Can Scalar and YM Lagrangians Be Written Using Tetrads and Spin Connection?

In summary, the lagrangian densities for a massless scalar field and a YM field can be written using tetrads and spin connection, with the former being L_{\phi} = e^{a} \wedge *(e_a \wedge d\phi) and the latter being L_{YM}=\left<e^{a}\wedge *F_{ab}\wedge e^b\right>.
  • #1
Dox
26
1
Hi everybody!

I'm studing some classical field theory in general backgrounds. Of course the most beautiful way of doing so is using differential forms. For example, the lagrangian density of a massless scalar field would be
[tex]L_{\phi}=d\phi\wedge * d\phi,[/tex]​
while the lagrangian density for a YM field is
[tex]L_{YM}=\left<d_A A\wedge *d_A A\right>. [/tex]​

However, once one is interested in adding spinors, tetrads (and spin connection) enter into action...
[tex]L_{\psi}=\epsilon_{abcd}\bar{\psi}\Gamma^a e^b e^c e^d (d+\omega)\psi,[/tex]​
with [tex]e^{a}[/tex] the tetrad 1-form and [tex]\omega[/tex]
the spin-connection 1-form.

Although all lagrangian densities are coordinate independent, they are written in different ways... Is there a form of writing the first two using tetrads and spin connection?

Thanks in advance!
 
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  • #2
</code>Yes, there is a way to write the first two lagrangian densities using tetrads and spin connection. The lagrangian density of a massless scalar field can be written as:L_{\phi} = e^{a} \wedge *(e_a \wedge d\phi)where e^{a} is the tetrad 1-form and * denotes the Hodge dual.The lagrangian density for a YM field can be written as:L_{YM}=\left<e^{a}\wedge *F_{ab}\wedge e^b\right>, where F_{ab} is the curvature 2-form associated with the spin connection 1-form, \omega. Hope this helps!
 
  • #3


Hello! It's great to see someone studying classical field theory in general backgrounds. You're right, using differential forms is a beautiful way to approach this topic. The lagrangian density you provided for a massless scalar field and a YM field are both excellent examples of this approach.

As for your question about adding spinors and tetrads into the equation, yes, they do introduce a bit more complexity. In this case, you can write the lagrangian density using tetrads and spin connection by using the vielbein formalism. This allows us to write the lagrangian in terms of the tetrad and spin connection 1-forms, as you have shown in your example for the spinor field.

Using the vielbein formalism, we can express all of the lagrangian densities in a unified way, making it easier to compare and analyze them. This approach is often used in the study of gravity and other theories involving spinors.

I hope this helps answer your question. Keep up the great work in your studies!
 

FAQ: Can Scalar and YM Lagrangians Be Written Using Tetrads and Spin Connection?

What is a field in general background?

A field in general background refers to a physical quantity that is present throughout a continuous region of space. It can be a scalar field, which has a single value at each point in space, or a vector field, which has both magnitude and direction at each point.

What are some examples of fields in general background?

Examples of fields in general background include electric fields, magnetic fields, gravitational fields, and temperature fields. These fields are present all around us and interact with matter to produce various effects.

What is the difference between a conservative and a non-conservative field?

A conservative field is one in which the work done by the field on a particle moving between two points is independent of the path taken between those points. In contrast, a non-conservative field depends on the path taken, and work done may vary depending on the path.

How are fields in general background measured and represented?

Fields in general background are measured using various instruments such as voltmeters, ammeters, and thermometers. They can also be represented graphically using field lines, which show the direction and strength of the field at each point.

How do fields in general background interact with matter?

Fields in general background interact with matter through forces. For example, electric fields interact with charged particles, magnetic fields interact with moving charged particles, and gravitational fields interact with masses. These interactions can cause particles to accelerate, change direction, or experience a force.

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