English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Tools annual

Global: Zendy Free Plan

Global: Zendy Tools monthly

Global: Zendy Plus monthly

We exploit the power and potential of the (anti-)chiral superfield approach(ACSA) to Becchi-Rouet-Stora-Tyutin (BRST) formalism to derive the nilpotent(anti-)BRST symmetry transformations for any arbitrary D-dimensionalinteracting non-Abelian 1-form gauge theory where there is a SU(N) gaugeinvariant coupling between the gauge field and the Dirac fields. We derive theconserved and nilpotent (anti-)BRST charges and establish their nilpotency andabsolute anticommutativity properties within the framework of ACSA to BRSTformalism. The clinching proof of the absolute anticommutativity property ofthe conserved and nilpotent (anti-)BRST charges is a novel result in view ofthe fact that we consider, in our present endeavor, only the (anti-)chiralsuper expansions of the superfields that are defined on the (D, 1)-dimensionalsuper-submanifolds of the general (D, 2)-dimensional supermanifold on which ourD-dimensional ordinary interacting non-Abelian 1-form gauge theory isgeneralized. To corroborate the novelty of the above result, we apply the ACSAto an N = 2 supersymmetric (SUSY) quantum mechanical (QM) model of a harmonicoscillator and show that the nilpotent and conserved N = 2 supercharges of thissystem do not absolutely anticommute.

Nilpotent Charges in an Interacting Gauge Theory and an N = 2 SUSY Quantum Mechanical Model: (Anti-)Chiral Superfield Approach