Properties of l=1 B-1 and B*(2) Mesons

This Letter presents the first strong evidence for the resolution of the excited B mesons B-1 and B-2(*) as two separate states in fully reconstructed decays to B+(*())pi(-). The mass of B-1 is measured to be 5720.6 +/- 2.4 +/- 1.4 MeV/c(2) and the mass difference Delta M between B-2* and B-1 is 26.2 +/- 3.1 +/- 0: 9 MeV/c(2), giving the mass of the B-2* as 5746.8 +/- 2.4 +/- 1.7 MeV/c(2). The production rate for B-1 and B-2* mesons is determined to be a fraction (13.9 +/- 1.9 +/- 3.2)% of the production rate of the B+ meson.

Study of Z Boson Production in PbPb Collisions at root s(NN)=2.76 TeV

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

Search for a Vectorlike Quark with Charge 2/3 in t plus Z Events from pp Collisions at root s 7 TeV

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

Self-assembly of cyclometallated Pd(II) compounds directed by C-H center dot center dot center dot pi interactions: A structural evidence for metalloaromaticity in a cyclopalladated ring

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

Cryopreservation at-80A degrees C of Agaricus blazei on rice grains

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Methyl- and phenylmercury(II) derivatives of 2-mercaptobenzothiazole. Crystal structure of (2-mercaptobenzothiazolato)methylmercury(II)

The complexes MeHgL and PhHgL (HL = 2-mercaptobenzothiazole) have been obtained from the reaction of the ligand with methylmercury hydroxide and phenylmercury acetate, respectively, in methanol. MeHgL, which has been characterized by single-crystal X-ray diffraction analysis (crystal data: triclinic, space group P1, with a = 8.009 (4) Å, b = 10.042 (4) Å, c = 13.074 (3) Å, α = 101.25 (2)°, β = 102.61(3)°, γ = 101.42 (3)°, R = 0.067), crystallizes with two independent molecules, I and I′, contained in each asymmetric unit with a coordination geometry based on the almost linear C-Hg-S group (Hg-S = 2.369 (6) Å, Hg-C = 2.06 (2) Å, and C-Hg-S = 177.7 (7)° for I; Hg-S = 2.375 (6) Å, Hg-C = 2.10 (3) Å, and C-Hg-S = 178.8 (6)° for I′). A secondary intramolecular interaction between the mercury atom and the C=N group of the ring and some weak intermolecular interactions between the metal and sulfur atoms were also found. The vibrational spectra of this compound and the phenylmercury(II) compound are discussed in light of the crystal structure. Diagnostic criteria of the bonding modes for the ligand are assessed. © 1985 American Chemical Society.

Evidence for 2.35 to 2.30 Ga juvenile crustal growth in the northwest Borborema Province, NE Brazil

The c. 600 Ma Brasiliano Borborema Province of NE Brazil comprises a complex collage of Precambrian crustal blocks cut by a series of continental-scale shear zones. The predominant basement rocks in the province are 2.1-2.0 Ga Transamazonian gneisses of both juvenile and reworked nature. U-Pb zircon and Sm-Nd whole-rock studies of tonalite-trondhjemite-granodiorite basement gneisses in the NW Ceará or Médio Coreaú domain in the northwestern part of the Borborema Province indicate that this represents a continental fragment formed by 2.35-2.30 Ga juvenile crust. This block has no apparent genetic affinity with any other basement gneisses in the Borborema Province, and it does not represent the tectonized margin of the c. 2.1-2.0 Ga São Luis Craton to the NW. The petrological and geochemical characteristics, as well as the Nd-isotopic signatures of these gneisses, are consistent with their genesis in an island arc setting. This finding documents a period of crustal growth during a period of the Earth's history which is known for its tectonic quiescence and paucity of crust formation. © Geological Society of London 2009.

Measurement of the elliptic anisotropy of charged particles produced in PbPb collisions at √sNN=2.76 TeV

The anisotropy of the azimuthal distributions of charged particles produced in √sNN=2.76 TeV PbPb collisions is studied with the CMS experiment at the LHC. The elliptic anisotropy parameter, v2, defined as the second coefficient in a Fourier expansion of the particle invariant yields, is extracted using the event-plane method, two- and four-particle cumulants, and Lee-Yang zeros. The anisotropy is presented as a function of transverse momentum (pT), pseudorapidity (η) over a broad kinematic range, 0.3<pT<20 GeV/c, |η|<2.4, and in 12 classes of collision centrality from 0 to 80%. The results are compared to those obtained at lower center-of-mass energies, and various scaling behaviors are examined. When scaled by the geometric eccentricity of the collision zone, the elliptic anisotropy is found to obey a universal scaling with the transverse particle density for different collision systems and center-of-mass energies. © 2013 CERN. Published by the American Physical Society under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.

Cytotoxic non-aromatic B-ring flavanones from Piper carniconnectivum C. DC.

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Stress distribution on dentin-cement-post interface varying root canal and glass fiber post diameters. A three-dimensional finite element analysis based on micro-C data

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

STOCHASTIC ADDING MACHINE AND 2-DIMENSIONAL JULIA SETS

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

Unusual C,O-fused glycosylapigenins from Serjania marginata leaves

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Vitamin C prevents the effects of high rearing temperatures on the quality of broiler thigh meat

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

In Vitro Schistosomicidal Activity of Balsaminol F and Karavilagenin C

Five cucurbitane-type triterpenes (1-5), previously isolated from the African medicinal plant Momordica balsamina, along with five ester derivatives (6-10) of karavilagenin C (2), were evaluated for their potential schistosomicidal activity against Schistosoma mansoni adult worms. The natural compounds were isolated from the ethyl acetate-soluble fraction of the methanol extract of the aerial parts of M. balsamina. In a preliminary study, a significant schistosomicidal activity was observed for both the crude methanol extract and the ethyl acetate fraction. The compounds responsible for the activity were found to be balsaminol F (1) and karavilagenin C (2) with LC50 values of 14.7 +/- 1.5 and 28.9 +/- 1.8 mu M, respectively, after 24 h of incubation (positive control praziquantel, LC50 = 1.2 +/- 0.1 mu M). Both compounds (1, 2), at 10-50 mu M, induced significant reductions in the motor activity of the worms and significantly decreased the egg production. Furthermore, they were able (at 10-100 mu M) to separate the adult worm pairs into male and female after 24 h. Compounds 3-5, bearing a sugar moiety as a substituent, and the acylated derivatives of karavilagenin C (6-10) were inactive, suggesting that the presence of free hydroxyl groups in the tetracyclic skeleton might be important for the activity. A correlation between activity and the molecular volume/weight of compounds was also found.

Formfaktor-Bestimmung des semileptonischen K +- pi 0 my +- ny-Zerfalls mit dem NA48/2-Experiment

Der semileptonische Zerfall K^±→π^0 μ^± υ ist ein geeigneter Kanal zur Be-stimmung des CKM-Matrixelementes 〖|V〗_us |. Das hadronische Matrixelement dieses Zerfalls wird durch zwei dimensionslose Formfaktoren f_± (t) beschrieben. Diese sind abhängig vom Impulsübertrag t=〖(p_K-p_π)〗^2 auf das Leptonpaar. Zur Bestimmung von 〖|V〗_us | dienen die Formfaktoren als wichtige Parameter zur Berechnung des Phasenraumintegrals dieses Zerfalls. Eine präzise Messung der Formfaktoren ist zusätzlich dadurch motiviert, dass das Resultat des NA48-Experimentes von den übrigen Messungen der Experimente KLOE, KTeV und ISTRA+ abweicht. Die Daten einer Messperiode des NA48/2 -Experimentes mit offenem Trigger aus dem Jahre 2004 wurden analysiert. Daraus wählte ich 1.8 Millionen K_μ3^±-Zerfallskandidaten mit einem Untergrundanteil von weniger als 0.1% aus. Zur Bestimmung der Formfaktoren diente die zweidimensionale Dalitz-Verteilung der Daten, nachdem sie auf Akzeptanz des Detektors und auf radiative Effekte korrigiert war. An diese Verteilung wurde die theoretische Parameter-abhängige Funktion mit einer Chiquadrat-Methode angepasst. Es ergeben sich für quadratische, Pol- und dispersive Parametrisierung folgende Formfaktoren: λ_0=(14.82±〖1.67〗_stat±〖0.62〗_sys )×〖10〗^(-3) λ_+^'=(25.53±〖3.51〗_stat±〖1.90〗_sys )×〖10〗^(-3) λ_+^''=( 1.40±〖1.30〗_stat±〖0.48〗_sys )×〖10〗^(-3) m_S=1204.8±〖32.0〗_stat±〖11.4〗_(sys ) MeV/c^2 m_V=(877.4±〖11.1〗_stat±〖11.2〗_(sys ) MeV/c^2 LnC=0.1871±〖0.0088〗_stat±〖0.0031〗_(sys )±=〖0.0056〗_ext Λ_+=(25.42±〖0.73〗_stat±〖0.73〗_(sys )±=〖1.52〗_ext )×〖10〗^(-3) Die Resultate stimmen mit den Messungen der Experimente KLOE, KTeV und ISTRA+ gut überein, und ermöglichen eine Verbesserung des globalen Fits der Formfaktoren. Mit Hilfe der dispersiven Parametrisierung der Formfaktoren, unter Verwendung des Callan-Treiman-Theorems, ist es möglich, einen Wert für f_± (0) zu bestimmen. Das Resultat lautet: f_+ (0)=0.987±〖0.011〗_(NA48/2)±〖0.008〗_(ext ) Der für f_+ (0) berechnete Wert stimmt im Fehler gut mit den vorherigen Messungen von KTeV, KLOE und ISTRA+ überein, weicht jedoch um knapp zwei Standardabweichungen von der theoretischen Vorhersage ab.