23 research outputs found
Quenched lattice calculation of semileptonic heavy-light meson form factors
We calculate, in the continuum limit of quenched lattice QCD, the matrix
elements of the heavy-heavy vector current between heavy-light pseudoscalar
meson states. We present the form factors for different values of the initial
and final meson masses at finite momentum transfer. In particular, we calculate
the non-perturbative correction to the differential decay rate of the process B
--> D l nu including the case of a non-vanishing lepton mass.Comment: 16 pages, 10 figures, version accepted for publication on JHE
SF near the electroweak scale
We employ the chirally rotated Schr"odinger functional (SF) to study two-point fermion bilinear correlation functions used in the determination of on a series of well-tuned ensembles. The gauge configurations, which span renormalisation scales from 4 to 70~GeV, are generated with massless flavors and Schr"odinger Functional (SF) boundary conditions. Valence quarks are computed with SF boundary conditions. We show preliminary results on the tuning of the SF Symanzik coefficient and the scaling of the axial current normalization . Moreover we carry out a detailed comparison with the expectations from one-loop perturbation theory. Finally we outline how automatically -improved matrix elements, including BSM contributions, can be computed in a SF renormalization scheme
Nonperturbative running of the tensor operator for N_\rm{f}=3 QCD from the chirally rotated Schr\"odinger Functional
We study the Renormalisation Group (RG) running of the non-singlet tensor
operator, for QCD with Wilson fermions in a mixed
action setup, with standard Schr\"odinger Functional (SF) boundary conditions
for sea quarks and chirally rotated Schr\"odinger Functional (SF)
boundary conditions for valence quarks. Based on a recursive finite-size
scaling technique we compute non-perturbatively the tensor step-scaling
function for an energy range between a hadronic scale and an electroweak scale,
above which perturbation theory may be safely applied. Our result is expressed
as the RG-running factor , where the numerator is the scale
independent (Renormalisation Group Invariant - RGI) tensor operator and the
denominator is its renormalised counterpart at a hadronic scale
~MeV in a given scheme. We determine the
step-scaling function in four distinct renormalisation schemes. We also compute
the renormalisation parameters of these schemes at which,
combined with the RG-running factor, gives the scheme-independent quantity
in four schemes and for a range of bare
gauge couplings in which large volume hadronic matrix element simulations are
performed by the CLS consortium in QCD. All
four results are compatible and also agree with a recent determination based on
a unitary setup for Wilson quarks with Schr\"odinger Functional boundary
conditions~arXiv:2309.04314 . This provides a strong universality test.Comment: 35 pages, 28 figure
Non-perturbative generation of elementary fermion masses: a numerical study
In this talk we present a numerical lattice study of an SU(3) gauge model
where an SU(2) doublet of non-Abelian strongly interacting fermions is coupled
to a complex scalar field doublet via a Yukawa and a Wilson-like term. The
model enjoys an exact symmetry, acting on all fields, which prevents UV power
divergent fermion mass corrections, despite the presence of these two chiral
breaking operators in the Lagrangian. In the phase where the scalar potential
is non-degenerate and fermions are massless, the bare Yukawa coupling can be
set at a critical value at which chiral fermion transformations become
symmetries of the theory. Numerical simulations in the Nambu-Goldstone phase of
the critical theory, for which the renormalized Yukawa coupling by construction
vanishes, give evidence for non-perturbative generation of a UV finite fermion
mass term in the effective action.Comment: 7 pages, 8 figures, Proceedings of The 36th Annual International
Symposium on Lattice Field Theory, July 22-28, 2018, East Lansing, Michigan,
US
Non-perturbative determination of improvement b
We present our preliminary results of the non-perturbative determination of the valence mass dependent coefficients bA - bP and bm as well as the ratio ZPZm=ZA entering the flavour non-singlet PCAC relation in lattice QCD with Nf = 3 dynamical flavours. We apply the method proposed in the past for quenched approximation and Nf = 2 cases, employing a set of finite-volume ALPHA configurations with Schrödinger functional boundary conditions, generated with O(a) improved Wilson fermions and the tree-level Symanzik-improved gauge action for a range of couplings relevant for simulations at lattice spacings of about 0.09 fm and below
Non-perturbative determination of improvement b-coefficients in Nf = 3*
We present our preliminary results of the non-perturbative determination of the valence mass dependent coefficients bA - bP and bm as well as the ratio ZPZm=ZA entering the flavour non-singlet PCAC relation in lattice QCD with Nf = 3 dynamical flavours. We apply the method proposed in the past for quenched approximation and Nf = 2 cases, employing a set of finite-volume ALPHA configurations with Schrödinger functional boundary conditions, generated with O(a) improved Wilson fermions and the tree-level Symanzik-improved gauge action for a range of couplings relevant for simulations at lattice spacings of about 0.09 fm and below
Non-perturbative determination of improvement b-coefficients in Nf=3
We present our preliminary results of the non-perturbative determination of the valence mass dependent coefficients bA - bP and bm as well as the ratio ZPZm=ZA entering the flavour non-singlet PCAC relation in lattice QCD with Nf = 3 dynamical flavours. We apply the method proposed in the past for quenched approximation and Nf = 2 cases, employing a set of finite-volume ALPHA configurations with Schrödinger functional boundary conditions, generated with O(a) improved Wilson fermions and the tree-level Symanzik-improved gauge action for a range of couplings relevant for simulations at lattice spacings of about 0.09 fm and below