ترغب بنشر مسار تعليمي؟ اضغط هنا

Towards fully non-perturbative computation of inelastic $ell N$ scattering cross sections from lattice QCD

61   0   0.0 ( 0 )
 نشر من قبل Shoji Hashimoto
 تاريخ النشر 2020
  مجال البحث
والبحث باللغة English




اسأل ChatGPT حول البحث

We propose a fully non-perturbative method to compute inelastic lepton-nucleon ($ell N$) scattering cross sections using lattice QCD. The method is applicable even at low energies, such as the energy region relevant for the recent and future neutrino-nucleon ($ u N$) scattering experiments, for which perturbative analysis is invalidated. The basic building block is the forward Compton-scattering amplitude, or the hadronic tensor, computed on a Euclidean lattice. Total cross section is constructed from the hadronic tensor by multiplying a phase space factor and integrating over the energy and momentum of final hadronic states. The energy integral that induces a sum over all possible final states is performed implicitly by promoting the phase space factor to an operator written in terms of the transfer matrix on the lattice. The formalism is imported from that of the inclusive semileptonic B meson decay [P. Gambino, S. Hashimoto, arXiv:2005.13730]. It can be generalized to compute the $ell N$ scattering cross sections and their moments, as well as the virtual correction to the nuclear $beta$-decay. Necessary quark-line contractions for two current insertions corresponding to the Compton amplitude to be computed on the lattice are summarized.



قيم البحث

اقرأ أيضاً

206 - Yasumichi Aoki 2010
Recent developments in non-perturbative renormalization for lattice QCD are reviewed with a particular emphasis on RI/MOM scheme and its variants, RI/SMOM schemes. Summary of recent developments in Schroedinger functional scheme, as well as the summa ry of related topics are presented. Comparison of strong coupling constant and the strange quark mass from various methods are made.
We present lattice results for the isovector unpolarized parton distribution with nonperturbative RI/MOM-scheme renormalization on the lattice. In the framework of large-momentum effective field theory (LaMET), the full Bjorken-$x$ dependence of a mo mentum-dependent quasi-distribution is calculated on the lattice and matched to the ordinary lightcone parton distribution at one-loop order, with power corrections included. The important step of RI/MOM renormalization that connects the lattice and continuum matrix elements is detailed in this paper. A few consequences of the results are also addressed here.
We present the first lattice QCD determination of the $Lambda_b to Lambda^*(1520)$ vector, axial vector, and tensor form factors that are relevant for the rare decays $Lambda_b to Lambda^*(1520)ell^+ell^-$. The lattice calculation is performed in the $Lambda^*(1520)$ rest frame with nonzero $Lambda_b$ momenta, and is limited to the high-$q^2$ region. An interpolating field with covariant derivatives is used to obtain good overlap with the $Lambda^*(1520)$. The analysis treats the $Lambda^*(1520)$ as a stable particle, which is expected to be a reasonable approximation for this narrow resonance. A domain-wall action is used for the light and strange quarks, while the $b$ quark is implemented with an anisotropic clover action with coefficients tuned to produce the correct $B_s$ kinetic mass, rest mass, and hyperfine splitting. We use three different ensembles of lattice gauge-field configurations generated by the RBC and UKQCD collaborations, and perform extrapolations of the form factors to the continuum limit and physical pion mass. We give Standard-Model predictions for the $Lambda_b to Lambda^*(1520)ell^+ell^-$ differential branching fraction and angular observables in the high-$q^2$ region.
341 - Rainer Sommer , Ulli Wolff 2015
We review the long term project of the ALPHA collaboration to compute in QCD the running coupling constant and quark masses at high energy scales in terms of low energy hadronic quantities. The adapted techniques required to numerically carry out the required multiscale non-perturbative calculation with our special emphasis on the control of systematic errors are summarized. The complete results in the two dynamical flavor approximation are reviewed and an outlook is given on the ongoing three flavor extension of the programme with improved target precision.
We develop a methodology for the computation of the $Kto ell u_ell ell^+ ell^-$ decay width using lattice QCD and present an exploratory study here. We use a scalar function method to account for the momentum dependence of the decay amplitude and ado pt the infinite volume reconstruction (IVR) method to reduce the systematic errors such as the temporal truncation effects and the finite-volume effects. We then perform a four-body phase-space integral to obtain the decay width. The only remaining technical problem is the possible power-law finite-volume effects associated with the process of $Ktopipi ell u_ellto ell u_ell ell^+ ell^-$, where the intermediate state involves multiple hadrons. In this work, we use a gauge ensemble of twisted mass fermion with a pion mass $m_pi=352$ MeV and a nearly-physical kaon mass. At this kinematics, the $pipi$ in the intermediate state cannot be on shell simultaneously as $2m_pi>m_K$ and the finite-volume effects associate with $pipi$ state are exponentially suppressed. Using the developed methods mentioned above, we calculate the branching ratios for four channels of $Kto ell u_ellell^+ ell^-$, and obtain the results close to the experimental measurements and ChPT predictions. Our work demonstrates the capability of lattice QCD to improve Standard Model prediction in $Kto ell u_ell ell^+ ell^-$ decay width.
التعليقات
جاري جلب التعليقات جاري جلب التعليقات
سجل دخول لتتمكن من متابعة معايير البحث التي قمت باختيارها
mircosoft-partner

هل ترغب بارسال اشعارات عن اخر التحديثات في شمرا-اكاديميا