B → D ℓ ν ℓ semileptonic form factors from lattice QCD with Möbius domain-wall quarks
We calculate the form factors for the B → D * ℓ ν ℓ decay in 2 + 1 flavor lattice QCD. For all quark flavors, we employ the Möbius domain-wall action, which preserves chiral symmetry to a good precision. Our gauge ensembles are generated at three lattice cutoffs a − 1 ∼ 2.5 , 3.6, and 4.5 GeV with p...
Gespeichert in:
Veröffentlicht in: | Physical review. D 2024-04, Vol.109 (7), Article 074503 |
---|---|
Hauptverfasser: | , , , , , , , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | We calculate the form factors for the
B
→
D
*
ℓ
ν
ℓ
decay in
2
+
1
flavor lattice QCD. For all quark flavors, we employ the Möbius domain-wall action, which preserves chiral symmetry to a good precision. Our gauge ensembles are generated at three lattice cutoffs
a
−
1
∼
2.5
, 3.6, and 4.5 GeV with pion masses as low as
M
π
∼
230
MeV
. The physical lattice size
L
satisfies the condition
M
π
L
≥
4
to control finite volume effects (FVEs), while we simulate a smaller size at the smallest
M
π
to directly examine FVEs. The bottom quark masses are chosen in a range from the physical charm quark mass to
0.7
a
−
1
to control discretization effects. We extrapolate the form factors to the continuum limit and physical quark masses based on heavy meson chiral perturbation theory at next-to-leading order. Then the recoil parameter dependence is parametrized using a model independent form leading to our estimate of the decay rate ratio between the tau (
ℓ
=
τ
) and light lepton (
ℓ
=
e
,
μ
) channels
R
(
D
*
)
=
0.252
(
22
)
in the Standard Model. A simultaneous fit with recent data from the Belle experiment yields
|
V
c
b
|
=
39.19
(
91
)
×
10
−
3
, which is consistent with previous exclusive determinations, and shows good consistency in the kinematical distribution of the differential decay rate between the lattice and experimental data. |
---|---|
ISSN: | 2470-0010 2470-0029 |
DOI: | 10.1103/PhysRevD.109.074503 |