Avaliação físico-química de águas minerais comercializadas na região de Campinas, SP

Com o objetivo de avaliar a qualidade de águas minerais, foram analisadas amostras, adquiridas em supermercados, de oito fontes localizadas no Estado de São Paulo entre agosto de 1999 e maio de 2000, com coletas trimestrais. Os resultados das análises físico-químicas mostraram que as amostras possuíam, em sua maioria, composição química dentro dos limites permitidos pela legislação brasileira, exceto quatro amostras, que apresentaram resultados na análise de cor acima de 5 unidades PtCo, uma amostra com pH fora da faixa recomendada de 4,0 a 9,0 e uma amostra com alcalinidade em hidróxidos em duas épocas de análise. Os resultados obtidos para as diferentes amostras variaram de acordo com as seguintes faixas: pH de 6,39 a 9,92, alcalinidade de 0,0 a 189,1mg L-1 de bicarbonato, dureza de 0,00 a 136,00mg L-1 de carbonato de cálcio, cor de 0,0 a 9,0 unidades de PtCo, turbidez de 0,00 a 2,00 FTU de turvação, sulfato de 0,00 a 55,67mg L-1, sulfeto de 0,00 a 0,002mg L-1, cloreto de 0,00 a 23,53mg L-1, fluoreto de 0,02 a 0,8mg L-1, alumínio de 0,01 a 0,09mg L-1, bário de 0,00 a 0,26mg L-1, cálcio de 0,53 a 28,35mg L-1, crômio de 0,00 a 0,01mg L-1, ferro de 0,00 a 0,03mg L-1, potássio de 0,39 a 3,27mg L-1, sódio de 0,53 a 97,29mg L-1, magnésio de 0,00 a 9,10mg L-1, manganês de 0,00 a 0,05mg L-1, zinco de 0,00 a 0,03mg L-1, chumbo de 0,00 a 0,01mg L-1 e lítio de 0,00 a 0,02mg L-1. Os elementos cádmio, cobre e cobalto apresentaram-se abaixo dos limites de detecção dos métodos

Total and differential cross sections of η-production in proton–deuteron fusion for excess energies between Qη = 13 MeV and Qη = 81 MeV

New data on both total and differential cross sections of the production of η mesons in proton–deuteron fusion to He3η in the excess energy region 13.6MeV≤Qη≤80.9MeV are presented. These data have been obtained with the WASA-at-COSY detector setup located at the Forschungszentrum Jülich, using a proton beam at 15 different beam momenta between pp=1.60GeV/c and pp=1.74GeV/c. While significant structure of the total cross section is observed in the energy region 20MeV≲Qη≲60MeV, a previously reported sharp variation around Qη≈50MeV cannot be confirmed. Angular distributions show the typical forward-peaking that was noted earlier. For the first time, it is possible to study the development of these angular distributions with rising excess energy over a wide interval

Importance of d-wave contributions in the charge symmetry breaking reaction dd -> He-4 pi(0)

This letter reports a first quantitative analysis of the contribution of higher partial waves in the charge symmetry breaking reaction dd -> He-4 pi(0) using the WASA-at-COSY detector setup at an excess energy of Q = 60 MeV. The determined differential cross section can be parametrized as d sigma/d Omega = a + b cos(2) theta*, where theta* is the production angle of the pion in the center-of-mass coordinate system, and the results for the parameters are a = (1.55 +/- 0.46(stat)(-0.8)(+0.32)(syst)) pb/sr and b = (13.1 +/- 2.1(stat)(-2.7)(+1.0)(syst)) pb/sr. The data are compatible with vanishing p-waves and a sizable d-wave contribution. This finding should strongly constrain the contribution of the A isobar to the dd -> He-4 pi(0) reaction and is, therefore, crucial for a quantitative understanding of quark mass effects in nuclear production reactions. (C) 2018 The Author(s). Published by Elsevier B.V

Isotensor Dibaryon in the pp →ppπ+π- Reaction?

Exclusive measurements of the quasifree pp→ppπ+π- reaction have been carried out at WASA@COSY by means of pd collisions at Tp=1.2 GeV. Total and differential cross sections have been extracted covering the energy region Tp=1.08-1.36 GeV, which is the region of N∗(1440) and Δ(1232)Δ(1232) resonance excitations. Calculations describing these excitations by t-channel meson exchange are at variance with the measured differential cross sections and underpredict substantially the experimental total cross section. An isotensor ΔN dibaryon resonance with I(JP)=2(1+) produced associatedly with a pion is able to overcome these deficiencies