(ProQuest: ... denotes formulae and/or non-USASCII text omitted) We report results of a study of doubly charmed baryons and charmed strange baryons. The analysis is performed using a 980 fb super(-1) ...data sample collected with the Belle detector at the KEKB asymmetric-energy e super(+)e super(-) collider. We search for doubly charmed baryons ... with the ... and ... final states. No significant signal is observed. We also search for two excited charmed strange baryons, Xi sub(c)(3055) super(+) and Xi sub(c)(3123) super(+) with the ... and ... final states. The Xi sub(c)(3055) super(+) signal is observed with a significance of 6.6 standard deviations including systematic uncertainty, while no signature of the Xi sub(c)(3123) super(+) is seen. We also study properties of the Xi sub(c)(2645) super(+) and measure a width of 2.6 + or - 0.2(stat) + or - 0.4(syst) MeV /c super(2), which is the first significant determination.
PM
10
, PM
25
, precursor gas, and upper-air meteorological measurements were taken in Mexico City, Mexico, from February 23 to March 22, 1997, to understand concentrations and chemical compositions ...of the city's particulate matter (PM). Average 24-hr PM
10
concentrations over the period of study at the core sites in the city were 75 H g/m
3
. The 24-hr standard of 150 μ g/m
3
was exceeded for seven samples taken during the study period; the maximum 24-hr concentration measured was 542 μ g/m
3
. Nearly half of the PM
10
was composed of fugitive dust from roadways, construction, and bare land. About 50% of the PM
10
consisted of PM
2.5
, with higher percentages during the morning hours. Organic and black carbon constituted up to half of the PM
2.5
. PM concentrations were highest during the early morning and after sunset, when the mixed layers were shallow. Meteorological measurements taken during the field campaign show that on most days air was transported out of the Mexico City basin during the afternoon with little day-to-day carryover.
Remodeling of conduction pathways in the hypertrophic response to myocardial injury is a potential mechanism leading to the development of anatomic substrates of lethal arrhythmias. To delineate the ...responsible mechanisms and to directly relate changes in intercellular coupling at gap junctions with electrophysiological alterations, we studied the effects of cAMP, a mediator of cardiac hypertrophy, on action potential conduction velocity and connexin expression in neonatal rat ventricular myocyte cultures. Conduction velocity was measured with an optical activation mapping technique in cells loaded with the voltage-sensitive dye RH-237. Action potentials were conducted 24% to 29% more rapidly (P < .005) after incubating cultures for 24 hours with the cAMP analogue dibutyryl cAMP (db-cAMP, 1 mmol/L). However, db-cAMP caused no change in the maximum rate of rise of the action potential upstroke, Vmax. Electron and immunofluorescence microscopy revealed a significant increase in the number and size of gap junctions in db-cAMP-treated cells. Immunoblotting showed that the total amounts of the ventricular gap junction proteins connexin43 and connexin45 (Cx43 and Cx45, respectively) increased 2- to 4-fold. Immuno-precipitation of metabolically labeled connexin proteins revealed a dose-dependent increase in the rate of Cx45 protein synthesis in myocytes exposed to db-cAMP ( > 2-fold after a 4-hour exposure) but no change in the Cx43 synthesis rate. Northern blot analysis demonstrated a time-dependent increase in the amount of Cx43 mRNA, with a maximum 3.3-fold increase after 4 hours of exposure to 1 mmol/L db-cAMP; cycloheximide did not block this effect. In contrast, Cx45 mRNA levels were not altered significantly after db-cAMP treatment. Thus, cAMP causes a significant increase in conduction velocity that appears to be attributable largely to enhanced expression of proteins responsible for intercellular communication. Cx43 and Cx45 levels appear to be upregulated by cAMP by disparate molecular mechanisms.
We report the first observation of the double strange baryon Ξ(1620)0 in its decay to Ξ−π+ via Ξ+c → Ξ−π+π+ decays based on a 980 fb−1 data sample collected with the Belle detector at the KEKB ...asymmetric-energy e+e− collider. The mass and width are measured to be 1610.4 ± 6.0(stat)+6.1−4.2(syst) MeV /c2 and 59.9 ± 4.8(stat)+2.8−7.1(syst) MeV, respectively. We obtain 4.0σ evidence of the Ξ(1690)0 with the same data sample. These results shed light on the structure of hyperon resonances with strangeness S = −2
The Majorana Demonstrator will search for the neutrinoless double-beta (ββ0ν) decay of the isotope 76Ge with a mixed array of enriched and natural germanium detectors. The observation of this rare ...decay would indicate that the neutrino is its own antiparticle, demonstrate that lepton number is not conserved, and provide information on the absolute mass scale of the neutrino. The Demonstrator is being assembled at the 4850-foot level of the Sanford Underground Research Facility in Lead, South Dakota. The array will be situated in a low-background environment and surrounded by passive and active shielding. Here we describe the science goals of the Demonstrator and the details of its design.
The Majorana Demonstrator will search for the neutrinoless double–beta decay (0vββ) of the 76Ge isotope with a mixed array of enriched and natural germanium detectors. The observation of this rare ...decay would indicate the neutrino is its own anti–particle, demonstrate that lepton number is not conserved, and provide information on the absolute mass–scale of the neutrino. The Demonstrator is being assembled at the 4850 foot level of the Sanford Underground Research Facility in Lead, South Dakota. The array will be contained in a low–background environment and surrounded by passive and active shielding. The goals for the Demonstrator are: demonstrating a background rate less than 3 t−1 y−1 in the 4 keV region of interest (ROI) surrounding the 2039 keV 76Ge endpoint energy; establishing the technology required to build a tonne–scale germanium based double–beta decay experiment; testing the recent claim of observation of 0vββ 1; and performing a direct search for light WIMPs (3-10 GeV/c2).
Atmospheric aerosols affect the global energy budget by scattering and absorbing sunlight (direct effects) and by changing the microphysical structure, lifetime, and coverage of clouds (indirect ...effects). Both aerosol direct and indirect effects are affected by the vertical distribution of aerosols in the atmosphere, which is further influenced by a range of processes, such as aerosol dynamics, long-range transport, and entrainment. However, many observations of these processes are based on ground measurements, limiting our ability to understand the vertical distribution of aerosols and simulate their impact on clouds and climate. In this work, we examined the vertical heterogeneity of aerosols over the Atmospheric Radiation Measurement (ARM) Southern Great Plains (SGP) using data collected from the Holistic Interactions of Shallow Clouds, Aerosols and Land Ecosystems (HI-SCALE) campaign. The vertical profiles of meteorological and aerosol physiochemical properties up to 2500 m above are examined based on the 38 flights conducted during the HI-SCALE campaign.
We perform a full amplitude analysis of the process e+e−→J/ψDD¯, where D refers to either D0 or D+. A new charmoniumlike state X*(3860) that decays to DD¯ is observed with a significance of 6.5σ. Its ...mass is (3862−32+26 −13+40) MeV/c2, and its width is (201−67+154 −82+88) MeV. The JPC=0++ hypothesis is favored over the 2++ hypothesis at the level of 2.5σ. The analysis is based on the 980 fb−1 data sample collected by the Belle detector at the asymmetric-energy e+e− collider KEKB.
The dark photon A^{'} and the dark Higgs boson h^{'} are hypothetical constituents featured in a number of recently proposed dark sector models. Assuming prompt decays of both dark particles, we ...search for their production in the so-called Higgstrahlung channel e^{+}e^{-}→A^{'}h^{'}, with h^{'}→A^{'}A^{'}. We investigate ten exclusive final states with A^{'}→e^{+}e^{-}, μ^{+}μ^{-}, or π^{+}π^{-} in the mass ranges 0.1 GeV/c^{2} <m_{A^{'}}<3.5 GeV/c^{2} and 0.2 GeV/c^{2} <m_{h^{'}}<10.5 GeV/c^{2}. We also investigate three inclusive final states 2(e^{+}e^{-})X, 2(μ^{+}μ^{-})X, and (e^{+}e^{-})(μ^{+}μ^{-})X, where X denotes a dark photon candidate detected via missing mass, in the mass ranges 1.1 GeV/c^{2} <m_{A^{'}}<3.5 GeV/c^{2} and 2.2 GeV/c^{2} <m_{h^{'}}<10.5 GeV/c^{2}. Using the entire 977 fb^{-1} data set collected by Belle, we observe no significant signal. We obtain individual and combined 90% credibility level upper limits on the branching fraction times the Born cross section, B×σ_{Born}, on the Born cross section σ_{Born}, and on the dark photon coupling to the dark Higgs boson times the kinetic mixing between the standard model photon and the dark photon, α_{D}×ε^{2}. These limits improve upon and cover wider mass ranges than previous experiments. The limits from the final states 3(π^{+}π^{-}) and 2(e^{+}e^{-})X are the first placed by any experiment. For α_{D} equal to 1/137, m_{h^{'}}< 8 GeV/c^{2}, and m_{A^{'}}<1 GeV/c^{2}, we exclude values of the mixing parameter ε above ∼8×10^{-4}.
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