Nucleon axial form factors using Nf=2 twisted mass fermions with a physical value of the pion mass
dc.creator | Alexandrou, C | |
dc.creator | Constantinou, M | |
dc.creator | Hadjiyiannakou, K | |
dc.creator | Jansen, K | |
dc.creator | Kallidonis, C | |
dc.creator | Koutsou, G | |
dc.creator | Vaquero Aviles-Casco, A | |
dc.date.accessioned | 2021-02-03T00:04:00Z | |
dc.date.available | 2021-02-03T00:04:00Z | |
dc.date.issued | 2017-09-01 | |
dc.identifier.issn | 2470-0010 | |
dc.identifier.issn | 2470-0029 | |
dc.identifier.doi | http://dx.doi.org/10.34944/dspace/5663 | |
dc.identifier.other | FG4EB (isidoc) | |
dc.identifier.uri | http://hdl.handle.net/20.500.12613/5681 | |
dc.description.abstract | © 2017 American Physical Society. We present results on the nucleon axial and induced pseudoscalar form factors using an ensemble of two degenerate twisted mass clover-improved fermions with mass yielding a pion mass of mπ=130 MeV. We evaluate the isovector and the isoscalar, as well as the strange and the charm axial form factors. The disconnected contributions are evaluated using recently developed methods that include deflation of the lower eigenstates, allowing us to extract the isoscalar, strange, and charm axial form factors. We find that the disconnected quark loop contributions are nonzero and particularly large for the induced pseudoscalar form factor. | |
dc.format.extent | 054507- | |
dc.language.iso | en | |
dc.relation.haspart | Physical Review D | |
dc.relation.isreferencedby | American Physical Society (APS) | |
dc.subject | hep-lat | |
dc.subject | hep-lat | |
dc.title | Nucleon axial form factors using Nf=2 twisted mass fermions with a physical value of the pion mass | |
dc.type | Article | |
dc.type.genre | Journal Article | |
dc.relation.doi | 10.1103/PhysRevD.96.054507 | |
dc.ada.note | For Americans with Disabilities Act (ADA) accommodation, including help with reading this content, please contact scholarshare@temple.edu | |
dc.date.updated | 2021-02-03T00:03:57Z | |
refterms.dateFOA | 2021-02-03T00:04:00Z |