Running EFT-hedron with null constraints at loop level
APA
(2025). Running EFT-hedron with null constraints at loop level. Perimeter Institute. https://pirsa.org/25030169
MLA
Running EFT-hedron with null constraints at loop level. Perimeter Institute, Mar. 18, 2025, https://pirsa.org/25030169
BibTex
@misc{ pirsa_PIRSA:25030169, doi = {10.48660/25030169}, url = {https://pirsa.org/25030169}, author = {}, keywords = {Particle Physics}, language = {en}, title = {Running EFT-hedron with null constraints at loop level}, publisher = {Perimeter Institute}, year = {2025}, month = {mar}, note = {PIRSA:25030169 see, \url{https://pirsa.org}} }
Abstract
I will introduce how to incorporate loop contributions into positivity bounds in a massless scalar theory with shift symmetry. The allowed region of Wilson coefficients is called the EFT-hedron. With loop contributions, the n=4 null constraint, which plays an important role in determining the allowed region for g3–g4 (the Wilson coefficients of dimension-10 and dimension-12 operators, respectively), is modified. This modification of the null constraint reveals new features of the EFT-hedron. We obtained a much stronger bound for g2 (the Wilson coefficient of dimension-8 operators) without using the full unitarity condition. Furthermore, we found a negative g4, which is not possible under the tree-level bound. It would be interesting to generalize our method to more complicated theory and test our results.