153 research outputs found

    How long does it take to pull an ideal polymer into a small hole?

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    We present scaling estimates for characteristic times τlin\tau_{\rm lin} and τbr\tau_{\rm br} of pulling ideal linear and randomly branched polymers of NN monomers into a small hole by a force ff. We show that the absorbtion process develops as sequential straightening of folds of the initial polymer configuration. By estimating the typical size of the fold involved into the motion, we arrive at the following predictions: τlin(N)N3/2/f\tau_{\rm lin}(N) \sim N^{3/2}/f and τbr(N)N5/4/f\tau_{\rm br}(N) \sim N^{5/4}/f, and we also confirm them by the molecular dynamics experiment.Comment: 4 pages, 3 figure

    NN potentials from inverse scattering in the J-matrix approach

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    An approximate inverse scattering method [7,8] has been used to construct separable potentials with the Laguerre form factors. As an application, we invert the phase shifts of proton-proton in the 1S0^1S_0 and 3P23F2^3P_2-^3F_2 channels and neutron-proton in the 3S13D1^3S_1-^3D_1 channel elastic scattering. In the latter case the deuteron wave function of a realistic npnp potential was used as input.Comment: LaTex2e, 17 pages, 3 Postscript figures; corrected typo

    Radiation-induced hydrogen transfer in metals

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    The paper presents processes of hydrogen (deuterium) diffusion and release from hydrogen-saturated condensed matters in atomic, molecular and ionized states under the influence of the electron beam and X-ray radiation in the pre-threshold region. The dependence is described between the hydrogen isotope release intensity and the current density and the electron beam energy affecting sample, hydrogen concentration in the material volume and time of radiation exposure to the sample. The energy distribution of the emitted positive ions of hydrogen isotopes is investigated herein. Mechanisms of radiation-induced hydrogen transfer in condensed matters are suggested

    Nucleon-nucleon interaction in the JJ-matrix inverse scattering approach and few-nucleon systems

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    The nucleon-nucleon interaction is constructed by means of the JJ-matrix version of inverse scattering theory. Ambiguities of the interaction are eliminated by postulating tridiagonal and quasi-tridiagonal forms of the potential matrix in the oscillator basis in uncoupled and coupled waves, respectively. The obtained interaction is very accurate in reproducing the NNNN scattering data and deuteron properties. The interaction is used in the no-core shell model calculations of 3^3H and 4^4He nuclei. The resulting binding energies of 3^3H and 4^4He are very close to experimental values.Comment: Text is revised, new figures and references adde

    Critical exponents for random knots

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    The size of a zero thickness (no excluded volume) polymer ring is shown to scale with chain length NN in the same way as the size of the excluded volume (self-avoiding) linear polymer, as NνN^{\nu}, where ν0.588\nu \approx 0.588. The consequences of that fact are examined, including sizes of trivial and non-trivial knots.Comment: 4 pages, 0 figure

    Kinetics of stochastically-gated diffusion-limited reactions and geometry of random walk trajectories

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    In this paper we study the kinetics of diffusion-limited, pseudo-first-order A + B -> B reactions in situations in which the particles' intrinsic reactivities vary randomly in time. That is, we suppose that the particles are bearing "gates" which interchange randomly and independently of each other between two states - an active state, when the reaction may take place, and a blocked state, when the reaction is completly inhibited. We consider four different models, such that the A particle can be either mobile or immobile, gated or ungated, as well as ungated or gated B particles can be fixed at random positions or move randomly. All models are formulated on a dd-dimensional regular lattice and we suppose that the mobile species perform independent, homogeneous, discrete-time lattice random walks. The model involving a single, immobile, ungated target A and a concentration of mobile, gated B particles is solved exactly. For the remaining three models we determine exactly, in form of rigorous lower and upper bounds, the large-N asymptotical behavior of the A particle survival probability. We also realize that for all four models studied here such a probalibity can be interpreted as the moment generating function of some functionals of random walk trajectories, such as, e.g., the number of self-intersections, the number of sites visited exactly a given number of times, "residence time" on a random array of lattice sites and etc. Our results thus apply to the asymptotical behavior of the corresponding generating functions which has not been known as yet.Comment: Latex, 45 pages, 5 ps-figures, submitted to PR

    Epidemiological features Delta together multiple infection in Saint-Petersburg

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    Studied the epidemiological features of the delta as a coinfection of hepatitis B in Saint-Petersburg for 14-year period (2002–2014). Clinical and laboratory data of 232 patients admitted to Botkin CIB them during this period. Revealed a 2-fold increase in performance of co-infection (Br + + IOP HIV) by 2014. In 49,6% of patients (group 1) were diagnosed less often chronic and acute forms of HBV in combination with delta infection. In 24,5% of cases (group 2) delta infection is associated with chronic hepatitis B and C. In the remaining 25,9% of the cases (B group) occurred multiple infection(HBV + HCV + HIV + IOP). Based on the clinical and epidemiological and laboratory data in 75,8% of patients defined delta superinfection, at 24,2% – co-infection. The marked increase in co-delta infection in recent years due to the accumulation of the potential epidemic of chronic hepatitis B in the population and the increase in the number of imported cases from 8,8% to 37,2% of migrants in the city. Cytolytic components, characterized by higher rates of ALT activity was most pronounced in the first group and the third group is minimal. However, the mean activity values for patients of the 3rd group were higher than in the first. ACAT groups had the same tendency as AlAt. Patients third group was a higher mortality, compared with other groups
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