Jet Bundle Geometry of Scalar Field Theories
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arXiv
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| Format: | Preprint |
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2023
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| _version_ | 1866909343557877760 |
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| author | Alminawi, Mohammad Brivio, Ilaria Davighi, Joe |
| author_facet | Alminawi, Mohammad Brivio, Ilaria Davighi, Joe |
| contents | For scalar field theories, such as those EFTs describing the Higgs, it is well-known that the 2-derivative Lagrangian is captured by geometry. That is, the set of operators with exactly 2 derivatives can be obtained by pulling back a metric from a field space manifold $M$ to spacetime $Σ$. We here generalise this geometric understanding of scalar field theories to higher- (and lower-) derivative Lagrangians. We show how the entire EFT Lagrangian with up to 4-derivatives can be obtained from geometry by pulling back a metric to $Σ$ from the 1-jet bundle that is (roughly) associated with maps from $Σ$ to $M$. More precisely, our starting point is to trade the field space $M$ for a fibre bundle $π:E \to Σ$, with fibre $M$, of which the scalar field $ϕ$ is a local section. We discuss symmetries and field redefinitions in this bundle formalism, before showing how everything can be `prolongated' to the 1-jet bundle $J^1 E$ which, as a manifold, is the space of sections $ϕ$ that agree in their zeroth and first derivatives above each spacetime point. Equipped with a notion of (spacetime and internal) symmetry on $J^1 E$, the idea is that one can write down the most general metric on $J^1 E$ consistent with symmetries, in the spirit of the effective field theorist, and pull it back to spacetime to build an invariant Lagrangian; because $J^1 E$ has `derivative coordinates', one naturally obtains operators with more than 2-derivatives from this geometry. We apply this formalism to various examples, including a single real scalar in 4d and a quartet of real scalars with $O(4)$ symmetry that describes the Higgs EFTs. We show how an entire non-redundant basis of 0-, 2-, and 4-derivative operators is obtained from jet bundle geometry in this way. Finally, we study the connection to amplitudes and the role of geometric invariants. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2308_00017 |
| institution | arXiv |
| publishDate | 2023 |
| record_format | arxiv |
| spellingShingle | Jet Bundle Geometry of Scalar Field Theories Alminawi, Mohammad Brivio, Ilaria Davighi, Joe High Energy Physics - Phenomenology High Energy Physics - Theory Mathematical Physics For scalar field theories, such as those EFTs describing the Higgs, it is well-known that the 2-derivative Lagrangian is captured by geometry. That is, the set of operators with exactly 2 derivatives can be obtained by pulling back a metric from a field space manifold $M$ to spacetime $Σ$. We here generalise this geometric understanding of scalar field theories to higher- (and lower-) derivative Lagrangians. We show how the entire EFT Lagrangian with up to 4-derivatives can be obtained from geometry by pulling back a metric to $Σ$ from the 1-jet bundle that is (roughly) associated with maps from $Σ$ to $M$. More precisely, our starting point is to trade the field space $M$ for a fibre bundle $π:E \to Σ$, with fibre $M$, of which the scalar field $ϕ$ is a local section. We discuss symmetries and field redefinitions in this bundle formalism, before showing how everything can be `prolongated' to the 1-jet bundle $J^1 E$ which, as a manifold, is the space of sections $ϕ$ that agree in their zeroth and first derivatives above each spacetime point. Equipped with a notion of (spacetime and internal) symmetry on $J^1 E$, the idea is that one can write down the most general metric on $J^1 E$ consistent with symmetries, in the spirit of the effective field theorist, and pull it back to spacetime to build an invariant Lagrangian; because $J^1 E$ has `derivative coordinates', one naturally obtains operators with more than 2-derivatives from this geometry. We apply this formalism to various examples, including a single real scalar in 4d and a quartet of real scalars with $O(4)$ symmetry that describes the Higgs EFTs. We show how an entire non-redundant basis of 0-, 2-, and 4-derivative operators is obtained from jet bundle geometry in this way. Finally, we study the connection to amplitudes and the role of geometric invariants. |
| title | Jet Bundle Geometry of Scalar Field Theories |
| topic | High Energy Physics - Phenomenology High Energy Physics - Theory Mathematical Physics |
| url | https://arxiv.org/abs/2308.00017 |