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On energy-momentum and spin/helicity of quark and gluon fields
General Relativity and Quantum Cosmology · Submitted 2 Feb 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim (iv) Within the viable EC-theory, our theses (i) and (ii) are fulfilled and, thus, we favor this gravitational theory.
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The abstract, sentence by sentence
In special relativity, quantum matter can be classified according to mass-energy and spin. The corresponding field-theoretical notions are the energy-momentum-stress tensor T and the spin angular momentum tensor S. Since each object in physics carries energy and, if fermionic, also spin, the notions of T and S can be spotted in all domains of physics. We discuss the T and S currents in Special Relativity (SR), in General Relativity (GR), and in the Einstein-Cartan theory of gravity (EC). We collect our results in 4 theses: (i) The quark energy-momentum and the quark spin are described correctly by the canonical (Noether) currents T and S, respectively. (ii) The gluon energy-momentum current is described correctly by the (symmetric and gauge invariant) Minkowski type current. Its (Lorentz) spin current vanishes, S = 0. However, it carries helicity of plus or minus one. (iii) GR contradicts thesis (i), but is compatible with thesis (ii). (iv) Within the viable EC-theory, our theses (i) and (ii) are fulfilled and, thus, we favor this gravitational theory.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In special relativity, quantum matter can be classified according to mass-energy and spin. | background 1.00 | 0.03 | 0.02 | asserted 0.96 |
| s1 | The corresponding field-theoretical notions are the energy-momentum-stress tensor T and the spin angular momentum tensor S. | background 1.00 | 0.06 | 0.02 | asserted 1.00 |
| s2 | Since each object in physics carries energy and, if fermionic, also spin, the notions of T and S can be spotted in all domains of physics. | background 1.00 | 0.04 | 0.02 | asserted 0.97 |
| s3 | We discuss the T and S currents in Special Relativity (SR), in General Relativity (GR), and in the Einstein-Cartan theory of gravity (EC). | contribution 0.93 | 0.63 | 0.03 | asserted 0.89 |
| s4 | We collect our results in 4 theses: (i) The quark energy-momentum and the quark spin are described correctly by the canonical (Noether) currents T and S, respectively. | result 0.96 | 0.78 | 0.30 | asserted 1.00 |
| s5 | (ii) The gluon energy-momentum current is described correctly by the (symmetric and gauge invariant) Minkowski type current. | result 1.00 | 0.77 | 0.21 | asserted 1.00 |
| s6 | Its (Lorentz) spin current vanishes, S = 0. | result 1.00 | 0.60 | 0.07 | asserted 1.00 |
| s7 | However, it carries helicity of plus or minus one. | result 0.98 | 0.57 | 0.08 | asserted 1.00 |
| s8 | (iii) GR contradicts thesis (i), but is compatible with thesis (ii). | result 0.91 | 0.57 | 0.13 | asserted 1.00 |
| s9 | (iv) Within the viable EC-theory, our theses (i) and (ii) are fulfilled and, thus, we favor this gravitational theory. | interpretation 0.87 | 0.74 | 0.79 | asserted 0.71 |
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The paper
Original abstract
In special relativity, quantum matter can be classified according to mass-energy and spin. The corresponding field-theoretical notions are the energy-momentum-stress tensor T and the spin angular momentum tensor S. Since each object in physics carries energy and, if fermionic, also spin, the notions of T and S can be spotted in all domains of physics. We discuss the T and S currents in Special Relativity (SR), in General Relativity (GR), and in the Einstein-Cartan theory of gravity (EC). We collect our results in 4 theses: (i) The quark energy-momentum and the quark spin are described correctly by the canonical (Noether) currents T and S, respectively. (ii) The gluon energy-momentum current is described correctly by the (symmetric and gauge invariant) Minkowski type current. Its (Lorentz) spin current vanishes, S = 0. However, it carries helicity of plus or minus one. (iii) GR contradicts thesis (i), but is compatible with thesis (ii). (iv) Within the viable EC-theory, our theses (i) and (ii) are fulfilled and, thus, we favor this gravitational theory.
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How the literature uses it
9 arXiv papers cite this in 15 sentences
Papers citing it · 13 sentences without a confident label
Cites it as background 2 papers
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The affine connection $Γ^ k_i j$ in the ECSK theory of gravity is not symmetric and has the antisymmetric part, the torsion tensor $S^k_kij=(Γ^ k_i j-Γ^ k_j i)/2$ [ref] .
Universe in a black hole in Einstein$-$Cartan gravity · Einstein-Cartan-Sciama-Kibble theory of gravity · 0.99
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In relativistic theories with spinful matter there are two possible definitions of the stress-energy tensor [ref] .
Physical stress, mass, and energy for non-relativistic matter · Introduction · 0.97
What it cites · 11 sentences without a confident label
Cites as background 3 papers
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A short outline and the classical papers of the subject can be found in Blagojević and Hehl [ref] , see also the review paper [ref] .
On the Gauge Aspects of Gravity · Introduction · 0.99
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Recently, in this context, the problem has been addressed of the appropriate energy-momentum and spin tensors of quark and gluon fields, see the review paper of Leader and Lorcé [ref] .
The angular momentum controversy: What's it all about and does it matter? · Introduction · 0.99
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On the gravitational side, there took some developments place that are not without implications for the understanding of the energy-momentum and the spin distribution of matter fields, see also the thermodynamic considerations of Becattini & Tinti [ref] .
Thermodynamical inequivalence of quantum stress-energy and spin tensors · Introduction · 0.88
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