Aviso: para depositar documentos, por favor, inicia sesión e identifícate con tu cuenta de correo institucional de la UCM con el botón MI CUENTA UCM. No emplees la opción AUTENTICACIÓN CON CONTRASEÑA
 

$$\omega \rightarrow 3\pi $$ and $$\omega \pi ^{0}$$ transition form factor revisited

dc.contributor.authorAlbaladejo, M.
dc.contributor.authorDanilkin, I.
dc.contributor.authorGonzàlez Solís, S.
dc.contributor.authorWinney, D.
dc.contributor.authorFernández Ramírez, César
dc.contributor.authorBlin, A. N. Hiller
dc.contributor.authorMathieu, Vincent
dc.contributor.authorMikhasenko, M.
dc.contributor.authorPilloni, A.
dc.contributor.authorSzczepaniak, A.
dc.date.accessioned2023-06-17T08:29:14Z
dc.date.available2023-06-17T08:29:14Z
dc.date.issued2020-12-02
dc.description.abstractIn light of recent experimental results, we revisit the dispersive analysis of the ω→3π decay amplitude and of the ωπ0 transition form factor. Within the framework of the Khuri–Treiman equations, we show that the ω→3π Dalitz-plot parameters obtained with a once-subtracted amplitude are in agreement with the latest experimental determination by BESIII. Furthermore, we show that at low energies the ωπ0 transition form factor obtained from our determination of the ω→3π amplitude is consistent with the data from MAMI and NA60 experiments.
dc.description.departmentDepto. de Física Teórica
dc.description.facultyFac. de Ciencias Físicas
dc.description.refereedTRUE
dc.description.sponsorshipU.S. Department of Energy
dc.description.sponsorshipU.S. National Science Foundation
dc.description.sponsorshipDeutsche Forschungsgemeinschaft
dc.description.sponsorshipNational Science Foundation
dc.description.sponsorshipPAPIITDGAPA (UNAM, Mexico)
dc.description.sponsorshipCONACYT (Mexico)
dc.description.statuspub
dc.eprint.idhttps://eprints.ucm.es/id/eprint/74457
dc.identifier.doi10.1140/epjc/s10052-020-08576-6
dc.identifier.issn1434-6044
dc.identifier.officialurlhttps://doi.org/10.1140/epjc%2Fs10052-020-08576-6
dc.identifier.relatedurlhttps://link.springer.com/article/10.1140/epjc/s10052-020-08576-6
dc.identifier.urihttps://hdl.handle.net/20.500.14352/7264
dc.issue.number12
dc.journal.titleThe European Physical Journal C
dc.language.isoeng
dc.publisherSpringer
dc.relation.projectIDDE-AC05-06OR23177 and DEFG02-87ER40365
dc.relation.projectIDPHY-1415459
dc.relation.projectID204404729 - SFB 1044, 39083149
dc.relation.projectIDPHY-2013184
dc.relation.projectIDIA101819
dc.relation.projectIDA1-S-21389
dc.rightsAtribución 3.0 España
dc.rights.accessRightsopen access
dc.rights.urihttps://creativecommons.org/licenses/by/3.0/es/
dc.subject.ucmFísica-Modelos matemáticos
dc.subject.ucmFísica matemática
dc.title$$\omega \rightarrow 3\pi $$ and $$\omega \pi ^{0}$$ transition form factor revisited
dc.typejournal article
dc.volume.number80
dspace.entity.typePublication
relation.isAuthorOfPublication51733d00-4a0c-402c-8870-a26d1b00ea00
relation.isAuthorOfPublication17de49b7-46a8-4bce-b8df-ee29abc569d8
relation.isAuthorOfPublication.latestForDiscovery51733d00-4a0c-402c-8870-a26d1b00ea00

Download

Original bundle

Now showing 1 - 1 of 1
Loading...
Thumbnail Image
Name:
s10052-020-08576-6.pdf
Size:
3.11 MB
Format:
Adobe Portable Document Format

Collections