Bose-Fermi Degeneracies in Large Adjoint QCD
arXiv:1409.1617 · doi:http://dx.doi.org/10.1007/JHEP07(2015)016
Abstract
We analyze the large limit of adjoint QCD, an gauge theory with flavors of massless adjoint Majorana fermions, compactified on . We focus on the weakly-coupled confining small- regime. If the fermions are given periodic boundary conditions on , we show that there are large cancellations between bosonic and fermionic contributions to the twisted partition function. These cancellations follow a pattern previously seen in the context of misaligned supersymmetry, and lead to the absence of Hagedorn instabilities for any size , even though the bosonic and fermionic densities of states both have Hagedorn growth. Adjoint QCD stays in the confining phase for any , explaining how it is able to enjoy large volume independence for any . The large boson-fermion cancellations take place in a setting where adjoint QCD is manifestly non-supersymmetric at any finite , and are consistent with the recent conjecture that adjoint QCD has emergent fermionic symmetries in the large limit.
35 pages, 5 figures. v3: further minor corrections
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