520 research outputs found

    ORAL CREATINE SUPPLEMENTATION AND SHORT-TERM DYNAMIC POWER PRODUCTION IN HEALTHY YOUNG MEN

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    This experiment examined the effect of creatine monohydrate supplementation on corrected peak power output and peak acceleration during repeated, high intensity sprint cycling. The investigation was randomised, placebo-controlled, double-blind and adopted a crossover design. Eight male, adult volunteers participated in this study. Subjects were administered with creatine monohydrate (0.28g.kg-1 per day) or a glucose placebo. Following experimental treatments, subjects underwent 10 maximal effort, 6-s sprints on a cycle ergometer with a work to rest ratio of 5:1. The exercise protocol was fatiguing in nature with peak power output and peak acceleration decreasing significantly from the first to last sprint. Creatine supplementation significantly attenuated the decline in peak power output in the latter stages of the intermittent sprint cycling

    Characterisation of the Muscle Protein Synthetic Response to Resistance Exercise in Healthy Adults: A Systematic Review and Exploratory Meta-Analysis

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    Background and Objective: The rate of skeletal muscle protein synthesis (MPS) is the principal driving force underpinning the muscular adaptive response to resistance exercise (RE). This study aims to consolidate the literature, characterise MPS response to RE, and assess the impact of key covariates. Methods: Five electronic databases (PubMed (Medline), Web of Science, Embase, Sport Discus, and Cochrane Library) were searched for controlled trials that assessed the MPS response to RE in healthy, adult humans, postabsorptive state. Individual study and random-effects meta-analysis arewere used to inform the effects of RE and covariates on MPS. Results from 79 controlled trials with 237 participants were analysed. Results: Analysis of the pooled effects revealed robust increases in MPS following RE (weighted mean difference (WMD): 0.032% h−1, 95% CI: [0.024, 0.041] % h−1, I2 = 92%, k = 37, P<0.001). However, the magnitude of the increase in MPS was lower in older adults (>50 y: WMD: 0.015% h−1, 95% CI: [0.007, 0.022] % h−1, I2 = 76%, k = 12, P=0.002) compared to younger adults (<35 y: WMD: 0.041% h−1, 95% CI: [0.030, 0.052] % h−1, I2 = 88%, k = 25, P<0.001). Individual studies have reported that the temporal proximity of the RE, muscle group, muscle protein fraction, RE training experience, and the loading parameters of the RE (i.e., intensity, workload, and effort) appeared to affect the MPS response to RE, whereas sex or type of muscle contraction does not. Conclusion: A single bout of RE can sustain measurable increases in postabsorptive MPS soon after RE cessation and up to 48 h post-RE. However, there is substantial heterogeneity in the magnitude and time course of the MPS response between trials, which appears to be influenced by participants’ age and/or the loading parameters of the RE itself.Funder: Marigot Ltd; FundRef: https://doi.org/10.13039/10.13039/501100000821; Grant(s): IP_2019_087

    Photon statistics of a random laser

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    A general relationship is presented between the statistics of thermal radiation from a random medium and its scattering matrix S. Familiar results for black-body radiation are recovered in the limit S to 0. The mean photocount is proportional to the trace of 1-SS^dagger, in accordance with Kirchhoff's law relating emissivity and absorptivity. Higher moments of the photocount distribution are related to traces of powers of 1-SS^dagger, a generalization of Kirchhoff's law. The theory can be applied to a random amplifying medium (or "random laser") below the laser threshold, by evaluating the Bose-Einstein function at a negative temperature. Anomalously large fluctuations are predicted in the photocount upon approaching the laser threshold, as a consequence of overlapping cavity modes with a broad distribution of spectral widths.Comment: 26 pages, including 9 figure

    On random flights with non-uniformly distributed directions

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    This paper deals with a new class of random flights Xd(t),t>0,\underline{\bf X}_d(t),t>0, defined in the real space Rd,d2,\mathbb{R}^d, d\geq 2, characterized by non-uniform probability distributions on the multidimensional sphere. These random motions differ from similar models appeared in literature which take directions according to the uniform law. The family of angular probability distributions introduced in this paper depends on a parameter ν0\nu\geq 0 which gives the level of drift of the motion. Furthermore, we assume that the number of changes of direction performed by the random flight is fixed. The time lengths between two consecutive changes of orientation have joint probability distribution given by a Dirichlet density function. The analysis of Xd(t),t>0,\underline{\bf X}_d(t),t>0, is not an easy task, because it involves the calculation of integrals which are not always solvable. Therefore, we analyze the random flight Xmd(t),t>0,\underline{\bf X}_m^d(t),t>0, obtained as projection onto the lower spaces Rm,m<d,\mathbb{R}^m,m<d, of the original random motion in Rd\mathbb{R}^d. Then we get the probability distribution of Xmd(t),t>0.\underline{\bf X}_m^d(t),t>0. Although, in its general framework, the analysis of Xd(t),t>0,\underline{\bf X}_d(t),t>0, is very complicated, for some values of ν\nu, we can provide some results on the process. Indeed, for ν=1\nu=1, we obtain the characteristic function of the random flight moving in Rd\mathbb{R}^d. Furthermore, by inverting the characteristic function, we are able to give the analytic form (up to some constants) of the probability distribution of Xd(t),t>0.\underline{\bf X}_d(t),t>0.Comment: 28 pages, 3 figure

    Statistical features of edge turbulence in RFX-mod from Gas Puffing Imaging

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    Plasma density fluctuations in the edge plasma of the RFX-mod device are measured through the Gas Puffing Imaging Diagnostics. Statistical features of the signal are quantified in terms of the Probability Distribution Function (PDF), and computed for several kinds of discharges. The PDFs from discharges without particular control methods are found to be adequately described by a Gamma function, consistently with the recent results by Graves et al [J.P. Graves, et al, Plasma Phys. Control. Fusion 47, L1 (2005)]. On the other hand, pulses with external methods for plasma control feature modified PDFs. A first empirical analysis suggests that they may be interpolated through a linear combination of simple functions. An inspection of the literature shows that this kind of PDFs is common to other devices as well, and has been suggested to be due to the simultaneous presence of different mechanisms driving respectively coherent bursts and gaussian background turbulence. An attempt is made to relate differences in the PDFs to plasma conditions such as the local shift of the plasma column. A simple phenomenological model to interpret the nature of the PDF and assign a meaning to its parameters is also developed.Comment: 27 pages. Published in PPC

    Bernoulli potential in type-I and weak type-II superconductors: I. Surface charge

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    The electrostatic potential close to the surface of superconductors in the Meissner state is discussed. We show that beside the Bernoulli potential, the quasiparticle screening, and the thermodynamic contribution due to Rickayzen, there is a non-local contribution which is large for both type-I and weak type-II superconductors.Comment: 7 pages, 4 figure

    Manipulation of photon statistics of highly degenerate chaotic radiation

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    Highly degenerate chaotic radiation has a Gaussian density matrix and a large occupation number of modes ff . If it is passed through a weakly transmitting barrier, its counting statistics is close to Poissonian. We show that a second identical barrier, in series with the first, drastically modifies the statistics. The variance of the photocount is increased above the mean by a factor ff times a numerical coefficient. The photocount distribution reaches a limiting form with a Gaussian body and highly asymmetric tails. These are general consequences of the combination of weak transmission and multiple scattering.Comment: 4 pages, 2 figure
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