59,517 research outputs found

    Large-N analysis of (2+1)-dimensional Thirring model

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    We analyze (2+1)(2+1)-dimensional vector-vector type four-Fermi interaction (Thirring) model in the framework of the 1/N1/N expansion. By solving the Dyson-Schwinger equation in the large-NN limit, we show that in the two-component formalism the fermions acquire parity-violating mass dynamically in the range of the dimensionless coupling α\alpha, 0ααc116exp(Nπ216)0 \leq \alpha \leq \alpha_c \equiv {1\over16} {\rm exp} (- {N \pi^2 \over 16}). The symmetry breaking pattern is, however, in a way to conserve the overall parity of the theory such that the Chern-Simons term is not induced at any orders in 1/N1/N. αc\alpha_c turns out to be a non-perturbative UV-fixed point in 1/N1/N. The β\beta function is calculated to be β(α)=2(ααc)\beta (\alpha) = -2 (\alpha - \alpha_c) near the fixed point, and the UV-fixed point and the β\beta function are shown exact in the 1/N1/N expansion.Comment: 14 pages Latex. (Revised version: some changes have been made and references added.) To appear in Phys. Rev. D, SNUTP 93-4

    Broadband optical radiation detector

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    A method and apparatus for detecting optical radiation by optically monitoring temperature changes in a microvolume caused by absorption of the optical radiation to be detected is described. More specifically, a thermal lens forming material is provided which has first and second opposite, substantially parallel surfaces. A reflective coating is formed on the first surface, and a radiation absorbing coating is formed on the reflective coating. Chopped, incoming optical radiation to be detected is directed to irradiate a small portion of the radiation absorbing coating. Heat generated in this small area is conducted to the lens forming material through the reflective coating, thereby raising the temperature of a small portion of the lens forming material and causing a thermal lens to be formed therein

    Double-beam optical method and apparatus for measuring thermal diffusivity and other molecular dynamic processes in utilizing the transient thermal lens effect

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    A sample material was irradiated by relatively high power, short pulses from a dye laser. Energy from the pulses was absorbed by the sample material, thereby forming a thermal lens in the area of absorption. The pulse repetition rate was chosen so that the thermal lens is substantially dissipated by the time the next pulse reaches the sample material. A probe light beam, which in a specific embodiment is a relatively low power, continuous wave (cw) laser beam, irradiated the thermal lens formed in the sample material. The intensity characteristics of the probe light beam subsequent to irradiation of the thermal lens is related to changes in the refractive index of the sample material as the thermal lens is formed and dissipated

    Asymptotic behavior of the least common multiple of consecutive arithmetic progression terms

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    Let ll and mm be two integers with l>m0l>m\ge 0, and let aa and bb be integers with a1a\ge 1 and a+b1a+b\ge 1. In this paper, we prove that loglcmmn<iln{ai+b}=An+o(n)\log {\rm lcm}_{mn<i\le ln}\{ai+b\} =An+o(n), where AA is a constant depending on l,ml, m and aa.Comment: 8 pages. To appear in Archiv der Mathemati

    The least common multiple of a sequence of products of linear polynomials

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    Let f(x)f(x) be the product of several linear polynomials with integer coefficients. In this paper, we obtain the estimate: loglcm(f(1),...,f(n))An\log {\rm lcm}(f(1), ..., f(n))\sim An as nn\rightarrow\infty , where AA is a constant depending on ff.Comment: To appear in Acta Mathematica Hungaric
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