be to be written with rfl proofs, maybe this approach might generalize when adding the other fermions.
| map_mul' := by intros; simp [map_mul]; rfl | ||
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| /-! | ||
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Maybe we could define repLorentzGroup with valLineEquiv , such that it can match the style of repGuageGroup .
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awaiting-author |
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t-particles |
Adding quarks to ./StandardModel, defining their representation under the Lorentz group and under the gauge group.