Estudo das propriedades críticas do processo epidêmico por par com difusão de pares

The pair contact process - PCP is a nonequilibrium stochastic model which, like the basic contact process - CP, exhibits a phase transition to an absorbing state. While the absorbing state CP corresponds to a unique configuration (empty lattice), the PCP process infinitely many. Numerical and theoretical studies, nevertheless, indicate that the PCP belongs to the same universality class as the CP (direct percolation class), but with anomalies in the critical spreading dynamics. An infinite number of absorbing configurations arise in the PCP because all process (creation and annihilation) require a nearest-neighbor pair of particles. The diffusive pair contact process - PCPD) was proposed by Grassberger in 1982. But the interest in the problem follows its rediscovery by the Langevin description. On the basis of numerical results and renormalization group arguments, Carlon, Henkel and Schollwöck (2001), suggested that certain critical exponents in the PCPD had values similar to those of the party-conserving - PC class. On the other hand, Hinrichsen (2001), reported simulation results inconsistent with the PC class, and proposed that the PCPD belongs to a new universality class. The controversy regarding the universality of the PCPD remains unresolved. In the PCPD, a nearest-neighbor pair of particles is necessary for the process of creation and annihilation, but the particles to diffuse individually. In this work we study the PCPD with diffusion of pair, in which isolated particles cannot move; a nearest-neighbor pair diffuses as a unit. Using quasistationary simulation, we determined with good precision the critical point and critical exponents for three values of the diffusive probability: D=0.5 and D=0.1. For D=0.5: PC=0.89007(3), β/v=0.252(9), z=1.573(1), =1.10(2), m=1.1758(24). For D=0.1: PC=0.9172(1), β/v=0.252(9), z=1.579(11), =1.11(4), m=1.173(4)

Relação entre função sexual, sintomatologia depressiva e qualidade de vida em mulheres grávidas

INTRODUCTION: Human sexuality is recognized as one of the pillars of quality of life. In women, sexual function is influenced throughout life by many factors that can lead to the appearance of changes in the cycle of sexual response, and hence the quality of life (QOL). Pregnancy is a period of change, leaving them physically and mentally vulnerable, which may affect sexual function and quality of life during pregnancy. OBJECTIVE: To investigate the relationship between sexual function, presence of depressive symptoms and quality of life in pregnant women. METHODS: The study included 207 pregnant women attending prenatal examination of the Maternity Divine Love, Parnamirim / RN and the participants of the Course for Pregnant Women of the Department of Physical Therapy at UFRN (central campus). Initially it was applied, a questionnaire containing questions about sociodemographic, gynecological and obstetric data, as well as body and sexual self-knowledge. Sexual function was assessed using the Sexual Function Index Female (Female Sexual Function Index - FSFI). To assess the quality of life, we used the Quality Index Ferrans Life & Powers mom. The presence of depressive symptoms was verified by applying the Beck Depression Inventory. The Shapiro-Wilk test for normality was carried variables, Mann-Whitney test for carrying out the comparisons and the Wilcoxon test for comparing the monthly sexual frequency before and during pregnancy. Multiple linear regression was used to verify the relationship between sexual function, depressive symptoms and quality of life. We used the Spearman correlation to check correlation between the variables. Ap value <0.05 was adopted. RESULTS: Sexual function and depressive symptoms were related quality of life (R2 = 0.30, p <0.001). Depression had a moderate negative correlation with quality of life (0.53; p <0.001), whereas sexual function showed a positive correlation with low quality of life (0.22; p = 0.001). The planning of pregnancy, education and income shown to influence depression scores. With respect to sexual function, it was seen that during pregnancy, a reduction in the monthly frequency of sexual partner (Z = -10.56; p <0.001). Among the sexual domain, just the pain, showed a statistically significant difference compared between the second and third quarter (Z = -1.91, p <0.05). The score of the quality of life of women with sexual dysfunction was xvii significantly lower than that pregnant women without dysfunction (Z = -2.87, p = 0.004). Conclusion: Sexual function and the presence of depressive symptoms are related to the quality of life of pregnant women.

Estudo das propriedades críticas do processo epidêmico por par com difusão de pares

The pair contact process - PCP is a nonequilibrium stochastic model which, like the basic contact process - CP, exhibits a phase transition to an absorbing state. While the absorbing state CP corresponds to a unique configuration (empty lattice), the PCP process infinitely many. Numerical and theoretical studies, nevertheless, indicate that the PCP belongs to the same universality class as the CP (direct percolation class), but with anomalies in the critical spreading dynamics. An infinite number of absorbing configurations arise in the PCP because all process (creation and annihilation) require a nearest-neighbor pair of particles. The diffusive pair contact process - PCPD) was proposed by Grassberger in 1982. But the interest in the problem follows its rediscovery by the Langevin description. On the basis of numerical results and renormalization group arguments, Carlon, Henkel and Schollwöck (2001), suggested that certain critical exponents in the PCPD had values similar to those of the party-conserving - PC class. On the other hand, Hinrichsen (2001), reported simulation results inconsistent with the PC class, and proposed that the PCPD belongs to a new universality class. The controversy regarding the universality of the PCPD remains unresolved. In the PCPD, a nearest-neighbor pair of particles is necessary for the process of creation and annihilation, but the particles to diffuse individually. In this work we study the PCPD with diffusion of pair, in which isolated particles cannot move; a nearest-neighbor pair diffuses as a unit. Using quasistationary simulation, we determined with good precision the critical point and critical exponents for three values of the diffusive probability: D=0.5 and D=0.1. For D=0.5: PC=0.89007(3), β/v=0.252(9), z=1.573(1), =1.10(2), m=1.1758(24). For D=0.1: PC=0.9172(1), β/v=0.252(9), z=1.579(11), =1.11(4), m=1.173(4)