182 research outputs found

    Test of Local Scale Invariance from the direct measurement of the response function in the Ising model quenched to and to below TCT_C

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    In order to check on a recent suggestion that local scale invariance [M.Henkel et al. Phys.Rev.Lett. {\bf 87}, 265701 (2001)] might hold when the dynamics is of Gaussian nature, we have carried out the measurement of the response function in the kinetic Ising model with Glauber dynamics quenched to TCT_C in d=4d=4, where Gaussian behavior is expected to apply, and in the two other cases of the d=2d=2 model quenched to TCT_C and to below TCT_C, where instead deviations from Gaussian behavior are expected to appear. We find that in the d=4d=4 case there is an excellent agreement between the numerical data, the local scale invariance prediction and the analytical Gaussian approximation. No logarithmic corrections are numerically detected. Conversely, in the d=2d=2 cases, both in the quench to TCT_C and to below TCT_C, sizable deviations of the local scale invariance behavior from the numerical data are observed. These results do support the idea that local scale invariance might miss to capture the non Gaussian features of the dynamics. The considerable precision needed for the comparison has been achieved through the use of a fast new algorithm for the measurement of the response function without applying the external field. From these high quality data we obtain a=0.27±0.002a=0.27 \pm 0.002 for the scaling exponent of the response function in the d=2d=2 Ising model quenched to below TCT_C, in agreement with previous results.Comment: 24 pages, 6 figures. Resubmitted version with improved discussions and figure

    Luteal dynamics in goats: morphological and endocrine features.

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    Abstract: The aim of this study was to establish the morphologic and endocrine characteristics of luteal dynamics in goats. It was used Toggenburg female goats that showed natural estrus in a 48-hour interval. After estrus, ultrasonographic evaluations of the ovaries were daily performed during 21 days using a portable device (5MHz probe). Blood sample was collected for plasma progresterone (P4) determination. Corpora lutea were detected for the first time on day 5 and progressively increased in size until D9 (1.26 ± 0.08 cm2), with no variation on subsequent days. In females with one ovulation, the first visualization of the corpora lutea was earlier than in those with multiple ovulation (4.54 ± 0.18 vs 5.74 ± 0.25 days). At the moment of the first visualization, luteal area was smaller in animals with single ovulation. Plasma P4 concentration progressively increased until day 9 and it did not show significant increase until luteolysis, characterized by a sharp decrease in P4 concentration, reaching values below 1 ng/mL in 24 hours. The luteal area slowly and gradually decreased in size. It was observed a significant positive correlation between P4 concentration and area during luteogenesis and luteolysis (r = 0.63 and r = 0.50, respectively). When corpus luteum reached its maximum size (D9), female with more than one corpora lutea, with a greater luteal tissue area, did not show P4 concentration higher than those with one ovulation (5.92 ± 0.59 vs 7.04 ± 0.79 ng/mL). These results show that luteal dynamics in Toggenbur goats follow a similar pattern to those observed in other goat breeds and luteal tissue growth was positively correlated with corpora lutea functionality. [Dinâmica luteal em caprinos: características morfológicas e endócrinas]. Resumo: Objetivou-se neste estudo estabelecer as características morfológicas e endócrinas da dinâmica luteal em cabras. Foram utilizadas fêmeas da raça Toggenburg que manifestaram estro natural em um intervalo de 48 horas. Após o estro, foram realizadas avaliações ultrassonográficas diárias dos ovários durante 21 dias, utilizando-se um aparelho portátil (5 MHz). Amostras de sangue foram coletadas para dosagem de progesterona (P4) no plasma. Os corpos lúteos foram detectados pela primeira vez no D5 e aumentaram progressivamente de tamanho até o D9 (1,26 ± 0,08 cm2), não havendo variação nos dias subsequentes. Nas fêmeas com uma ovulação, a primeira visualização do corpo lúteo foi mais precoce que naquelas com ovulação múltipla (4,54 ± 0,18 vs 5,74 ± 0,25 dias). No momento da primeira visualização, a área luteal foi menor nos animais com uma ovulação. A concentração plasmática de P4 aumentou progressivamente até o D9 e não apresentou aumento significativo até o momento da luteólise, caracterizada por uma acentuada queda da concentração de P4, atingindo valores inferiores a 1 ng/mL em um intervalo de 24 horas. A área luteal diminuiu de forma lenta e gradual. Foi observada uma correlação positiva significativa entre a área e a concentração de P4 durante a lutegêonese e a luteólise (r = 0,63 e r = 0,50; respectivamente). No dia em que o corpo lúteo atinge sua área máxima (D9), as fêmeas com mais de um corpo lúteo, com maior área de tecido luteal, não apresentaram concentração de P4 superior à daquelas com uma ovulação (5,92 ± 0,59 vs 7,04 ± 0,79 ng/mL). Esses resultados indicam que a dinâmica luteal em caprinos da raça Toggenburg segue padrões semelhantes aos observados em outras raças e em outras espécies e que o crescimento de tecido luteal refletiu positivamente na funcionalidade do corpo lúteo

    Assessment of luteal function in Toggenburg goats by computer-assisted image analysis.

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    Edição dos proceedings da Annual Conference or the International Embryo Transfer Society, San Diego, California, 2009

    On universality in aging ferromagnets

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    This work is a contribution to the study of universality in out-of-equilibrium lattice models undergoing a second-order phase transition at equilibrium. The experimental protocol that we have chosen is the following: the system is prepared in its high-temperature phase and then quenched at the critical temperature TcT_c. We investigated by mean of Monte Carlo simulations two quantities that are believed to take universal values: the exponent λ/z\lambda/z obtained from the decay of autocorrelation functions and the asymptotic value XX_\infty of the fluctuation-dissipation ratio X(t,s)X(t,s). This protocol was applied to the Ising model, the 3-state clock model and the 4-state Potts model on square, triangular and honeycomb lattices and to the Ashkin-Teller model at the point belonging at equilibrium to the 3-state Potts model universality class and to a multispin Ising model and the Baxter-Wu model both belonging to the 4-state Potts model universality class at equilibrium.Comment: 17 page
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