Showing 7 of 7 results
This paper reports measurements of processes: e+e- -> gamma KsK+pi-, e+e- -> gamma K+K-pi0, e+e- -> gamma phi eta, and e+e- -> gamma phi pi0. The initial state radiated photon allows to cover the hadronic final state in the energy range from thresholds up to ~4.6 GeV. The overall size of the data sample analyzed is 232 fb-1, collected by the BaBar detector running at the PEP-II e+e- storage ring. From the Dalitz plot analysis of the KsK+pi- final state, moduli and relative phase of the isoscalar and the isovector components of the e+e- -> K K*(892) cross section are determined. Parameters of phi and rho recurrences are also measured, using a global fitting procedure which exploits the interconnection among amplitudes, moduli and phases of the e+e- -> KsK+pi-, K+K-pi0, phi eta final states. The cross section for the OZI-forbidden process e+e- -> phi pi0, and the J/psi branching fractions to KK*(892) and K+K-eta are also measured.
The cross section for E+ E- --> K0S K+ PI- + CC with statistical errors only.
The cross section for E+ E- --> K+ K- PI0 with statistical errors only.
The cross section for E+ E- --> PHI PI0 with statistical errors only.
The cross section for E+ E- --> ETA K+ K- excluding the contribution from PHI --> K+ K- with statistical errors only.
The cross section for E+ E- --> PHI ETA with statistical errors only.
Isoscalar (I=0) component of the cross section for E+ E- --> K*(892) K with statistical errors only.
Isovector (I=1) component of the cross section for E+ E- --> K*(892) K with statistical errors only.
Isoscalar (I=0) component of the cross section for E+ E- --> K2*(1430) K with statistical errors only.
Isovector (I=1) component of the cross section for E+ E- --> K2*(1430) K with statistical errors only.
We study the processes $e^+ e^-\to 2(\pi^+\pi^-)\pi^0\gamma$, $2(\pi^+\pi^-)\eta\gamma$, $K^+ K^-\pi^+\pi^-\pi^0\gamma$ and $K^+ K^-\pi^+\pi^-\eta\gamma$ with the hard photon radiated from the initial state. About 20000, 4300, 5500 and 375 fully reconstructed events, respectively, are selected from 232 fb$^{-1}$ of BaBar data. The invariant mass of the hadronic final state defines the effective $e^+ e^-$ center-of-mass energy, so that the obtained cross sections from the threshold to about 5 GeV can be compared with corresponding direct \epem measurements, currently available only for the $\eta\pi^+\pi^-$ and $\omega\pi^+\pi^-$ submodes of the $e^+ e^-\to 2(\pi^+\pi^-)\pi^0$ channel. Studying the structure of these events, we find contributions from a number of intermediate states, and we extract their cross sections where possible. In particular, we isolate the contribution from $e^+ e^-\to\omega(782)\pi^+\pi^-$ and study the $\omega(1420)$ and $\omega(1650)$ resonances. In the charmonium region, we observe the $J/\psi$ in all these final states and several intermediate states, as well as the $\psi(2S)$ in some modes, and we measure the corresponding branching fractions.
Measured cross section for E+ E- --> 2(PI+ PI-) PI0 with statistical errorsonly.
Measured cross section for E+ E- --> ETA PI+ PI- with statistical errors only.
Measured cross section for E+ E- --> OMEGA PI+ PI- with statistical errors only.
Measured cross section for E+ E- --> OMEGA F0(975) with statistical errors only.
Measured cross section for E+ E- --> 2(PI+ PI-) ETA with statistical errorsonly.
Measured cross section for E+ E- --> ETAPRIME PI+ PI- with statistical errors only.
Measured cross section for E+ E- --> F1(1285) PI+ PI- with statistical errors only.
Measured cross section for E+ E- --> K+ K- PI+ PI- PI0 with statistical errors only.
Measured cross section for E+ E- --> PHI ETA with statistical errors only.
Measured cross section for E+ E- --> OMEGA K+ K- with statistical errors only.
Measured cross section for E+ E- --> K+ K- PI+ PI- ETA with statistical errors only.
We report results for the virtual photon asymmetry $A_1$ on the nucleon from new Jefferson Lab measurements. The experiment, which used the CEBAF Large Acceptance Spectrometer and longitudinally polarized proton ($^{15}$NH$_3$) and deuteron ($^{15}$ND$_3$) targets, collected data with a longitudinally polarized electron beam at energies between 1.6 GeV and 5.7 GeV. In the present paper, we concentrate on our results for $A_1(x,Q^2)$ and the related ratio $g_1/F_1(x,Q^2)$ in the resonance and the deep inelastic regions for our lowest and highest beam energies, covering a range in momentum transfer $Q^2$ from 0.05 to 5.0 GeV$^2$ and in final-state invariant mass $W$ up to about 3 GeV. Our data show detailed structure in the resonance region, which leads to a strong $Q^2$--dependence of $A_1(x,Q^2)$ for $W$ below 2 GeV. At higher $W$, a smooth approach to the scaling limit, established by earlier experiments, can be seen, but $A_1(x,Q^2)$ is not strictly $Q^2$--independent. We add significantly to the world data set at high $x$, up to $x = 0.6$. Our data exceed the SU(6)-symmetric quark model expectation for both the proton and the deuteron while being consistent with a negative $d$-quark polarization up to our highest $x$. This data setshould improve next-to-leading order (NLO) pQCD fits of the parton polarization distributions.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.1300 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.1500 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.1700 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.1900 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2100 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2300 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2500 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2700 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2900 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3100 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3300 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3500 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3700 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3900 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4100 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4300 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4500 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4700 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4900 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5100 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5300 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5500 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5700 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5900 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.6100 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.6300 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.6500 GeV.
A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.1100 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.1750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.2250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.2750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.3250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.3750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.4250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.4750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.5250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.5750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.6250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.6750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.7250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.7750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.8250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.8750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.9250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.9750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.0250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.0750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.1250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.1750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.2250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.2750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.3250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.3750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.4250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.4750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.5250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.5750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.6250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.6750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.7250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.7750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.8250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.8750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.9250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.9750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 3.0250 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 3.0750 GeV.
A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.1250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.0850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.0850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.0950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.0950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.7050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.7150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.7250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.7350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6950 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7050 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7150 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7250 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7350 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7450 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7550 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7650 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7750 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7850 GeV.
A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7950 GeV.
The ep -> e'pi^+n reaction was studied in the first and second nucleon resonance regions in the 0.25 GeV^2 < Q^2 < 0.65 GeV^2 range using the CLAS detector at Thomas Jefferson National Accelerator Facility. For the first time the absolute cross sections were measured covering nearly the full angular range in the hadronic center-of-mass frame. The structure functions sigma_TL, sigma_TT and the linear combination sigma_T+epsilon*sigma_L were extracted by fitting the phi-dependence of the measured cross sections, and were compared to the MAID and Sato-Lee models.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.11 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.13 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.15 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.17 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.19 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.21 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.23 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.25 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.27 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.29 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.31 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.33 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.35 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.37 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.39 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.41 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.43 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.45 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.47 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.49 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.51 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.53 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.55 GeV.
Structure functions for Q**2 = 0.30 GeV**2 and W = 1.57 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.11 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.13 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.15 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.17 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.19 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.21 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.23 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.25 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.27 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.29 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.31 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.33 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.35 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.37 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.39 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.41 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.43 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.45 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.47 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.49 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.51 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.53 GeV.
Structure functions for Q**2 = 0.40 GeV**2 and W = 1.55 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.11 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.13 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.15 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.17 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.19 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.21 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.23 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.25 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.27 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.29 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.31 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.33 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.35 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.37 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.39 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.41 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.43 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.45 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.47 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.49 GeV.
Structure functions for Q**2 = 0.50 GeV**2 and W = 1.51 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.11 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.13 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.15 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.17 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.19 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.21 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.23 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.25 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.27 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.29 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.31 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.33 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.35 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.37 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.39 GeV.
Structure functions for Q**2 = 0.60 GeV**2 and W = 1.41 GeV.
Cross sections for W = 1.11 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.11 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.11 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.11 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.11 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.11 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.11 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.11 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.11 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.13 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.15 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.17 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.19 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.21 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.23 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.25 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.27 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.29 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.31 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.33 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.35 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.37 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.39 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.41 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.43 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.45 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.47 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.49 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.51 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.53 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.55 GeV**2 and THETA = 157.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 7.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 22.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 37.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 52.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 67.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 82.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 97.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 112.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 127.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 142.5 deg.
Cross sections for W = 1.57 GeV**2 and THETA = 157.5 deg.
We measured the inclusive electron-proton cross section in the nucleon resonance region (W < 2.5 GeV) at momentum transfers Q**2 below 4.5 (GeV/c)**2 with the CLAS detector. The large acceptance of CLAS allowed for the first time the measurement of the cross section in a large, contiguous two-dimensional range of Q**2 and x, making it possible to perform an integration of the data at fixed Q**2 over the whole significant x-interval. From these data we extracted the structure function F2 and, by including other world data, we studied the Q**2 evolution of its moments, Mn(Q**2), in order to estimate higher twist contributions. The small statistical and systematic uncertainties of the CLAS data allow a precise extraction of the higher twists and demand significant improvements in theoretical predictions for a meaningful comparison with new experimental results.
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Short overview of experiments with SND detector at VEPP-2M e^+e^- collider in the energy range 2E = 400 - 1400 MeV and preliminary results of data analysis are presented.
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We have used the momentum spectrum of leptons produced in semileptonic B-meson decays to set a 90%-confidence-level upper limit on Γ(b→ulν)Γ(b→clν) of 4%. We also measure the semileptonic branching fractions of the B meson to be (12.0±0.7±0.5)% for electrons and (10.8±0.6±1.0)% for muons.
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