Lorentz transformation and its Noether current

[Ken Gallock]

Hi.
I'd like to ask about the calculation of Noether current.
On page16 of David Tong's lecture note(http://www.damtp.cam.ac.uk/user/tong/qft.html), there is a topic about Noether current and Lorentz transformation.
I want to derive ##\delta \mathcal{L}##, but during my calculation, I encountered this:
\begin{align}
\delta \mathcal{L}&=\dfrac{\partial \mathcal{L}}{\partial \phi}\delta \phi+\dfrac{\partial \mathcal{L}}{\partial(\partial_\mu \phi)}\partial_\mu (\delta \phi)\\
&=\dfrac{\partial \mathcal{L}}{\partial \phi}(-\omega^\rho_{~\sigma}x^\sigma \partial_\rho \phi)+
\dfrac{\partial \mathcal{L}}{\partial(\partial_\mu \phi)}\partial_\mu
(-\omega^\rho_{~\sigma}x^\sigma \partial_\rho \phi).
\end{align}
The second term,
$$
\partial_\mu(-\omega^\rho_{~\sigma}x^\sigma \partial_\rho \phi)
$$
is a troubling term for me. Since there is ##x^\sigma## and ##\partial_\mu##, I thought I have to derivate ##x^\sigma## like ##\partial_\mu x^\sigma##. But if I do so, it doesn't match with the result in the textbook.
Am I supposed not to derivate ##x##? or am I missing something?

Thanks.

 

[Orodruin]

Exactly which equation are you trying to reproduce?

 

[Ken Gallock]

Exactly which equation are you trying to reproduce?

I want eq(1.53):
$$
\delta \mathcal{L}=-\omega^\mu_{~\nu}x^\nu\partial_\mu \mathcal{L}.
$$

 

[Orodruin]

I want eq(1.53):
$$
\delta \mathcal{L}=-\omega^\mu_{~\nu}x^\nu\partial_\mu \mathcal{L}.
$$

This is a direct consequence of the Lagrangian being a scalar field.

 

[Ken Gallock]

This is a direct consequence of the Lagrangian being a scalar field.

Is it different when I'm dealing with spinor fields?

 

[samalkhaiat]

Hi.
I'd like to ask about the calculation of Noether current.
...
But if I do so, it doesn't match with the result in the textbook.
Thanks.

You get the same result, if you differentiate and remember to use the fact that your field is a scalar and [itex]\omega_{\mu\nu} = -\omega_{\nu\mu}[/itex]:
[tex]-\delta \mathcal{L} = \frac{\partial \mathcal{L}}{\partial \phi} \left(\omega^{\rho}{}_{\sigma} x^{\sigma} \ \partial_{\rho}\phi \right) + \frac{\partial \mathcal{L}}{\partial (\partial_{\mu} \phi ) } \left( \omega^{\rho}{}_{\sigma}x^{\sigma} \ \partial_{\rho} \partial_{\mu} \phi + \partial^{\rho}\phi \ \omega_{\rho \mu}\right) .[/tex] Arrange the terms to get [tex]\delta \mathcal{L} = - \omega^{\rho}{}_{\sigma} x^{\sigma} \ \partial_{\rho}\mathcal{L} - \omega_{\rho \mu} \ \partial^{\rho} \phi \ \frac{\partial \mathcal{L}}{\partial (\partial_{\mu}\phi )} .[/tex] Now, for a scalar field, you have [tex]\omega_{\rho \mu} \ \partial^{\rho} \phi \ \frac{\partial \mathcal{L}}{\partial (\partial_{\mu}\phi )} \propto \omega_{\rho \mu} \ \partial^{\rho} \phi \ \partial^{\mu}\phi = 0 ,[/tex] because of the [itex]\omega_{\rho \mu} = - \omega_{\mu\rho}[/itex]. So, you are left with [tex]\delta \mathcal{L} = - \omega^{\rho}{}_{\sigma} x^{\sigma} \ \partial_{\rho}\mathcal{L} = - \omega^{\rho}{}_{\sigma} \ \partial_{\rho} \left( x^{\sigma} \mathcal{L}\right) .[/tex]

Is it different when I'm dealing with spinor fields?

The Lagrangian will still be scalar, but the transformation of the (spinor) field will no longer be [itex]\delta \psi = -\omega^{\mu}{}_{\nu}x^{\nu}\partial_{\mu}\psi .[/itex] You have to account for the spin of the field by including an appropriate spin matrix [itex]\Sigma[/itex]: [tex] \delta \psi_{a} = -\omega^{\mu}{}_{\nu}x^{\nu}\ \partial_{\mu}\psi_{a} + \omega_{\rho \sigma} (\Sigma^{\rho\sigma})_{a}{}^{c} \ \psi_{c} .[/tex]

 

[Ken Gallock]

You get the same result, if you differentiate and remember to use the fact that your field is a scalar and [itex]\omega_{\mu\nu} = -\omega_{\nu\mu}[/itex]:
[tex]-\delta \mathcal{L} = \frac{\partial \mathcal{L}}{\partial \phi} \left(\omega^{\rho}{}_{\sigma} x^{\sigma} \ \partial_{\rho}\phi \right) + \frac{\partial \mathcal{L}}{\partial (\partial_{\mu} \phi ) } \left( \omega^{\rho}{}_{\sigma}x^{\sigma} \ \partial_{\rho} \partial_{\mu} \phi + \partial^{\rho}\phi \ \omega_{\rho \mu}\right) .[/tex] Arrange the terms to get [tex]\delta \mathcal{L} = - \omega^{\rho}{}_{\sigma} x^{\sigma} \ \partial_{\rho}\mathcal{L} - \omega_{\rho \mu} \ \partial^{\rho} \phi \ \frac{\partial \mathcal{L}}{\partial (\partial_{\mu}\phi )} .[/tex] Now, for a scalar field, you have [tex]\omega_{\rho \mu} \ \partial^{\rho} \phi \ \frac{\partial \mathcal{L}}{\partial (\partial_{\mu}\phi )} \propto \omega_{\rho \mu} \ \partial^{\rho} \phi \ \partial^{\mu}\phi = 0 ,[/tex] because of the [itex]\omega_{\rho \mu} = - \omega_{\mu\rho}[/itex]. So, you are left with [tex]\delta \mathcal{L} = - \omega^{\rho}{}_{\sigma} x^{\sigma} \ \partial_{\rho}\mathcal{L} = - \omega^{\rho}{}_{\sigma} \ \partial_{\rho} \left( x^{\sigma} \mathcal{L}\right) .[/tex]
The Lagrangian will still be scalar, but the transformation of the (spinor) field will no longer be [itex]\delta \psi = -\omega^{\mu}{}_{\nu}x^{\nu}\partial_{\mu}\psi .[/itex] You have to account for the spin of the field by including an appropriate spin matrix [itex]\Sigma[/itex]: [tex] \delta \psi_{a} = -\omega^{\mu}{}_{\nu}x^{\nu}\ \partial_{\mu}\psi_{a} + \omega_{\rho \sigma} (\Sigma^{\rho\sigma})_{a}{}^{c} \ \psi_{c} .[/tex]

Thanks!
I got the same result!