2016/09/30 by Jordan François, Jérémy Attard, Jeremy Attard · 16 citations
Mathematics · Physics and Astronomy · #BRST quantization #Black Holes and Theoretical Physics #Conformal map #Cosmology and Gravitation Theories #Covariant transformation #Differential form #Differential geometry #Gauge anomaly #Gauge covariant derivative #Gauge symmetry #Gauge theory #Geometry #Mathematical physics #Mathematics #Noncommutative and Quantum Gravity Theories #Physics #Supersymmetric gauge theory #Symmetry (geometry) #Theoretical physics #math-ph #math.MP
paper · pdf · doi:10.1088/1361-6382/aa627d
published in Classical and Quantum Gravity 34(8), 085004 (IOP Publishing) · 29 pages, minor typos corrected
openalex created_date 2016/10/07 · arxiv created 2016/11/04 · openalex publication_date 2017/03/21 · arxiv updated 2017/03/29 · openalex updated_date 2026/08/05
Abstract Tractor and Twistor bundles provide natural conformally covariant calculi on 4D-Riemannian manifolds. They have different origins but are closely related, and usually constructed bottom–up through prolongation of defining differential equations. We propose alternative top–down gauge theoretic constructions, starting from the conformal Cartan bundle <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mstyle displaystyle="false"> <mml:mrow> <mml:mrow> <mml:mi mathvariant="script">P</mml:mi> </mml:mrow> </mml:mrow> </mml:mstyle> </mml:math> and its vectorial E and spinorial <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mstyle displaystyle="false"> <mml:mrow> <mml:mrow> <mml:mtext mathvariant="sans-serif">E</mml:mtext> </mml:mrow> </mml:mrow> </mml:mstyle> </mml:math> associated bundles. Our key ingredient is the dressing field method of gauge symmetry reduction, which allows tractors and twistors and their associated connections to exhibit as gauge fields of a non-standard kind as far as Weyl rescaling transformation is concerned. By non-standard we mean that they implement the gauge principle of physics, but are of a different geometric nature than the well-known differential geometric objects usually underlying gauge theories. We provide the corresponding BRST treatment. In a companion paper we dealt with tractors, in the present one we address the case of twistors.