Abstract
Abstract
We introduce (generalised) Pfaffian operators into our lattice calculations of the mass spectra and confining string tensions of SO(2N) gauge theories, complementing the conventional trace operators used in previous lattice calculations. In SO(6) the corresponding ‘Pfaffian’ particles match the negative charge conjugation particles of SU(4), thus resolving a puzzle arising from the observation that SO(6) and SU(4) have the same Lie algebra. The same holds true (but much more trivially) for SO(2) and U(1). For SO(4) the Pfaffian particles are degenerate with, but orthogonal to, those obtained with the usual single trace operators. That is to say, there is a doubling of the spectrum, as one might expect given that the Lie algebra of SO(4) is the same as that of SU(2) × SU(2). Additional SO(8) and SO(10) calculations of the Pfaffian spectrum confirm the naive expectation that these masses increase with N, so that they cease to play a role in the physics of SO(N) gauge theories as N → ∞. We also calculate the energies of Pfaffian ‘strings’ in these gauge theories. Although all our lattice calculations are for gauge theories in D = 2 + 1, similar conclusions should hold for D = 3 + 1.
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
Reference26 articles.
1. R. Lau and M. Teper, SO(N) gauge theories in 2 + 1 dimensions: glueball spectra and confinement, JHEP
10 (2017) 022 [arXiv:1701.06941] [INSPIRE].
2. R. Lau and M. Teper, The deconfining phase transition of SO(N) gauge theories in 2 + 1 dimensions, JHEP
03 (2016) 072 [arXiv:1510.07841] [INSPIRE].
3. M. Teper, SO(4), SO(3) and SU(2) gauge theories in 2 + 1 dimensions: comparing glueball spectra and string tensions, arXiv:1801.05693 [INSPIRE].
4. A. Athenodorou and M. Teper, SU(N) gauge theories in 2 + 1 dimensions: glueball spectra and k-string tensions, JHEP
02 (2017) 015 [arXiv:1609.03873] [INSPIRE].
5. G. ’t Hooft, A Planar Diagram Theory for Strong Interactions, Nucl. Phys.
B 72 (1974) 461 [INSPIRE].