- #1
saadhusayn
- 22
- 1
- Homework Statement
- I'm trying to derive the effective action at two loops for the quartic vertices from the attached paper. For quartic vertices, e.g. $$-\frac{g}{2}\epsilon^{abx}\epsilon^{cdx} A_{a} Y^{i}_{b}A_{c}Y^{i}_{d} \tag{5.6}.$$
According to the paper,the explicit expressions for quartic vertices are given by
$$ \int \lambda_{4} \Delta_{1}(\tau, \tau | m_{1}) \Delta_{2}(\tau, \tau | m_{2}) \text{ }(5.1)$$
Here, $$\lambda_{4}$$ is a quartic vertex and the $$\Delta_{i}$$s are propagators with masses $$m_{i}$$.
[1]: https://arxiv.org/abs/hep-th/9705091
- Relevant Equations
- The Feynman diagrams are given in figure 1 in the paper.
Does this mean that the expression for the above vertex is
$$ -\frac{g}{2}\epsilon^{abx}\epsilon^{cdx}\int d\tau \langle A_{a} (\tau) A_{c} (\tau)\rangle \langle Y^{i}_{b} (\tau)Y^{i}_{d}(\tau) \rangle $$
$$ -\frac{g}{2}\epsilon^{abx}\epsilon^{cdx}\int d\tau \langle A_{a} (\tau) A_{c} (\tau)\rangle \langle Y^{i}_{b} (\tau)Y^{i}_{d}(\tau) \rangle $$