Cargando…

Semileptonic $D \rightarrow \pi \ell \nu$, $D \rightarrow K \ell \nu$ and $D_s \rightarrow K \ell \nu$ decays with 2+1f domain wall fermions

We present the status of our project to calculate $D \to \pi \ell \nu$, $D \to K \ell \nu$ and $D_s \to K \ell \nu$ semileptonic form factors using domain wall fermions for both heavy and light quarks. Our computations are performed using RBC/UKQCD's set of 2+1 flavour domain wall fermion and I...

Descripción completa

Detalles Bibliográficos
Autores principales: Marshall, Michael, Boyle, Peter, Del Debbio, Luigi, Erben, Felix, Flynn, Jonathan, Jüttner, Andreas, Portelli, Antonin, Tsang, Justus Tobias, Witzel, Oliver
Lenguaje:eng
Publicado: 2022
Materias:
Acceso en línea:https://dx.doi.org/10.22323/1.396.0416
http://cds.cern.ch/record/2799239
_version_ 1780972527505375232
author Marshall, Michael
Boyle, Peter
Del Debbio, Luigi
Erben, Felix
Flynn, Jonathan
Jüttner, Andreas
Portelli, Antonin
Tsang, Justus Tobias
Witzel, Oliver
author_facet Marshall, Michael
Boyle, Peter
Del Debbio, Luigi
Erben, Felix
Flynn, Jonathan
Jüttner, Andreas
Portelli, Antonin
Tsang, Justus Tobias
Witzel, Oliver
author_sort Marshall, Michael
collection CERN
description We present the status of our project to calculate $D \to \pi \ell \nu$, $D \to K \ell \nu$ and $D_s \to K \ell \nu$ semileptonic form factors using domain wall fermions for both heavy and light quarks. Our computations are performed using RBC/UKQCD's set of 2+1 flavour domain wall fermion and Iwasaki gauge field ensembles. We plan to calculate three-point functions covering the full, physically allowed kinematic range. Given that the signal decays faster than the noise, unambiguously and reliably extracting the ground state is critical for success. We include an analysis of operator diagonalisation within several possible $2 \times 2$ operator bases and find an admixture of gauged fixed wall and $\mathbb{Z} \left( 2 \right)$ wall sources to be acceptable at both zero and non-zero momentum. Initial results for semileptonic form factors are presented for first ensembles.
id cern-2799239
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2022
record_format invenio
spelling cern-27992392023-03-14T07:58:15Zdoi:10.22323/1.396.0416http://cds.cern.ch/record/2799239engMarshall, MichaelBoyle, PeterDel Debbio, LuigiErben, FelixFlynn, JonathanJüttner, AndreasPortelli, AntoninTsang, Justus TobiasWitzel, OliverSemileptonic $D \rightarrow \pi \ell \nu$, $D \rightarrow K \ell \nu$ and $D_s \rightarrow K \ell \nu$ decays with 2+1f domain wall fermionshep-latParticle Physics - LatticeWe present the status of our project to calculate $D \to \pi \ell \nu$, $D \to K \ell \nu$ and $D_s \to K \ell \nu$ semileptonic form factors using domain wall fermions for both heavy and light quarks. Our computations are performed using RBC/UKQCD's set of 2+1 flavour domain wall fermion and Iwasaki gauge field ensembles. We plan to calculate three-point functions covering the full, physically allowed kinematic range. Given that the signal decays faster than the noise, unambiguously and reliably extracting the ground state is critical for success. We include an analysis of operator diagonalisation within several possible $2 \times 2$ operator bases and find an admixture of gauged fixed wall and $\mathbb{Z} \left( 2 \right)$ wall sources to be acceptable at both zero and non-zero momentum. Initial results for semileptonic form factors are presented for first ensembles.We present the status of our project to calculate $D \to \pi \ell \nu$, $D \to K \ell \nu$ and $D_s \to K \ell \nu$ semileptonic form factors using domain wall fermions for both heavy and light quarks. Our computations are performed using RBC/UKQCD's set of 2+1 flavour domain wall fermion and Iwasaki gauge field ensembles. We plan to calculate three-point functions covering the full, physically allowed kinematic range. Given that the signal decays faster than the noise, unambiguously and reliably extracting the ground state is critical for success. We include an analysis of operator diagonalisation within several possible $2 \times 2$ operator bases and find an admixture of gauged fixed wall and $\mathbb{Z} \left( 2 \right)$ wall sources to be acceptable at both zero and non-zero momentum. Initial results for semileptonic form factors are presented for first ensembles.arXiv:2201.02680oai:cds.cern.ch:27992392022-01-07
spellingShingle hep-lat
Particle Physics - Lattice
Marshall, Michael
Boyle, Peter
Del Debbio, Luigi
Erben, Felix
Flynn, Jonathan
Jüttner, Andreas
Portelli, Antonin
Tsang, Justus Tobias
Witzel, Oliver
Semileptonic $D \rightarrow \pi \ell \nu$, $D \rightarrow K \ell \nu$ and $D_s \rightarrow K \ell \nu$ decays with 2+1f domain wall fermions
title Semileptonic $D \rightarrow \pi \ell \nu$, $D \rightarrow K \ell \nu$ and $D_s \rightarrow K \ell \nu$ decays with 2+1f domain wall fermions
title_full Semileptonic $D \rightarrow \pi \ell \nu$, $D \rightarrow K \ell \nu$ and $D_s \rightarrow K \ell \nu$ decays with 2+1f domain wall fermions
title_fullStr Semileptonic $D \rightarrow \pi \ell \nu$, $D \rightarrow K \ell \nu$ and $D_s \rightarrow K \ell \nu$ decays with 2+1f domain wall fermions
title_full_unstemmed Semileptonic $D \rightarrow \pi \ell \nu$, $D \rightarrow K \ell \nu$ and $D_s \rightarrow K \ell \nu$ decays with 2+1f domain wall fermions
title_short Semileptonic $D \rightarrow \pi \ell \nu$, $D \rightarrow K \ell \nu$ and $D_s \rightarrow K \ell \nu$ decays with 2+1f domain wall fermions
title_sort semileptonic $d \rightarrow \pi \ell \nu$, $d \rightarrow k \ell \nu$ and $d_s \rightarrow k \ell \nu$ decays with 2+1f domain wall fermions
topic hep-lat
Particle Physics - Lattice
url https://dx.doi.org/10.22323/1.396.0416
http://cds.cern.ch/record/2799239
work_keys_str_mv AT marshallmichael semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions
AT boylepeter semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions
AT deldebbioluigi semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions
AT erbenfelix semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions
AT flynnjonathan semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions
AT juttnerandreas semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions
AT portelliantonin semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions
AT tsangjustustobias semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions
AT witzeloliver semileptonicdrightarrowpiellnudrightarrowkellnuanddsrightarrowkellnudecayswith21fdomainwallfermions