Abstract

In [8] we proposed the linear relations between the Weyl anomaly c1, c2, c3 coefficients and the 4 coefficients in the chiral anomaly polynomial for (1,0) superconformal 6d theories. These relations were determined up to one free parameter ξ and its value was then conjectured using some additional assumptions. A different value for ξ was recently suggested in arXiv:1702.03518 using an alternative method. Here we confirm that this latter value is indeed the correct one by providing an additional data point: the Weyl anomaly coefficient c3 for the higher derivative (1,0) superconformal 6d vector multiplet. This multiplet contains the 4-derivative conformal gauge vector, 3-derivative fermion and 2-derivative scalar. We find the corresponding value of c3 which is proportional to the coefficient CT in the 2-point function of stress tensor using its relation to the first derivative of the Renyi entropy or the second derivative of the free energy on the product of thermal circle and 5d hyperbolic space. We present some general results of the computation of the Rényi entropy and CT from the partition function on S1 × ℍd − 1 for higher derivative conformal scalars, spinors and vectors in even dimensions. We also give an independent derivation of the conformal anomaly coefficients of the 6d higher derivative vector multiplet from the Seeley-DeWitt coefficients on an Einstein background.

Highlights

  • General relationsWe shall use the latter definition of Sq in terms of the partition function or free energy on Sq1 × Hd−1 for even d

  • Stress tensor T T, c2 and c3 — from the 3-point function1 and the a-coefficient — from the 4-point function

  • In [8] we proposed the linear relations between the Weyl anomaly c1, c2, c3 coefficients and the 4 coefficients in the chiral anomaly polynomial for (1,0) superconformal 6d theories

Read more

Summary

General relations

We shall use the latter definition of Sq in terms of the partition function or free energy on Sq1 × Hd−1 for even d. For even d the free energy on Sq1 × Hd−1 does not contain logarithmic UV divergences while the non-universal power divergent part of Fq (which is proportional to the volume and is linear in q) should be subtracted using some regularization prescription. It was observed that for fields with gauge invariance S1 computed on Sq1 × Hd−1 is not automatically proportional to the Weyl anomaly a-coefficient (see [45, 46] for 4d vectors and [47] for 6d antisymmetric tensors), but one can achieve this by shifting.

Computational scheme
Scalar fields
Conformal vector fields
Fermionic fields
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call