Quanta of massive vector fields

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Discussion Overview

The discussion revolves around the nature of massive vector fields, specifically focusing on the W+, W-, and Z0 bosons as field quanta. Participants explore concepts related to Proca fields, gauge fields, and the relationships between these particles in the context of electroweak interactions and nuclear physics.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants assert that W+, W-, and Z0 bosons are examples of massive vector fields, specifically Proca fields.
  • Others clarify that while W and Z bosons are massive gauge fields, the Z0 boson is not charged.
  • One participant mentions that Proca fields are not unique and can describe various massive spin-1 bosons, including the rho meson.
  • There is a contention regarding the classification of hadrons as fundamental particles, with some arguing that hadrons are not fundamental.
  • Participants discuss the possibility of expressing the Z0 field as a linear combination of W+ and W- fields, with conflicting views on this point.
  • One participant argues that the Z boson is distinct and not a linear combination of the charged W bosons.
  • Confusion arises regarding the description of pions in nuclear physics, with references to complex scalar fields and the neutral pion's representation.
  • Another participant corrects misconceptions about the relationship between neutral and charged pions, emphasizing their independence in field representation.

Areas of Agreement / Disagreement

Participants express differing views on the relationships between the Z0 boson and the W bosons, as well as the nature of pions in nuclear physics. The discussion remains unresolved with multiple competing perspectives on these topics.

Contextual Notes

There are limitations in the discussion regarding the definitions of "fundamental" particles and the assumptions made about the relationships between various fields and particles. Some mathematical representations and relationships remain unresolved.

quantumfireball
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Are the W+,W- and Z0 the field quanta of the massive charged vector fields?
ie Proca fields
 
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They are massive and they are gauge fields (electroweak force). but the Z0 is not charged.
 
"Proca" fields are massive, spin-1 bosons. These objects are not unique. W and Z bosons are examples of these things. So is the rho meson in hadron physics. They are each their own separate Proca field.
 
but hadrons are not fundamental
but thanks for clearing the doubt regarding w bosons
 
what does "fundamental" have to do with anything?
 
olgranpappy said:
They are massive and they are gauge fields (electroweak force). but the Z0 is not charged.


yes but Z0 field can be written as a linear combination of W+ and W- fields
like in scalar fields right?to get a real valued field
 
what I mean by my above post is that "Proca" has nothing to do with "fundamental" - it's just the Lagrangian for a massive, spin-1 particle. The deuteron, for example, can be described by a proca field, as long as you're not interested in the substructure of the deuteron (ex: problems in atomic or molecular physics)!
 
quantumfireball said:
yes but Z0 field can be written as a linear combination of W+ and W- fields
like in scalar fields right?to get a real valued field

NO! The Z boson is NOT a linear combination of the charged W bosons! It is its own thing.
 
  • #10
wait a minute this is getting a bit confusing in nuclear physics the pions are described by complex scalar fields and over there the neutral pion is decribed by the field 1/2*(phi+phi*),i think i read this in JJ Sakurai advanced QM
Plz confirm
 
  • #11
quantumfireball said:
wait a minute this is getting a bit confusing in nuclear physics the pions are described by complex scalar fields and over there the neutral pion is decribed by the field 1/2*(phi+phi*),i think i read this in JJ Sakurai advanced QM
Plz confirm

You are mis-informed! The neutral pion is not related to the charged pions - it is a linearly independent scalar field.

I think you're getting confused with the following: the 3 pions form an isospin-1 field (3 components), call them [itex]\pi_1,\pi_2,\pi_3[/itex]. now you can write:

[tex]\pi^{\pm}=\frac{1}{\sqrt{2}}(\pi_1\pm i\pi_2)[/tex]

while [itex]\pi^0 = \pi_3[/itex]. Here the sign corresponds to the charge.

Now for the W bosons, you can also write [itex]W^\pm\propto(W_1\pm iW_2)[/itex] while the Z-boson is related to [itex]W_3[/itex], although the Z boson also has hypercharge so it's more complicated than the [itex]\pi^0[/itex].

Does that help?
 
  • #12
Also, in the quark model, remember that the charged pions are (u-dbar) and (d-ubar), while the neutral pion is (u-ubar)+(d-dbar) - so these are not the same thing!
 
  • #13
thanks a lot belchman
i know i was a confused
 

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