582 research outputs found

    Entropy of chains placed on the square lattice

    Full text link
    We obtain the entropy of flexible linear chains composed of M monomers placed on the square lattice using a transfer matrix approach. An excluded volume interaction is included by considering the chains to be self-and mutually avoiding, and a fraction rho of the sites are occupied by monomers. We solve the problem exactly on stripes of increasing width m and then extrapolate our results to the two-dimensional limit to infinity using finite-size scaling. The extrapolated results for several finite values of M and in the polymer limit M to infinity for the cases where all lattice sites are occupied (rho=1) and for the partially filled case rho<1 are compared with earlier results. These results are exact for dimers (M=2) and full occupation (\rho=1) and derived from series expansions, mean-field like approximations, and transfer matrix calculations for some other cases. For small values of M, as well as for the polymer limit M to infinity, rather precise estimates of the entropy are obtained.Comment: 6 pages, 7 figure

    Silicon spin diffusion transistor: materials, physics and device characteristics

    No full text
    The realisation that eaveryday electronics has ignored the spin of the carrier in favour of its charge is the foundation of the field of spintronics. Starting with simple two-terminal devices based on GMR and tunnel magnetoresistance, the technology has advanced to consider three-terminal devices that aim to combine spin sensitivity with a high current gain and a large current output. These devices require both efficient spin injection and semiconductor fabrication. In this paper, a discussion is presented of the design, operation and characteristics of the only spin transistor that has yielded a current gain greater than one in combination with reasonable output current

    Understanding and engineering beneficial plant–microbe interactions:Plant growth promotion in energy crops

    Get PDF
    Plant production systems globally must be optimized to produce stable high yields from limited land under changing and variable climates. Demands for food, animal feed, and feedstocks for bioenergy and biorefining applications, are increasing with population growth, urbanization and affluence. Low-input, sustainable, alternatives to petrochemical-derived fertilizers and pesticides are required to reduce input costs and maintain or increase yields, with potential biological solutions having an important role to play. In contrast to crops that have been bred for food, many bioenergy crops are largely undomesticated, and so there is an opportunity to harness beneficial plant–microbe relationships which may have been inadvertently lost through intensive crop breeding. Plant–microbe interactions span a wide range of relationships in which one or both of the organisms may have a beneficial, neutral or negative effect on the other partner. A relatively small number of beneficial plant–microbe interactions are well understood and already exploited; however, others remain understudied and represent an untapped reservoir for optimizing plant production. There may be near-term applications for bacterial strains as microbial biopesticides and biofertilizers to increase biomass yield from energy crops grown on land unsuitable for food production. Longer term aims involve the design of synthetic genetic circuits within and between the host and microbes to optimize plant production. A highly exciting prospect is that endosymbionts comprise a unique resource of reduced complexity microbial genomes with adaptive traits of great interest for a wide variety of applications

    Pocket Monte Carlo algorithm for classical doped dimer models

    Full text link
    We study the correlations of classical hardcore dimer models doped with monomers by Monte Carlo simulation. We introduce an efficient cluster algorithm, which is applicable in any dimension, for different lattices and arbitrary doping. We use this algorithm for the dimer model on the square lattice, where a finite density of monomers destroys the critical confinement of the two-monomer problem. The monomers form a two-component plasma located in its high-temperature phase, with the Coulomb interaction screened at finite densities. On the triangular lattice, a single pair of monomers is not confined. The monomer correlations are extremely short-ranged and hardly change with doping.Comment: 6 pages, REVTeX

    Non-linear Dynamics in QED_3 and Non-trivial Infrared Structure

    Get PDF
    In this work we consider a coupled system of Schwinger-Dyson equations for self-energy and vertex functions in QED_3. Using the concept of a semi-amputated vertex function, we manage to decouple the vertex equation and transform it in the infrared into a non-linear differential equation of Emden-Fowler type. Its solution suggests the following picture: in the absence of infrared cut-offs there is only a trivial infrared fixed-point structure in the theory. However, the presence of masses, for either fermions or photons, changes the situation drastically, leading to a mass-dependent non-trivial infrared fixed point. In this picture a dynamical mass for the fermions is found to be generated consistently. The non-linearity of the equations gives rise to highly non-trivial constraints among the mass and effective (`running') gauge coupling, which impose lower and upper bounds on the latter for dynamical mass generation to occur. Possible implications of this to the theory of high-temperature superconductivity are briefly discussed.Comment: 29 pages LATEX, 7 eps figures incorporated, uses axodraw style. Discussion on the massless case (section 2) modified; no effect on conclusions, typos correcte

    Dimer coverings on the Sierpinski gasket with possible vacancies on the outmost vertices

    Full text link
    We present the number of dimers Nd(n)N_d(n) on the Sierpinski gasket SGd(n)SG_d(n) at stage nn with dimension dd equal to two, three, four or five, where one of the outmost vertices is not covered when the number of vertices v(n)v(n) is an odd number. The entropy of absorption of diatomic molecules per site, defined as SSGd=lim⁡n→∞ln⁡Nd(n)/v(n)S_{SG_d}=\lim_{n \to \infty} \ln N_d(n)/v(n), is calculated to be ln⁡(2)/3\ln(2)/3 exactly for SG2(n)SG_2(n). The numbers of dimers on the generalized Sierpinski gasket SGd,b(n)SG_{d,b}(n) with d=2d=2 and b=3,4,5b=3,4,5 are also obtained exactly. Their entropies are equal to ln⁡(6)/7\ln(6)/7, ln⁡(28)/12\ln(28)/12, ln⁡(200)/18\ln(200)/18, respectively. The upper and lower bounds for the entropy are derived in terms of the results at a certain stage for SGd(n)SG_d(n) with d=3,4,5d=3,4,5. As the difference between these bounds converges quickly to zero as the calculated stage increases, the numerical value of SSGdS_{SG_d} with d=3,4,5d=3,4,5 can be evaluated with more than a hundred significant figures accurate.Comment: 35 pages, 20 figures and 1 tabl

    Using process algebra to model radiation induced bystander effects

    Get PDF
    Radiation induced bystander effects are secondary effects caused by the production of chemical signals by cells in response to radiation. We present a Bio-PEPA model which builds on previous modelling work in this field to predict: the surviving fraction of cells in response to radiation, the relative proportion of cell death caused by bystander signalling, the risk of non-lethal damage and the probability of observing bystander signalling for a given dose. This work provides the foundation for modelling bystander effects caused by biologically realistic dose distributions, with implications for cancer therapies

    Scaling analysis of a model Hamiltonian for Ce3+^{3+} impurity in a cubic metal

    Full text link
    We introduce various exchange interactions in a model Hamiltonian for Ce3+^{3+} ions in cubic symmetry with three configurations (f0f^0,f1f^1,f2f^2). With the impurity pseudo spin SI=1/2S_I=1/2, our Hamiltonian includes: (i) One-channel Sc=1/2S_c=1/2 Anderson model; (ii) Two-channel Sc=1/2S_c=1/2 Anderson model; (iii) An unforseen one-channel Sc=3/2S_c=3/2 Anderson model with a non-trivial fixed point; (iv) Mixing exchange interaction between the Γ6,7\Gamma_{6,7} and the Γ8\Gamma_8 conduction electron partial wave states; (v) Multiple conduction electron partial wave states. Using the third-order scaling (perturbative renormalization group) analysis, we study stability of various fixed points relevant to various exchange interactions for Ce3+^{3+} ions in cubic symmetry.Comment: 68 pages. 4 figures are available upon request from [email protected] (revised
    • 

    corecore