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005 | 20241222111609.0 | ||
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024 | 7 | _ | |a arXiv:2402.08715 |2 arXiv |
024 | 7 | _ | |a 10.3204/PUBDB-2024-00666 |2 datacite_doi |
037 | _ | _ | |a PUBDB-2024-00666 |
041 | _ | _ | |a English |
088 | _ | _ | |a DESY-24-020 |2 DESY |
088 | _ | _ | |a arXiv:2402.08715 |2 arXiv |
100 | 1 | _ | |a Manohar, Aneesh V. |b 0 |
245 | _ | _ | |a Field Redefinitions and Infinite Field Anomalous Dimensions |
260 | _ | _ | |c 2024 |
336 | 7 | _ | |a Preprint |b preprint |m preprint |0 PUB:(DE-HGF)25 |s 1710851280_2758569 |2 PUB:(DE-HGF) |
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336 | 7 | _ | |a ARTICLE |2 BibTeX |
336 | 7 | _ | |a Output Types/Working Paper |2 DataCite |
500 | _ | _ | |a 10+6 pages, 2 figures |
520 | _ | _ | |a Field redefinitions are commonly used to reduce the number of operators in the Lagrangian by removing redundant operators and transforming to a minimal operator basis. We give a general argument that such field redefinitions, while leaving the $S$-matrix invariant and consequently finite, lead not only to infinite Green's functions, but also to infinite field anomalous dimensions $\gamma_\phi$. These divergences cannot be removed by counterterms without reintroducing redundant operators. |
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536 | _ | _ | |a ASYMMETRY - Essential Asymmetries of Nature (101086085) |0 G:(EU-Grant)101086085 |c 101086085 |f HORIZON-MSCA-2021-SE-01 |x 2 |
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650 | _ | 7 | |a Green function |2 INSPIRE |
650 | _ | 7 | |a S-matrix |2 INSPIRE |
650 | _ | 7 | |a effective field theory |2 INSPIRE |
693 | _ | _ | |0 EXP:(DE-MLZ)NOSPEC-20140101 |5 EXP:(DE-MLZ)NOSPEC-20140101 |e No specific instrument |x 0 |
700 | 1 | _ | |a Pagès, Julie |b 1 |
700 | 1 | _ | |a Roosmale Nepveu, Jasper |0 P:(DE-H253)PIP1098857 |b 2 |e Corresponding author |
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913 | 1 | _ | |a DE-HGF |b Forschungsbereich Materie |l Matter and the Universe |1 G:(DE-HGF)POF4-610 |0 G:(DE-HGF)POF4-611 |3 G:(DE-HGF)POF4 |2 G:(DE-HGF)POF4-600 |4 G:(DE-HGF)POF |v Fundamental Particles and Forces |x 0 |
914 | 1 | _ | |y 2024 |
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