Effect of large-scale biomass burning on aerosol optical properties at the GAW regional station pha din, Vietnam.

In 2014, Pha Din (1466 m a.s.l.) was established as a Global Atmosphere Watch (GAW) regional station for aerosol and trace gas measurements in northwestern Vietnam. This study presents a five-year climatology of aerosol optical properties derived from nephelometer and aethalometer measurements and a comparison with ground-based remote sensing measurements at the nearby AERONET station Son La. The annual variations of the aerosol measurements at Pha Din are clearly dominated by annually recurring periods with high biomass burning activity in northern Southeast Asia (February– May). During these periods, the majority of air masses arriving at Pha Din originate from the southwest (northern Thailand, Laos and Myanmar). Both the meteorological conditions and the aerosol optical properties are very similar during the individual high biomass burning periods (increased temperature: > 20°C; moderate ambient relative humidity: 60–70%; decreased single scattering albedo: 0.8–0.9; increased absorption Ångström exponent: 1.6–2.0; and scattering Ångström exponent significantly larger than 1). Prior to the biomass burning season (October–January), the meteorological conditions at Pha Din are influenced by the SE Asian monsoon, leading to a frequent transport of air masses from SW China with moderate aerosol loadings. The lowest pollution levels are observed from June to September, which represents the wet season

Evidence for the singly Cabibbo suppressed decay Lambda_c+ --> p eta and search for Lambda_c+ --> p pi0

We study the singly Cabibbo suppressed decays Lambda_c+ --> p eta and Lambda_c+ → pπ0 using Lambda+Lambda_c- pairs produced by e+e- collisions at a center-of-mass energy of sqrt(s) =4.6 GeV. The data sample was collected by the BESIII detector at the BEPCII collider and corresponds to an integrated luminosity of 567 pb-1. We find the first evidence for the decay Lambda_c+ --> p eta with a statistical significance of 4.2 sigma and measure its branching fraction to be B( Lambda_c+ --> p eta)=(1.24±0.28(stat)±0.10(syst))10-3. No significant Lambda_c+ --> p pi0 signal is observed. We set an upper limit on its branching fraction B( Lambda_c+ --> p pi0)<2.7x10-4 at the 90% confidence level

Observation of χc2→η′η′\chi_{c2}\to\eta'\eta' and χc0,2→ηη′\chi_{c0,2}\to\eta\eta'

Using a sample of 448.1×106  ψ(3686) events collected with the BESIII detector in 2009 and 2012, we study the decays χc0,2→η′η′ and ηη′. The decays χc2→η′η′, χc0→ηη′ and χc2→ηη′ are observed for the first time with statistical significances of 9.6σ, 13.4σ and 7.5σ, respectively. The branching fractions are determined to be B(χc0→η′η′)=(2.19±0.03±0.14)×10-3, B(χc2→η′η′)=(4.76±0.56±0.38)×10-5, B(χc0→ηη′)=(8.92±0.84±0.65)×10-5 and B(χc2→ηη′)=(2.27±0.43±0.25)×10-5, where the first uncertainties are statistical and the second are systematic. The precision for the measurement of B(χc0→η′η′) is significantly improved compared to previous measurements. Based on the measured branching fractions, the role played by the doubly and singly Okubo-Zweig-Iizuka disconnected transition amplitudes for χc0,2 decays into pseudoscalar meson pairs can be clarified.Using a sample of $447.9\times 10^6$ $\psi(3686)$ events collected with the BESIII detector in 2009 and 2012, we study the decays $\chi_{c0,2}\to$ $\eta'\eta'$ and $\eta\eta'$. The decays $\chi_{c2}\to\eta'\eta'$, $\chi_{c0}\to\eta\eta'$ and $\chi_{c2}\to\eta\eta'$ are observed for the first time with statistical significances of $9.6\sigma$, $13.4\sigma$ and $7.5\sigma$, respectively. The branching fractions are determined to be $\mathcal{B}(\chi_{c0}\to\eta'\eta') =(2.19\pm0.03\pm0.14)\times10^{-3}$, $\mathcal{B}(\chi_{c2}\to\eta'\eta') = (4.76\pm0.56\pm0.38)\times10^{-5}$, $\mathcal{B}(\chi_{c0}\to\eta\eta') = (8.92\pm0.84\pm0.65)\times10^{-5}$ and $\mathcal{B}(\chi_{c2}\to\eta\eta') = (2.27\pm0.43\pm0.25)\times10^{-5}$, where the first uncertainties are statistical and the second systematic. The precision for the measurement of $\mathcal{B}(\chi_{c0}\to\eta'\eta')$ is significantly improved compared to previous measurements. Based on the measured branching fractions, the role played by the doubly and singly Okubo-Zweig-Iizuka disconnected transition amplitudes for $\chi_{c0,2}$ decays into pseudoscalar meson pairs can be clarified

Measurement of the phase between strong and electromagnetic amplitudes of J/ψ decays

Using 16 energy points of e+e− annihilation data collected in the vicinity of the J/ψ resonance with the BESIII detector and with a total integrated luminosity of around 100pb−1, we study the relative phase between the strong and electromagnetic amplitudes of J/ψ decays. The relative phase between J/ψ electromagnetic decay and the continuum process (e+e− annihilation without the J/ψ resonance) is confirmed to be zero by studying the cross section lineshape of μ+μ− production. The relative phase between J/ψ strong and electromagnetic decays is then measured to be (84.9±3.6)∘ or (−84.7±3.1)∘ for the 2(π+π−)π0 final state by investigating the interference pattern between the J/ψ decay and the continuum process. This is the first measurement of the relative phase between J/ψ strong and electromagnetic decays into a multihadron final state using the lineshape of the production cross section. We also study the production lineshape of the multihadron final state ηπ+π− with η→π+π−π0, which provides additional information about the phase between the J/ψ electromagnetic decay amplitude and the continuum process. Additionally, the branching fraction of J/ψ→2(π+π−)π0 is measured to be (4.73±0.44)% or (4.85±0.45)%, and the branching fraction of J/ψ→ηπ+π− is measured to be (3.78±0.68)×10−4. Both of them are consistent with the world average values. The quoted uncertainties include both statistical and systematic uncertainties, which are mainly caused by the low statistics. Keywords: Phase, Strong amplitude, Electromagnetic amplitude, J/ψ decay, BESII

Observation of the decay Lamda_c+ -->Sigma-pi+pi+pi0

We report the first observation of the decay Lambda_c+ --> Sigma- pi+pi+pi0, based on data obtained in e+e- annihilations with an integrated luminosity of 567 pb−1 at sqrt(s)=4.6GeV. The data were collected with the BESIII detector at the BEPCII storage rings. The absolute branching fraction B(Lambda_c+ --> Sigma- pi+pi+pi0) is determined to be (2.11 ± 0.33(stat.) ± 0.14(syst.))%. In addition, an improved measurement of B(Lambda_c+ → Sigma−π+π+) is determined as (1.81 ± 0.17(stat.) ± 0.09(syst.))%