Reliability Ratio Based Weighted Bit-Flipping Decoding for LDPC Codes

In this contribution, a novel reliability-ratio based weighted bit-flipping(RRWBF) algorithm is proposed for decoding Low Density Parity Check (LDPC) codes. The RRWBF algorithm proposed is benchmarked against the conventional weighted bit-flipping (WBF) algorithm [1] and the improved weighted bit-flipping (IWBF) algorithm [2]. More than 1 and 2 dB coding gain was achieved at an BER of 10-5 while invoking the RRWBF algorithm in comparison to the two benchmarking schemes, when communicating over an AWGN and an uncorrelated Rayleigh channel, respectively. Furthermore, the decoding complexity of the proposed RRWBF algorithm is maintained at the same level as that of the conventional WBF algorithm

Nonperturbative model for optical response under intense periodic fields with application to graphene in a strong perpendicular magnetic field

Graphene exhibits extremely strong optical nonlinearity when a strong perpendicular magnetic field is applied, the response current shows strong field dependence even for moderate light intensity, and the perturbation theory fails. We nonperturbatively calculate full optical conductivities induced by a periodic field in an equation-of-motion framework based on the Floquet theorem, with the scattering described phenomenologically. The nonlinear response at high fields is understood in terms of the dressed electronic states, or Floquet states, which is further characterized by the optical conductivity for a weak probe light field. This approach is illustrated for a magnetic field at $5$ T and a driving field with photon energy $0.05$ eV. Our results show that the perturbation theory works only for weak fields $<3$ kV/cm, confirming the extremely strong light matter interaction for Landau levels of graphene. This approach can be easily extended to the calculation of optical conductivities in other systems

Photoproduction of K∗+ΛK^{*+}\Lambda and K+Σ(1385)K^+\Sigma(1385) in the reaction \gamma \lowercase{p} \to K^+ \Lambda \pi^0 at Jefferson Lab

The search for missing nucleon resonances using coupled channel analysis has mostly been concentrated on $N\pi$ and $KY$ channels, while the contributions of $K^*Y$ and $KY^*$ channels have not been investigated thoroughly mostly due to the lack of data. With an integrated luminosity of about 75 $pb^{-1}$, the photoproduction data using a proton target recently collected by the CLAS Collaboration at Jefferson Lab with a photon energy range of 1.5-3.8 GeV provided large statistics for the study of light hyperon photoproduction through exclusive reactions. The reaction $\gamma p \to K^+ \Lambda \pi^0$ has been investigated. Preliminary results of the $K^{*+}\Lambda$ and $K^+\Sigma(1385)$ cross sections are not negligible compared with the $KY$ channels. The $\Lambda \pi^0$ invariant mass spectrum is dominated by the $\Sigma(1385)$ signal and no significant structure was found around the $\Sigma(1480)$ region.Comment: 4 pages, 3 figures, to be publised on the NSTAR05 proceeding

Asymptotic inference in some heteroscedastic regression models with long memory design and errors

This paper discusses asymptotic distributions of various estimators of the underlying parameters in some regression models with long memory (LM) Gaussian design and nonparametric heteroscedastic LM moving average errors. In the simple linear regression model, the first-order asymptotic distribution of the least square estimator of the slope parameter is observed to be degenerate. However, in the second order, this estimator is $n^{1/2}$-consistent and asymptotically normal for $h+H<3/2$; nonnormal otherwise, where $h$ and $H$ are LM parameters of design and error processes, respectively. The finite-dimensional asymptotic distributions of a class of kernel type estimators of the conditional variance function $\sigma^2(x)$ in a more general heteroscedastic regression model are found to be normal whenever $H<(1+h)/2$, and non-normal otherwise. In addition, in this general model, $\log(n)$-consistency of the local Whittle estimator of $H$ based on pseudo residuals and consistency of a cross validation type estimator of $\sigma^2(x)$ are established. All of these findings are then used to propose a lack-of-fit test of a parametric regression model, with an application to some currency exchange rate data which exhibit LM.Comment: Published in at http://dx.doi.org/10.1214/009053607000000686 the Annals of Statistics (http://www.imstat.org/aos/) by the Institute of Mathematical Statistics (http://www.imstat.org

Experimental studies on the shear resistance of original coal-shale joint

Purpose. Experimental study and theoretical modeling of the shear resistance of original coal-shale joint. Methods. A two-segment model was developed to describe the shear resistance-shear displacement curves obtained from the direct shear tests of eight coal-shale joints by letting the two segments of the fitting curve pass through the peak point of each curve. Findings. The two-segment model well describes the shear resistance variation of the coal-shale joints during the shear process, and there exist good relationships between the fitting parameters and the shear testing parameters. The initial slope of the softening part of the shear resistance – shear displacement curve can help to predict whether the coal pillar will burst drastically when it fails. Moreover, the normal displacement was very small in the pre-peak range which indicates that the complete detachment of original coal-shale joint surfaces has not occurred before the peak. Originality. Direct shear tests were conducted on original coal-shale specimens for the first time, and a two-segment model is developed to describe their shear resistance-shear displacement curves. The initial slope of the softening part of the shear resistance – shear displacement curve is proposed to predict the burst tendency of coal pillar. Different from unbonded rock joints, the detachment of the original coal-shale joint occurs just after the peak. Practical implications. The conclusions may have some help to understand the shear resistance mechanism of original coal-shale joint and to provide some new ideas of maintaining coal pillar stability.Мета. Експериментальне дослідження та теоретичне моделювання опору зсуву початкового шару вуглистого сланцю. Методика. Розроблено модель для опису кривих опору зсуву й зсувного зміщення, отриманих у результаті випробувань на прямий зсув восьми шарів вуглистого сланцю. Модель включає два сегменти апроксимуючої кривої, що проходять через вищі точки описуваних кривих. Результати. Запропонована модель достовірно описує зміну опору на зсув шарів вуглистого сланцю в про-процесі зсуву, при цьому визначено наявність тісного зв’язку між параметрами апроксимації та параметрами випробування на зсув. За початковим нахилом кривої в частині ослаблення опору зсуву й зсувного зміщення можна передбачити, чи відбудеться значне руйнування цілика вугілля при його обваленні. Нормальне зміщення є незначним у передпіковому діапазоні, що свідчить про те, що в цей час не відбувається повного відриву поверхонь шару вуглистого сланцю. Наукова новизна. Випробування на прямий зсув проводилися вперше на зразках початкового вуглистого сланцю. Двохсегментна модель була розроблена спеціально для опису кривих опору зсуву та зсувного зміщення досліджуваних шарів. За початковим нахилом кривої в частині ослаблення опору зсуву й зсувного зміщення можна передбачити характер руйнування цілика. На відміну від незв’язаних шарів породи, відділення початкового шару вуглистого сланцю відбувається після пікових значень досліджуваних кривих. Практична значимість. Висновки можуть допомогти зрозуміти механізм опору зсуву в первісному шарі вуглистого сланцю й окреслити нові підходи до збереження стабільності вугільного цілика.Цель. Экспериментальное исследование и теоретическое моделирование сопротивления сдвигу первоначального слоя углистого сланца. Методика. Разработана модель для описания кривых сопротивления сдвигу и сдвигового смещения, полученных в результате испытаний на прямой сдвиг восьми слоев углистого сланца. Модель включает два сегмента аппроксимирующей кривой которые проходят через высшие точки описываемых кривых. Результаты. Предлагаемая модель достоверно описывает изменение сопротивления на сдвиг слоев углистого сланца в процессе сдвига, при этом определено наличие тесной связи между параметрами аппроксимации и параметрами испытания на сдвиг. По начальному наклону кривой в части ослабления сопротивления сдвигу и сдвигового смещения можно предсказать, произойдет ли значительное разрушение целика угля при его обрушении. Нормальное смещение незначительно в предпиковом диапазоне, что свидетельствует о том, что в это время не происходит полного отрыва поверхностей слоя углистого сланца. Научная новизна. Испытания на прямой сдвиг проводились впервые на образцах первоначального углистого сланца. Двухсегментная модель была разработана специально для описания кривых сопротивления сдвигу и сдвигового смещения исследуемых слоев. По начальному наклону кривой в части ослабления сопротивления сдвигу и сдвигового смещения можно предсказать характер разрушения целика. В отличие от несвязанных слоев породы, отделение первоначального слоя углистого сланца происходит после пиковых значений исследуемых кривых. Практическая значимость. Выводы могут помочь понять механизм сопротивления сдвигу в первоначальном слое углистого сланца и обозначить новые подходы к сохранению стабильности угольного целика.The authors gratefully acknowledge funding by China National Natural Science Foundation (51109076) and the key scientific and technological project of Henan Province (152102210316)

Blow up solutions to a viscoelastic fluid system and a coupled Navier-Stokes/Phase-Field system in R^2

We find explicit solutions to both the Oldroyd-B model with infinite Weissenberg number and the coupled Navier-Stokes/Phase-Field system. The solutions blow up in finite time.Comment: 5 page

Nonlinear magneto-optic effects in doped graphene and gapped graphene: a perturbative treatment

The nonlinear magneto-optic responses are investigated for gapped graphene and doped graphene in a perpendicular magnetic field. The electronic states are described by Landau levels, and the electron dynamics in an optical field is obtained by solving the density matrix in the equation of motion. In the linear dispersion approximation around the Dirac points, both linear conductivity and third order nonlinear conductivities are numerically evaluated for infrared frequencies. The nonlinear phenomena, including third harmonic generation, Kerr effects and two photon absorption, and four wave mixing, are studied. All optical conductivities show strong dependence on the magnetic field. At weak magnetic fields, our results for doped graphene agree with those in the literature. We also present the spectra of the conductivities of gapped graphene. At strong magnetic fields, the third order conductivities show peaks with varying the magnetic field and the photon energy. These peaks are induced by the resonant transitions between different Landau levels. The resonant channels, the positions, and the divergences of peaks are analyzed. The conductivities can be greatly modified, up to orders of magnitude. The dependence of the conductivities on the gap parameter and the chemical potential is studied.Comment: 18 pages, 8 figure