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More on the Tensorial Central Charges in N=1 Supersymmetric Gauge Theories (BPS Wall Junctions and Strings)

A. Gorsky, M. Shifman

TL;DR

The paper analyzes tensorial central charges in ${\cal N}=1$ supersymmetric gauge theories for solitons with axial geometry (strings and wall junctions) and derives a general expression for the central extension $Z_\mu$. It shows that, at weak coupling, BPS strings exist only in SQED with a Fayet–Iliopoulos term, while the $(1/2,1/2)$ central charge receives ambiguous matter contributions that do not affect the string tension; in non-Abelian theories these strings cannot saturate at weak coupling. The discussion extends to ${\cal N}=2$ theories, where strong-coupling BPS strings may arise on Coulomb or Higgs branches, with a brane picture offering geometric interpretations (D2 between NS5s for FI strings and M2 between M5s in M-theory). The work also highlights a precise interplay between ambiguities in the $(1/2,1/2)$ and $(1,0)$ charges that yields unambiguous wall-junction tensions, and it connects these results to two-dimensional sigma-model instantons and brane constructions. Overall, the paper clarifies when BPS axial objects can exist in ${\cal N}=1$ and ${\cal N}=2$ gauge theories and how brane realizations illuminate their central charges and saturations.

Abstract

We study the central extensions of the N=1 superalgebras relevant to the soliton solutions with the axial geometry - strings, wall junctions, etc. A general expression valid in any four-dimensional gauge theory is obtained. We prove that the only gauge theory admitting BPS strings at weak coupling is supersymmetric electrodynamics with the Fayet-Iliopoulos term. The problem of ambiguity of the (1/2,1/2) central charge in the generalized Wess-Zumino models and gauge theories with matter is addressed and solved. A possibility of existence of the BPS strings at strong coupling in N=2 theories is discussed. A representation of different strings within the brane picture is presented.

More on the Tensorial Central Charges in N=1 Supersymmetric Gauge Theories (BPS Wall Junctions and Strings)

TL;DR

The paper analyzes tensorial central charges in supersymmetric gauge theories for solitons with axial geometry (strings and wall junctions) and derives a general expression for the central extension . It shows that, at weak coupling, BPS strings exist only in SQED with a Fayet–Iliopoulos term, while the central charge receives ambiguous matter contributions that do not affect the string tension; in non-Abelian theories these strings cannot saturate at weak coupling. The discussion extends to theories, where strong-coupling BPS strings may arise on Coulomb or Higgs branches, with a brane picture offering geometric interpretations (D2 between NS5s for FI strings and M2 between M5s in M-theory). The work also highlights a precise interplay between ambiguities in the and charges that yields unambiguous wall-junction tensions, and it connects these results to two-dimensional sigma-model instantons and brane constructions. Overall, the paper clarifies when BPS axial objects can exist in and gauge theories and how brane realizations illuminate their central charges and saturations.

Abstract

We study the central extensions of the N=1 superalgebras relevant to the soliton solutions with the axial geometry - strings, wall junctions, etc. A general expression valid in any four-dimensional gauge theory is obtained. We prove that the only gauge theory admitting BPS strings at weak coupling is supersymmetric electrodynamics with the Fayet-Iliopoulos term. The problem of ambiguity of the (1/2,1/2) central charge in the generalized Wess-Zumino models and gauge theories with matter is addressed and solved. A possibility of existence of the BPS strings at strong coupling in N=2 theories is discussed. A representation of different strings within the brane picture is presented.

Paper Structure

This paper contains 16 sections, 78 equations, 2 figures.

Figures (2)

  • Figure 1: The integration contour in the $x,\, y$ plane. The soliton axis (the closed circle) lies perpendicular to this plane.
  • Figure 2: The domain wall junction in the theory with $Z_N$ symmetry. The "hub" is denoted by the closed circle.