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Fermions in conformally invariant geometrodynamics
General Relativity and Quantum Cosmology · Submitted 11 Jun 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is proved that the fields can be interpreted as observed, generated by bispinor degrees of freedom.
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The abstract, sentence by sentence
Dynamic equations that are the simplest conformally invariant generalization of Einstein equations with cosmological term are considered. Dimensions and Weyl weights of the additional geometrical fields (the vector and the antisymmetric tensor) appearing in the scheme are such, that they admit an unexpected interpretation. It is proved that the fields can be interpreted as observed, generated by bispinor degrees of freedom. The vacuum polarization density matrix leads to different probabilities of different helicity particle generation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Dynamic equations that are the simplest conformally invariant generalization of Einstein equations with cosmological term are considered. | contribution 0.69 | 0.56 | 0.05 | asserted 0.80 |
| s1 | Dimensions and Weyl weights of the additional geometrical fields (the vector and the antisymmetric tensor) appearing in the scheme are such, that they admit an unexpected interpretation. | result 0.47 | 0.67 | 0.08 | asserted 0.99 |
| s2 | It is proved that the fields can be interpreted as observed, generated by bispinor degrees of freedom. | interpretation 0.61 | 0.88 | 0.70 | asserted 1.00 |
| s3 | The vacuum polarization density matrix leads to different probabilities of different helicity particle generation. | result 0.99 | 0.79 | 0.17 | asserted 0.99 |
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The paper
Original abstract
Dynamic equations that are the simplest conformally invariant generalization of Einstein equations with cosmological term are considered. Dimensions and Weyl weights of the additional geometrical fields (the vector and the antisymmetric tensor) appearing in the scheme are such, that they admit an unexpected interpretation. It is proved that the fields can be interpreted as observed, generated by bispinor degrees of freedom. The vacuum polarization density matrix leads to different probabilities of different helicity particle generation.
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