639,717 research outputs found

    Local Regularization Assisted Orthogonal Least Squares Regression

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    A locally regularized orthogonal least squares (LROLS) algorithm is proposed for constructing parsimonious or sparse regression models that generalize well. By associating each orthogonal weight in the regression model with an individual regularization parameter, the ability for the orthogonal least squares (OLS) model selection to produce a very sparse model with good generalization performance is greatly enhanced. Furthermore, with the assistance of local regularization, when to terminate the model selection procedure becomes much clearer. This LROLS algorithm has computational advantages over the recently introduced relevance vector machine (RVM) method

    Stability Of contact discontinuity for steady Euler System in infinite duct

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    In this paper, we prove structural stability of contact discontinuities for full Euler system

    Pressure deformation of tires using differential stiffness for triangular solid-of-revolution elements

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    The derivation is presented of the differential stiffness for triangular solid of revolution elements. The derivation takes into account the element rigid body rotation only, the rotation being about the circumferential axis. Internal pressurization of a pneumatic tire is used to illustrate the application of this feature

    Determining the optimal decision delay parameter for a linear equalizer

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    The achievable bit error rate of a linear equalizer is crucially determined by the choice of a decision delay parameter. This brief paper presents a simple method for the efficient determination of the optimal decision delay parameter that results in the best bit error rate performance for a linear equaliz

    Strongly Coupled Inflaton

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    We continue to investigate properties of the strongly coupled inflaton in a setup introduced in arXiv:0807.3191 through the AdS/CFT correspondence. These properties are qualitatively different from those in conventional inflationary models. For example, in slow-roll inflation, the inflaton velocity is not determined by the shape of potential; the fine-tuning problem concerns the dual infrared geometry instead of the potential; the non-Gaussianities such as the local form can naturally become large.Comment: 12 pages; v3, minor revision, comments and reference added, JCAP versio

    Creating a virtual support group in an interactive narrative:a companionship game for cancer patients

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    Over one in five cancer patients are affected by feelings of loneliness [1]. This paper proposes a text-based game aimed at affected cancer patients, in which the player develops relationships with non-player characters in the context of a fictitious cancer support group. This would be designed with the aim of alleviating patient loneliness and fostering a sense of companionship. This work is part of an interdisciplinary project led by Abertay University and partnered with Macmillan Cancer Support, exploring the ways in which interactive storytelling can be used to support cancer patients. The game’s narrative and characters will be designed drawing on real patient experiences gathered in interviews. The game will go through several iterations of feedback and rewriting in response to focus groups held with patients and healthcare professionals.</p

    Driving Operators Relevant: A Feature of Chern-Simons Interaction

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    By computing anomalous dimensions of gauge invariant composite operators (ψˉψ)n(\bar\psi\psi)^n and (ϕϕ)n(\phi^*\phi)^n in Chern-Simons fermion and boson models, we address that Chern-Simons interactions make these operators more relevant or less irrelevant in the low energy region. We obtain a critical Chern-Simons fermion coupling, 1κc2=619{1\over \kappa_c^2} = {6\over 19}, for a phase transition at which the leading irrelevant four-fermion operator (ψˉψ)2(\bar\psi\psi)^2 becomes marginal, and a critical Chern-Simons boson coupling, 1κc2=634{1\over \kappa_c^2} = {6\over 34}, for a similar phase transition for the leading irrelevant operator (ϕϕ)4(\phi^*\phi)^4. We see this phenomenon also in the 1/N1/N expansion.Comment: (ten pages, latex, figures included
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