71 research outputs found
D-meson semileptonic decays to pseudoscalars from four-flavor lattice QCD
We present lattice-QCD calculations of the hadronic form factors for the
semileptonic decays , , and .
Our calculation uses the highly improved staggered quark (HISQ) action for all
valence and sea quarks and includes MILC ensembles with lattice
spacings ranging from fm down to fm. At most lattice
spacings, an ensemble with physical-mass light quarks is included. The HISQ
action allows all the quarks to be treated with the same relativistic
light-quark action, allowing for nonperturbative renormalization using partial
conservation of the vector current. We combine our results with experimental
measurements of the differential decay rates to determine
and This result for is
the most precise to date, with a lattice-QCD error that is, for the first time
for the semileptonic extraction, at the same level as the experimental error.
Using recent measurements from BES III, we also give the first-ever
determination of from . Our results also furnish new
Standard Model calculations of the lepton flavor universality ratios
, , and , which are consistent within with experimental
measurements. Our extractions of and , when combined with
a value for , provide the most precise test of second-row CKM
unitarity, finding agreement with unitarity at the level of one standard
deviation.Comment: 92 page
The anomalous magnetic moment of the muon in the Standard Model
194 pages, 103 figures, bib files for the citation references are available from: https://muon-gm2-theory.illinois.eduWe review the present status of the Standard Model calculation of the anomalous magnetic moment of the muon. This is performed in a perturbative expansion in the fine-structure constant and is broken down into pure QED, electroweak, and hadronic contributions. The pure QED contribution is by far the largest and has been evaluated up to and including with negligible numerical uncertainty. The electroweak contribution is suppressed by and only shows up at the level of the seventh significant digit. It has been evaluated up to two loops and is known to better than one percent. Hadronic contributions are the most difficult to calculate and are responsible for almost all of the theoretical uncertainty. The leading hadronic contribution appears at and is due to hadronic vacuum polarization, whereas at the hadronic light-by-light scattering contribution appears. Given the low characteristic scale of this observable, these contributions have to be calculated with nonperturbative methods, in particular, dispersion relations and the lattice approach to QCD. The largest part of this review is dedicated to a detailed account of recent efforts to improve the calculation of these two contributions with either a data-driven, dispersive approach, or a first-principle, lattice-QCD approach. The final result reads and is smaller than the Brookhaven measurement by 3.7. The experimental uncertainty will soon be reduced by up to a factor four by the new experiment currently running at Fermilab, and also by the future J-PARC experiment. This and the prospects to further reduce the theoretical uncertainty in the near future-which are also discussed here-make this quantity one of the most promising places to look for evidence of new physics
Association of Medical Directors of Information Systems Consensus on Inpatient Electronic Health Record Documentation
Altered dynamics of action potential restitution and alternans in humans with structural heart disease
abstract: BACKGROUND: Restitution kinetics and alternans of ventricular action potential duration (APD) have been shown to be important determinants of cardiac electrical stability. In this study, we tested the hypothesis that APD restitution and alternans properties differ between normal and diseased human ventricular myocardium. METHODS AND RESULTS: Monophasic action potentials were recorded from the right ventricular septum in 24 patients with structural heart disease (SHD) and in 12 patients without SHD. Standard and dynamic restitution relations were constructed by plotting APD as a function of the preceding diastolic interval. The dynamic restitution relation of both groups showed a steeply sloped segment at short diastolic intervals that was associated with the occurrence of APD alternans. Patients with SHD had a wider diastolic interval range over which APD alternans was present (mean+/-SEM 68+/-11 versus 12+/-2 ms) and showed an earlier onset (168+/-7 versus 225+/-4 bpm) and an increased magnitude (20+/-2 versus 11+/-2 ms) of APD alternans compared with patients without SHD. The occurrence of APD alternans during induced ventricular tachycardia (6 episodes) and during rapid pacing could be derived from the dynamic restitution function. CONCLUSIONS: There are marked differences in the dynamics of APD restitution and alternans in the ventricular myocardium of patients with SHD compared with patients without SHD. These differences may contribute importantly to cardiac electrical instability in diseased human hearts and may represent a promising target for antiarrhythmic substrate modification
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