Simultaneous Measurement of Muon Neutrino ν_{µ} Charged-Current Single π

Neutrino-induced charged-current single π^{+} production in the Δ(1232) resonance region is of considerable interest to accelerator-based neutrino oscillation experiments. In this Letter, high statistic differential cross sections are reported for the semiexclusive reaction ν_{µ}A→µ^{-}π^{+}+ nucleon(s) on scintillator, carbon, water, iron, and lead targets recorded by MINERvA using a wideband ν_{µ} beam with ⟨E_{ν}⟩≈6 GeV. Suppression of the cross section at low Q^{2} and enhancement of low T_{π} are observed in both light and heavy nuclear targets compared with phenomenological models used in current neutrino interaction generators. The cross sections per nucleon for iron and lead compared with CH across the kinematic variables probed are 0.8 and 0.5 respectively, a scaling which is also not predicted by current generators.

Nuclear effects in neutrino induced coherent pion production at K2K and MiniBooNE.

The coherent pion production induced by neutrinos in nuclei is studied using a delta hole model in the local density approximation taking into account the renormalization of Delta properties in a nuclear medium. The pion absorption effects are included in an eikonal approximation. These effects give a large reduction in the total cross section. The numerical results for the total cross section are found to be consistent with recent experimental results from the K2K and MiniBooNE Collaborations and other older experiments in the intermediate energy region.

Simplified [correction of Simlified] calculation of mean QRS vector (mean electrical axis of heart) of electrocardiogram.

In clinical practice assessment of the mean QRS axis (MQRSA) provides information related either with hypertrophy of the ventricles or conduction blocks. The method adopted by clinicians i.e. the inspection of the QRS voltage in six of the limb leads has inherent element of subjectivity of approximately 10degrees. Moreover, in certain condition, when there is ambiguity about differentiation of left axis deviation assessed by inspection method in to either hypertrophy of left ventricles or complete/hemi block of the left bundle branches, accurate measurement of the axis becomes necessary to arrive at the correct diagnosis. Though a formula based on area under R wave and S-wave of the same QRS complex has been derived for accurate measurement of axis, considering its use in the computer software, working with ordinary electrocardiograph the only method for accurate measurement of the QRS axis is plotting method i. e. the net voltages in Lead-I, and III on their respective axes which is not practicable in clinical settings. Although, calculation of MQRSA by area method gives an accurate assessment of MQRSA, some authors prefer measurement of axis by voltage method, as in cases of the right ventricular hypertrophy with a broad S-wave calculation of axis by area method may give erroneous results. Hence, to obtain correct measurement of MQRSA, we have derived a simplified formula based on the net voltage of QRS complexes in Lead-I and Lead-III. The formula derived is as follows, Tan(theta) =(I + 2III) divided by sqrt [3I], where I and III represent net voltage in Lead-I and III, theta = angle subtended with the axis Lead-I. The value of theta can be found by using scientific calculator or the table. In case net voltage of QRS complex in Lead-I being negative, the value of the theta should be subtracted from 180degrees to find the angle of mean QRS vector.