RECORD
Dynamically Broken U(1) `Left' Gauge Theories in Four Dimensions
High Energy Physics - Theory · Submitted 20 Oct 1993
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The anomaly disappears and the gauge current is conserved.
The compiled record
The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
Open the compiled record
The abstract, sentence by sentence
We study a dynamically broken U(1) "left" gauge theory endowed with a composite scalar doublet (one scalar and one pseudoscalar); its Lagrangian only differs from that of an abelian `Standard Model' by the addition of a derivative coupling between a Wess-Zumino field, linked to the previous scalars, and the fermionic current. Yet, in the Feynman path integral, the non independence of the fermionic and scalar variables of integration requires the introduction of constraints. When the gauge symmetry is broken by the vacuum expectation value of the scalar field, they freeze all degrees of freedom but those of a massive gauge field, including a (abelian) pion. The anomaly disappears and the gauge current is conserved. This is shown, and renormalizability studied, in the `Nambu-Jona-Lasinio approximation'. Unitarity is demonstrated on general grounds.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study a dynamically broken U(1) "left" gauge theory endowed with a composite scalar doublet (one scalar and one pseudoscalar); its Lagrangian only differs from that of an abelian `Standard Model' by the addition of a derivative coupling between a Wess-Zumino field, linked to the previous scalars, and the fermionic current. | contribution 0.99 | 0.71 | 0.08 | asserted 0.98 |
| s1 | Yet, in the Feynman path integral, the non independence of the fermionic and scalar variables of integration requires the introduction of constraints. | method 0.68 | 0.57 | 0.04 | asserted 1.00 |
| s2 | When the gauge symmetry is broken by the vacuum expectation value of the scalar field, they freeze all degrees of freedom but those of a massive gauge field, including a (abelian) pion. | result 0.98 | 0.77 | 0.23 | asserted 1.00 |
| s3 | The anomaly disappears and the gauge current is conserved. | result 1.00 | 0.78 | 0.35 | asserted 1.00 |
| s4 | This is shown, and renormalizability studied, in the `Nambu-Jona-Lasinio approximation'. | method 0.91 | 0.88 | 0.10 | asserted 0.99 |
| s5 | Unitarity is demonstrated on general grounds. | result 0.74 | 0.86 | 0.11 | asserted 1.00 |
What was examined, and what was not
- arXiv listing abstract v1
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
The paper
Original abstract
We study a dynamically broken U(1) "left" gauge theory endowed with a composite scalar doublet (one scalar and one pseudoscalar); its Lagrangian only differs from that of an abelian `Standard Model' by the addition of a derivative coupling between a Wess-Zumino field, linked to the previous scalars, and the fermionic current. Yet, in the Feynman path integral, the non independence of the fermionic and scalar variables of integration requires the introduction of constraints. When the gauge symmetry is broken by the vacuum expectation value of the scalar field, they freeze all degrees of freedom but those of a massive gauge field, including a (abelian) pion. The anomaly disappears and the gauge current is conserved. This is shown, and renormalizability studied, in the `Nambu-Jona-Lasinio approximation'. Unitarity is demonstrated on general grounds.
Human review
Discussion
Know something about this paper? Leave a comment, or highlight any passage above to comment on it.