10,631 research outputs found

    The η(2225)\eta(2225) observed by the BES Collaboration

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    In the framework of the 3P0^3P_0 meson decay model, the strong decays of the 31S03 ^1S_0 and 41S04 ^1S_0 ssˉs\bar{s} states are investigated. It is found that in the presence of the initial state mass being 2.24 GeV, the total widths of the 31S03 ^1S_0 and 41S04 ^1S_0 ssˉs\bar{s} states are about 438 MeV and 125 MeV, respectively. Also, when the initial state mass varies from 2220 to 2400 MeV, the total width of the 41S04 ^1S_0 ssˉs\bar{s} state varies from about 100 to 132 MeV, while the total width of the 31S03 ^1S_0 ssˉs\bar{s} state varies from about 400 to 594 MeV. A comparison of the predicted widths and the experimental result of (0.19±0.03−0.06+0.04)(0.19\pm 0.03^{+0.04}_{-0.06}) GeV, the width of the η(2225)\eta(2225) with a mass of (2.24−0.02−0.02+0.03+0.03)(2.24^{+0.03+0.03}_{-0.02-0.02}) GeV recently observed by the BES Collaboration in the radiative decay J/ψ→γϕϕ→γK+K−KS0KL0J/\psi\to\gamma\phi\phi\to\gamma K^+K^-K^0_SK^0_L, suggests that it would be very difficult to identify the η(2225)\eta(2225) as the 31S03 ^1S_0 ssˉs\bar{s} state, and the η(2225)\eta(2225) seams a good candidate for the 41S04 ^1S_0 ssˉs\bar{s} state.Comment: 14 pages, 3 figures, typos corrected, Accepted by Physical Review

    Analysis of HARP TPC krypton data

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    This memo describes the procedure which was adopted to equalize the response of the 3972 pads of the HARP TPC, using radioactive 83mKr gas. The results obtained from the study of reconstructed krypton clusters in the calibration data taken in 2002 are reported. Two complementary methods were employed in the data analysis. Compatible results were obtained for channel-to-channel equalization constants. An estimate of the overall systematic uncertainty was derived

    On the Matrix Element of the Transverse Component of Bilocal Vector Current and its Parton Interpretation

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    In this paper we study the matrix element of the transverse component of the bilocal vector current in the context of deep inelastic scattering. BJL limit of high energy amplitudes together with light-front current algebra imply the same parton interpretation for its matrix element as that of the plus component. On the other hand, the transverse component depends explicitly on the gluon field operator in QCD, appears as "twist three" and hence its matrix element has no manifest parton interpretation. In this paper we perform calculations in light-front time-ordering perturbative QCD for a dressed quark target to order αs\alpha_s and demonstrate that the matrix element of the transverse component of the bilocal vector current has the same parton interpretation as that of the plus component.Comment: 7 pages, REVTE

    Learning Bodily and Temporal Attention in Protective Movement Behavior Detection

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    For people with chronic pain, the assessment of protective behavior during physical functioning is essential to understand their subjective pain-related experiences (e.g., fear and anxiety toward pain and injury) and how they deal with such experiences (avoidance or reliance on specific body joints), with the ultimate goal of guiding intervention. Advances in deep learning (DL) can enable the development of such intervention. Using the EmoPain MoCap dataset, we investigate how attention-based DL architectures can be used to improve the detection of protective behavior by capturing the most informative temporal and body configurational cues characterizing specific movements and the strategies used to perform them. We propose an end-to-end deep learning architecture named BodyAttentionNet (BANet). BANet is designed to learn temporal and bodily parts that are more informative to the detection of protective behavior. The approach addresses the variety of ways people execute a movement (including healthy people) independently of the type of movement analyzed. Through extensive comparison experiments with other state-of-the-art machine learning techniques used with motion capture data, we show statistically significant improvements achieved by using these attention mechanisms. In addition, the BANet architecture requires a much lower number of parameters than the state of the art for comparable if not higher performances.Comment: 7 pages, 3 figures, 2 tables, code available, accepted in ACII 201

    On the mass relation of a meson nonet

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    It is pointed out that the omission of the effects of the transition between quarkonia or the assumption that the transition between quarkonia is flavor-independent would result in the inconsistent results for the pseudoscalar meson nonet. It is emphasized that the mass relation of the non-ideal mixing meson nonets should incorporate the effects of the flavor-dependent transition between quarkonia. The new mass relations of a meson nonet are presented.Comment: Latex, 10 pages, to appear in Mod. Phys. Lett.

    Evidence for the disintegration of KIC 12557548 b

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    Context. The Kepler object KIC 12557548 b is peculiar. It exhibits transit-like features every 15.7 hours that vary in depth between 0.2% and 1.2%. Rappaport et al. (2012) explain the observations in terms of a disintegrating, rocky planet that has a trailing cloud of dust created and constantly replenished by thermal surface erosion. The variability of the transit depth is then a consequence of changes in the cloud optical depth. Aims. We aim to validate the disintegrating-planet scenario by modeling the detailed shape of the observed light curve, and thereby constrain the cloud particle properties to better understand the nature of this intriguing object. Methods. We analysed the six publicly-available quarters of raw Kepler data, phase-folded the light curve and fitted it to a model for the trailing dust cloud. Constraints on the particle properties were investigated with a light-scattering code. Results. The light curve exhibits clear signatures of light scattering and absorption by dust, including a brightening in flux just before ingress correlated with the transit depth and explained by forward scattering, and an asymmetry in the transit light curve shape, which is easily reproduced by an exponentially decaying distribution of optically thin dust, with a typical grain size of 0.1 micron. Conclusions. Our quantitative analysis supports the hypothesis that the transit signal of KIC 12557548 b is due to a variable cloud of dust, most likely originating from a disintegrating object.Comment: 5 pages, 4 figures. Accepted for publication in Astronomy and Astrophysic

    Towards the assignment for the 41S04 ^1S_0 meson nonet

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    The strong decays of the π(2070)\pi(2070), η(2010)\eta(2010), η(2100)\eta(2100), η(2190)\eta(2190), and η(2225)\eta(2225) as the 41S04 ^1S_0 quark-antiquark states are investigated in the framework of the 3P0^3P_0 meson decay model. It is found that the π(2070)\pi(2070), η(2100)\eta(2100), and η(2225)\eta(2225) appear to be the convincing 41S04 ^1S_0 qqˉq\bar{q} states while the assignment of the η(2010)\eta(2010) and η(2190)\eta(2190) as the 41S04 ^1S_0 isoscalar states is not favored by their widths. In the presence of the π(2070)\pi(2070), η(2100)\eta(2100), and η(2225)\eta(2225) being the members of the 41S04 ^1S_0 meson nonet, the 41S04 ^1S_0 kaon is phenomenologically determined to has a mass of about 2153 MeV. The width of this unobserved kaon is expected to be about 197 MeV in the 3P0^3P_0 decay model.Comment: 15 pages, 5 figures, version accepted for publication in Physical Review
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