- #1
Ian Lovejoy
- 7
- 0
Hi,
I'm reading Quantum Field Theory in a Nutshell by A. Zee, which is excellent but it is occasionally difficult to fill in the blanks on one's own.
Once such place is the integration of the Hopf term, which results from integrating out the gauge field in a Lagrangian with a Chern-Simons term in 2+1 dimensional spacetime.
The Hopf term is:
[tex]L_{Hopf}=\frac{1}{4\gamma}j_\mu(\frac{\epsilon^{\mu\nu\lambda}\partial_\nu}{\partial^2})j_\lambda[/tex]
From here we are supposed to be able to define a current j representing one particle at rest at the origin while another particle goes halfway around it. Integrating the above with this current we are supposed to obtain [tex]1/4\gamma[/tex]. This defines the fractional statistics of the particles in the system.
Except for a factor of 2 the same treatment appears in section II of this document:
http://arxiv.org/PS_cache/cond-mat/pdf/9501/9501022v2.pdf
It all seems perfectly straightforward but I'm unable to do the integration. For [tex]1/{\partial^2}[/tex] I am using:
[tex]\int{\frac{d^3k}{(2\pi)^3}\frac{-e^{ik(x - y)}}{k^2 + i\epsilon}}[/tex]
No matter what order I do the integration in, I seem to get either an integral that is impossible to do, or an result that is apparently zero. The book and the above reference seem to imply that the result is easily obtained by plugging in the current into the Lagrangian.
Can anyone give me a hint? It would be much appreciated.
Thanks,
Ian
I'm reading Quantum Field Theory in a Nutshell by A. Zee, which is excellent but it is occasionally difficult to fill in the blanks on one's own.
Once such place is the integration of the Hopf term, which results from integrating out the gauge field in a Lagrangian with a Chern-Simons term in 2+1 dimensional spacetime.
The Hopf term is:
[tex]L_{Hopf}=\frac{1}{4\gamma}j_\mu(\frac{\epsilon^{\mu\nu\lambda}\partial_\nu}{\partial^2})j_\lambda[/tex]
From here we are supposed to be able to define a current j representing one particle at rest at the origin while another particle goes halfway around it. Integrating the above with this current we are supposed to obtain [tex]1/4\gamma[/tex]. This defines the fractional statistics of the particles in the system.
Except for a factor of 2 the same treatment appears in section II of this document:
http://arxiv.org/PS_cache/cond-mat/pdf/9501/9501022v2.pdf
It all seems perfectly straightforward but I'm unable to do the integration. For [tex]1/{\partial^2}[/tex] I am using:
[tex]\int{\frac{d^3k}{(2\pi)^3}\frac{-e^{ik(x - y)}}{k^2 + i\epsilon}}[/tex]
No matter what order I do the integration in, I seem to get either an integral that is impossible to do, or an result that is apparently zero. The book and the above reference seem to imply that the result is easily obtained by plugging in the current into the Lagrangian.
Can anyone give me a hint? It would be much appreciated.
Thanks,
Ian