arXiv subjects

T. N. Sherry

Publications and source records attributed to T. N. Sherry.

22 records · Page 2Linked to original sources

arXiv2001

Spinors and Supersymmetry

In this paper, we survey the nature of spinors and supersymmetry (SUSY) in various types of spaces. We treat two distinct types of spaces: flat spaces and spaces of constant (non-zero) curvature. The flat spaces we consider are either three or four dimensional of signatures 3 + 1, 4 + 0, 2 + 2 and 3 + 0. In each of these cases, SUSY generators anti-commute to yield the generators of translations in the non-compact flat spaces. The spaces of constant curvature we consider are two-dimensional: the surface of the sphere S_2 and the Anti-deSitter space AdS_2. S_2 is embedded in a 3 + 0 Euclidean space while AdS_2 is embedded in 2 + 1 Minkowski space. The SUSY generators in these cases anti-commute to yield the generators of the isometry groups (SO(3) or SO(2,1)) of the space involved. We also report on some recent developments in looking for superspace realizations of these SUSY algebras. We can report good progress in the 3 + 0 Euclidean and in the AdS_2 case, somewhat less in the S_2 case. In each of the compact cases, we can construct field multiplet models carrying invariance under the full SUSY algebra.

hep-th↗

arXiv1998

Gauge Model With Extended Field Transformations in Euclidean Space

An SO(4) gauge invariant model with extended field transformations is examined in four dimensional Euclidean space. The gauge field is $(A^μ)^{αβ} = 1/2 t^{μνλ} (M^{νλ})^{αβ}$ where $M^{νλ}$ are the SO(4) generators in the fundamental representation. The SO(4) gauge indices also participate in the Euclidean space SO(4) transformations giving the extended field transformations. We provide the decomposition of the reducible field $t^{μνλ}$ in terms of fields irreducible under SO(4). The SO(4) gauge transformations for the irreducible fields mix fields of different spin. Reducible matter fields are introduced in the form of a Dirac field in the fundamental representation of the gauge group and its decomposition in terms of irreducible fields is also provided. The approach is shown to be applicable also to SO(5) gauge models in five dimensional Euclidean space.

hep-th↗

arXiv1998

Aspects of the Supersymmetry Algebra in Four Dimensional Euclidean Space

The simplest supersymmetry (SUSY) algebra in four dimensional Euclidean space ($4dE$) has been shown to closely resemble the $N = 2$ SUSY algebra in four dimensional Minkowski space ($4dM$). The structure of the former algebra is examined in greater detail in this paper. We first present its Clifford algebra structure. This algebra shows that the momentum Casimir invariant of physical states has an upper bound which is fixed by the central charges. Secondly, we use reduction of the $N = 1$ SUSY algebra in six dimensional Minkowski space ($6dM$) to $4dE$; this reproduces our SUSY algebra in $4dE$. Moreover, this same reduction of supersymmetric Yang-Mills theory (SSYM) in $6dM$ reproduces Zumino's SSYM in $4dE$. We demonstrate how this dimensional reduction can be used to introduce additional generators into the SUSY algebra in $4dE$.

hep-th↗

arXiv1996

Gauge Dependence in Chern-Simons Theory

We compute the contribution to the modulus of the one-loop effective action in pure non-Abelian Chern-Simons theory in an arbitrary covariant gauge. We find that the results are dependent on both the gauge parameter ($α$) and the metric required in the gauge fixing. A contribution arises that has not been previously encountered; it is of the form $(α/ \sqrt{p^2}) ε_{μλν} p^λ$. This is possible as in three dimensions $α$ is dimensionful. A variant of proper time regularization is used to render these integrals well behaved (although no divergences occur when the regularization is turned off at the end of the calculation). Since the original Lagrangian is unaltered in this approach, no symmetries of the classical theory are explicitly broken and $ε_{μλν}$ is handled unambiguously since the system is three dimensional at all stages of the calculation. The results are shown to be consistent with the so-called Nielsen identities which predict the explicit gauge parameter dependence using an extension of BRS symmetry. We demonstrate that this $α$ dependence may potentially contribute to the vacuum expectation values of products of Wilson loops.

hep-th↗