Counting BPS operators in gauge theories: quivers, syzygies and plethystics
By S. Benvenuti, Bo Feng, A. Hanany, Yang-Hui He. 2006
455 citations recorded by the source corpus.
We develop a systematic and efficient method of counting single-trace and multi-trace BPS operators with two supercharges, for world-volume gauge theories of $N$ D-brane probes for both $N \to \infty$ and finite $N$. The techniques are applicable to generic singularities, orbifold, toric, non-toric, complete intersections, et cetera, even to geometries whose precise field theory duals are not yet known. The so-called ``Plethystic Exponential'' provides a simple bridge between (1) the defining equation of the Calabi-Yau, (2) the generating function of single-trace BPS operators and (3) the generating function of multi-trace operators. Mathematically, fascinating and intricate inter-relations between gauge theory, algebraic geometry, combinatorics and number theory exhibit themselves in the form of plethystics and syzygies.
Subfields: Geometry and Topology, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/a64321ac6e1fafafd9738aa0ff16f98e5d077157
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Citations in the corpus
- THE MASTER SPACE OF N=1 GAUGE THEORIES (2008, methodology): “Because the dummy variable t keeps track of the charge, we can think of the components as chemical potentials [9, 12].”
- SQCD: A Geometric Apercu (2008, background): “14), the generating function can be easily computed from the knowledge that the modul space is a complete intersection (See [13] for a detailed discussion on this).”
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- Comments on twisted indices in 3d supersymmetric gauge theories (2016, background): “81) becomes the ‘Molien formula’ for the Higgs branch HS [35, 84]:”
- The Hilbert series of the one instanton moduli space (2010, background): “) instanton moduli space is therefore C2N=Z 2. One can see the last statement clearly from the Hilbert series. The Hilbert series { 19 { of C2N=Z 2 is given by the discrete Molien formula (see, e.g., [30]): g(t;x 1;:::;x N;C2N=Z 2) = 1 2 PE [1;0;:::;0] Sp(N)t + PE [1;0;:::;0] Sp(N)( t) = X1 k=0 [2k;”
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