Abstract
In this paper using the Clifford bundle (\({\mathcal{C}\ell(M,\mathtt{g})}\)) and spin-Clifford bundle (\({\mathcal{C}\ell_{\mathrm{Spin}_{1,3}^{e}} (M,\mathtt{g})}\)) formalism, which allow to give a meaningful representative of a Dirac-Hestenes spinor field (even section of \({\mathcal{C}\ell_{\mathrm{Spin}_{1,3}^{e}}(M,\mathtt{g})}\)) in the Clifford bundle, we give a geometrical motivated definition for the Lie derivative of spinor fields in a Lorentzian structure (M, g) where M is a manifold such that dim M = 4, g is Lorentzian of signature (1, 3). Our Lie derivative, called the spinor Lie derivative (and denoted \({\overset{s}{\pounds}_{\boldsymbol{\xi}}}\)) is given by nice formulas when applied to Clifford and spinor fields, and moreover \({\overset{s}{\pounds }_{{\xi}}{\boldsymbol {g}}=0}\) for any vector field \({\boldsymbol {\xi}}\) . We compare our definitions and results with the many others appearing in literature on the subject.
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An erratum to this article is available at http://dx.doi.org/10.1007/s00006-015-0632-z.
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Leão, R.F., Rodrigues, W.A. & Wainer, S.A. Concept of Lie Derivative of Spinor Fields A Geometric Motivated Approach. Adv. Appl. Clifford Algebras 27, 209–227 (2017). https://doi.org/10.1007/s00006-015-0560-y
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DOI: https://doi.org/10.1007/s00006-015-0560-y