[PDF] Top 20 Braz. J. Phys. vol.38 número4
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Braz. J. Phys. vol.38 número4
... meanwhile in the model type II the same symmetry forbids terms proportional to ξ D,0 i j , η U,0 i j , ξ E,0 i j . On the other hand, we are considering the 2HDM-III in a basis where only one Higgs ... See full document
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Braz. J. Phys. vol.38 número4
... Inspired in the Flory’s free enegy model of an ideal poly- mer, we propose an alternative model to treat the cosmological constant problem. The basic hypothesis of the model are: i) The [r] ... See full document
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Braz. J. Phys. vol.38 número4
... As an application of the proposed formulation, it is an- alyzed the uncoupled multiparameter chaos control method applied to the H´enon and to the Ikeda maps using two con- trol paramete[r] ... See full document
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Braz. J. Phys. vol.38 número4
... The critical velocity can be found by sending a soliton with different initial speed and observing the final situation after the interaction (falling back or getting over the potential).[r] ... See full document
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Braz. J. Phys. vol.38 número4
... 8: Peak value and wave vector where transmission peak occurs as function of ratio between force constant binding to a fixed sub- strate and inter-atomic force constant.... 9: Mono-atomic[r] ... See full document
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Braz. J. Phys. vol.38 número4
... 3 we apply the model to study some aspects of pp / pp collisions, namely, overall multiplicity distributions, the range of impact parameters for multiple collisions of partons and the av[r] ... See full document
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Braz. J. Phys. vol.38 número4
... However, in this study indicates existence of an insulator layer (GaN) because the behavior of ideality factor and double Gaussian distribution of barrier height has been attributed insu[r] ... See full document
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Braz. J. Phys. vol.38 número4
... type II string cosmological models which represent geometri- cal and massive strings. Banerjee et al [7] investigated some cosmological solutions of massive strings for Bianchi type I sp[r] ... See full document
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Braz. J. Phys. vol.38 número4
... We begin by evalu- ating the Casimir pressure between two plates in a M 4 × S 1 manifold, and then use an appropriate statistical analysis in order to compare the theoretical expression [r] ... See full document
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Braz. J. Phys. vol.38 número4
... A first optimization of the power output, the efficiency and ecological function of an irreversible Carnot cycle, with respect to: internal temperature ratio, time ratio for the heat exc[r] ... See full document
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Braz. J. Phys. vol.38 número4
... The authors are indebted to various experimental groups, in particular, Prof. Margret D. Wilson, Prof. K. Na- gashima, Miss. Aoi Inoue and Prof. J. H. King for providing the data. The SOHO/LASCO data used here are ... See full document
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Braz. J. Phys. vol.38 número4
... potential versus the radial coordinate r. Then the expres- sion of potential energy ε(r) involves both a repulsive term ( j = 1) and an attractive term ( j = 2). Our calculations show that the DE potential ... See full document
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Braz. J. Phys. vol.38 número4
... Effect of gamma irradiation on optical absorption of nuclear track detectors like CR-39 was studied in differ- ent absorbed doses using ultraviolet-visible (UV-VIS) spectroscopy.. The ex[r] ... See full document
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Braz. J. Phys. vol.38 número4
... strength J = 50 MHz ≈ 33 neV, which is a common order of magnitude for magnetic dipolar interactions in proposals such as fullerene- based electron spin quantum computers [20, ...for J = 50 MHz, is ... See full document
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Braz. J. Phys. vol.38 número4
... Therefore, we have an interesting situation where we can study differ- ent properties of naked singularities and wormholes together through the effective potential diagrams and geodesics[r] ... See full document
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Braz. J. Phys. vol.38 número3B
... cross section of the reaction γ + p → J/Ψ+X(M ≤ 1.6 GeV). KMR calculation is simpler in as much as they consider just the elastic hard slope. In our opinion there is a gap between the sophistication of KMR soft ... See full document
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Braz. J. Phys. vol.38 número3A
... Although AZO film can obtain a good texture surface by diluted hydrochloric acid, the etching process and surface morphology are difficult to control due to the high etching rate even if[r] ... See full document
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Braz. J. Phys. vol.38 número3B
... [5] R. J. Furnstahl, T. Hatsuda, and S. H. Lee, Phys. Rev. D 42, 1744 (1990); C. Adami, T. Hatsuda, and I. Zahed, Phys. Rev. D 43, 921 (1991); C. Adami and I. Zahed, Phys. Rev. D 45, 4312 ... See full document
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Braz. J. Phys. vol.38 número3A
... [21] measured similar values of hardness and elastic modulus, as here reported, by using the same instrumented indentation technique for the ab -plane of melt-textured YBCO. Comparing th[r] ... See full document
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Braz. J. Phys. vol.38 número3B
... 5: The impact parameter dependence of prompt photon az- imuthal asymmetry, for q+Pb (at α = 1), p+Pb and Pb+Pb collisions for RHIC energy at midrapidities, with the Woods-Saxon (WS) nu- [r] ... See full document
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