3 research outputs found
Dispersive analysis of K_{L mu3} and K_{L e3} scalar and vector form factors using KTeV data
Using the published KTeV samples of K_L --> pi^{\pm} e^{\mp} nu and K_L -->
pi^{\pm} mu^{\mp} nu decays [1], we perform a reanalysis of the scalar and
vector form factors based on the dispersive parameterization [2,3]. We obtain
phase space integrals I^e_K = 0.15446 \pm 0.00025 and I^{mu}_K = 0.10219 \pm
0.00025. For the scalar form factor parameterization, the only free parameter
is the normalized form factor value at the Callan-Treiman point (C); our best
fit results in ln C = 0.1915 \pm 0.0122. We also study the sensitivity of C to
different parametrizations of the vector form factor. The results for the phase
space integrals and C are then used to make tests of the Standard Model.
Finally, we compare our results with lattice QCD calculations of F_K/F_pi and
f_+(0).Comment: 9 pages, 3 figures, to be published in PR
Search for Lepton Flavor Violating Decays of the Neutral Kaon
The Fermilab KTeV experiment has searched for lepton flavor violating decays
of the KL meson in three decay modes. We observe no events in the signal region
for any of the modes studied, and we set the following upper limits for their
branching ratios at the 90% CL: BR(KL--> pi0 mu e)
pi0 pi0 mu e) mu e) < 3.59 x 10^{-10).Comment: 5 pages, 4 figure
Ultra low friction coefficient in sliding of Si3N4-Al2O3. Effects of applied load, sliding velocity and test temperature.
Foram realizados ensaios tribológicos de deslizamento do par Si3N4-Al2O3, lubrificado com água, na configuração esfera contra disco, sendo a esfera de nitreto de silÃcio e o disco de alumina para investigar a influência da velocidade de deslizamento, da carga aplicada e da temperatura no coeficiente de atrito. As esferas de nitreto de silÃcio e os discos de alumina foram caracterizados determinando-se: densidades, dureza Vickers, módulo de elasticidade e tenacidade à fratura. Os ensaios foram realizados com rugosidade inicial nos discos de Rrms = 352 nm. O regime de ultra baixo coeficiente de atrito (UBCA, μ < 0,01) foi atingido após um perÃodo de running-in de aproximadamente uma hora e o coeficiente de atrito ficou na faixa de μ = 0,008 a μ = 0,002. Os resultados mostraram que este sistema deslizante tem caracterÃsticas hidrodinâmicas, pois o coeficiente de atrito diminuiu com o aumento da velocidade de deslizamento. Uma variação suave da carga aplicada fez com que o coeficiente de atrito permanecesse no regime de UBCA, com a carga aplicada variando de 54 N até 94 N. Em temperaturas menores ou iguais a 11°C o sistema não atingiu o regime de UBCA e o coeficiente de atrito final ficou da ordem de centésimos. Foi observado o fenômeno de UBCA em temperaturas de 30 e 40°C. No entanto, nestas temperaturas, a baixa viscosidade da água não deveria permitir que o sistema atingisse o regime de UBCA. A análise dos dados possibilitou inferir que durante o regime de UBCA o sistema desliza num regime de lubrificação mista, sendo lubrificação hidrodinâmica, devido ao filme de água, somada a lubrificação limite, devido à s camadas hidratadas formadas nas superfÃcies das cerâmicas. Os resultados mostraram que a temperatura influencia no desgaste das cerâmicas. A determinação do volume desgastado possibilitou observar que durante os ensaios a alumina sofre menos desgaste que o nitreto de silÃcio e que o desgaste de ambas cerâmicas aumenta com o aumento da temperatura.Tribological tests were conducted in a ball on disk setup, using water as lubricant. Were used a silicon nitride ball and alumina disk. The tests were conducted to investigate the effects of sliding speed, applied load and temperature on friction coefficient. The silicon nitride balls and alumina disks were characterized by determining density, Vickers hardness, elastic modulus and fracture toughness. The tests were conducted with initial roughness on the disk surface of 352 nm. The ultra low friction coefficient regime (ULFC, μ < 0.01) was reached after a running-in period of approximately one hour and the friction coefficient remains in the range of μ = 0.008 a μ = 0.002 during this steady state regime. The results showed that this sliding system has hydrodynamic characteristics, because the friction coefficient decreased with increasing of the sliding speed. With an smooth variation of the applied load the system remained in the ULFC regime, when the applied load varied from 54 N up to 94 N. At temperatures below or equal to 11°C the system did not reach the ULFC regime and the final friction coefficient was the order of hundredths. We observed the ULFC phenomenon at temperatures of 30 and 40°C. However, at these temperatures, the water viscosity is low and should not allow the system to reach the ULFC regime. The data analysis allowed infer that during the ULFC regime the system slides with a mixed lubrication regime, hydrodynamic plus limitrofe, the first due to water film and the second due to the hydrated layer formed on the ceramics surfaces. The results showed a influences of temperature in the ceramics wear. The results of the worn volume allowed to observe that during the tests alumina suffers less wear than the silicon nitride, and the ceramics wear increases with increasing temperature