414 research outputs found

    Cellular regenerative therapy for acquired noncongenital musculoskeletal disorders

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    CITATION: Niesler, C. U. et al. 2019. Cellular regenerative therapy for acquired noncongenital musculoskeletal disorders. South African Medical Journal, 109(8b):58-63. doi:10.7196/SAMJ.2019.v109i8b.13860The original publication is available at http://www.samj.org.za/index.php/samj/indexENGLISH ABSTRACT: Stem cells have an inherent capacity to facilitate regeneration; this has led to unprecedented growth in their experimental use in various clinical settings, particularly in patients with diseases with few alternative treatment options. However, their approved clinical use has to date been restricted largely to haematological diseases and epidermal transplantation to treat severe burns. After thorough searching of two databases, this review illuminates the role of stem cell therapy for treatment of musculoskeletal diseases. Research suggests that successful application of stem cells as regenerative mediators is in all likelihood dependent on the ability of endogenous tissue-resident reparative mediators to respond to paracrine signals provided by the applied stem cells. Therefore, an understanding of how the pathological environment influences this process is crucial for the ultimate success of stem cell therapies. The current review presents both the progress and limitations of stem cells as regenerative mediators in the context of musculoskeletal disorders.DST/NRF South African Research Chair Initiativehttp://www.samj.org.za/index.php/samj/article/view/12714Publisher’s versio

    Monte Carlo simulation of virtual Compton scattering below pion threshold

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    This paper describes the Monte Carlo simulation developed specifically for the VCS experiments below pion threshold that have been performed at MAMI and JLab. This simulation generates events according to the (Bethe-Heitler + Born) cross section behaviour and takes into account all relevant resolution-deteriorating effects. It determines the `effective' solid angle for the various experimental settings which are used for the precise determination of photon electroproduction absolute cross section.Comment: 24 pages, 6 figures, to be published in Nuclear Instruments and Methods in Physics Research, A One author adde

    The first determination of Generalized Polarizabilities of the proton by a Virtual Compton Scattering experiment

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    Absolute differential cross sections for the reaction (e+p -> e+p+gamma) have been measured at a four-momentum transfer with virtuality Q^2=0.33 GeV^2 and polarization \epsilon = 0.62 in the range 33.6 to 111.5 MeV/c for the momentum of the outgoing photon in the photon-proton center of mass frame. The experiment has been performed with the high resolution spectrometers at the Mainz Microtron MAMI. From the photon angular distributions, two structure functions which are a linear combination of the generalized polarizabilities have been determined for the first time.Comment: 4 pages, 3 figure

    The HERMES Dual-Radiator Ring Imaging Cerenkov Detector

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    The construction and use of a dual radiator Ring Imaging Cerenkov(RICH) detector is described. This instrument was developed for the HERMES experiment at DESY which emphasizes measurements of semi-inclusive deep-inelastic scattering. It provides particle identification for pions, kaons, and protons in the momentum range from 2 to 15 GeV, which is essential to these studies. The instrument uses two radiators, C4F10, a heavy fluorocarbon gas, and a wall of silica aerogel tiles. The use of aerogel in a RICH detector has only recently become possible with the development of clear, large homogeneous and hydrophobic aerogel. A lightweight mirror was constructed using a newly perfected technique to make resin-coated carbon-fiber surfaces of optical quality. The photon detector consists of 1934 photomultiplier tubes for each detector half, held in a soft steel matrix to provide shielding against the residual field of the main spectrometer magnet.Comment: 25 pages, 23 figure

    Measurement of the Beam-Recoil Polarization in Low-Energy Virtual Compton Scattering from the Proton

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    Double-polarization observables in the reaction epepγ\vec{e}p \rightarrow e'\vec{p'}\gamma{} have been measured at Q2=0.33(GeV/c)2Q^2=0.33 (GeV/c)^2. The experiment was performed at the spectrometer setup of the A1 Collaboration using the 855 MeV polarized electron beam provided by the Mainz Microtron (MAMI) and a recoil proton polarimeter. From the double-polarization observables the structure function PLTP_{LT}^\perp is extracted for the first time, with the value (15.4±3.3(stat.)2.4+1.5(syst.))GeV2(-15.4 \pm 3.3 (stat.)^{+1.5}_{-2.4} (syst.)) GeV^{-2}, using the low-energy theorem for Virtual Compton Sattering. This structure function provides a hitherto unmeasured linear combination of the generalized polarizabilities of the proton

    A new measurement of the structure functions PLLPTT/epsilonP_{LL}-P_{TT}/epsilon and PLTP_{LT} in virtual Compton scattering at Q2=Q^2= 0.33 (GeV/c)2^2

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    The cross section of the epepγep \to e' p' \gamma reaction has been measured at Q2=0.33Q^2 = 0.33 (GeV/c)2^2. The experiment was performed using the electron beam of the MAMI accelerator and the standard detector setup of the A1 Collaboration. The cross section is analyzed using the low-energy theorem for virtual Compton scattering, yielding a new determination of the two structure functions P_LL}-P_{TT}/epsilon and PLTP_{LT} which are linear combinations of the generalized polarizabilities of the proton. We find somewhat larger values than in the previous investigation at the same Q2Q^2. This difference, however, is purely due to our more refined analysis of the data. The results tend to confirm the non-trivial Q2Q^2-evolution of the generalized polarizabilities and call for more measurements in the low-Q2Q^2 region (\le 1 (GeV/c)2^2).Comment: 9 pages, 10 figures. EPJA version. slight revisions in the text and figure

    Measurement of the Proton Spin Structure Function g1p with a Pure Hydrogen Target

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    A measurement of the proton spin structure function g1p(x,Q^2) in deep-inelastic scattering is presented. The data were taken with the 27.6 GeV longitudinally polarised positron beam at HERA incident on a longitudinally polarised pure hydrogen gas target internal to the storage ring. The kinematic range is 0.021<x<0.85 and 0.8 GeV^2<Q^2<20 GeV^2. The integral Int_{0.021}^{0.85} g1p(x)dx evaluated at Q0^2 of 2.5 GeV^2 is 0.122+/-0.003(stat.)+/-0.010(syst.).Comment: 7 pages, 3 figures, 1 table, RevTeX late

    Evidence for Quark-Hadron Duality in the Proton Spin Asymmetry A1A_1

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    Spin-dependent lepton-nucleon scattering data have been used to investigate the validity of the concept of quark-hadron duality for the spin asymmetry A1A_1. Longitudinally polarised positrons were scattered off a longitudinally polarised hydrogen target for values of Q2Q^2 between 1.2 and 12 GeV2^2 and values of W2W^2 between 1 and 4 GeV2^2. The average double-spin asymmetry in the nucleon resonance region is found to agree with that measured in deep-inelastic scattering at the same values of the Bjorken scaling variable xx. This finding implies that the description of A1A_1 in terms of quark degrees of freedom is valid also in the nucleon resonance region for values of Q2Q^2 above 1.6 GeV2^2.Comment: 5 pages, 1 eps figure, table added, new references added, in print in Phys. Rev. Let

    Beam-Induced Nuclear Depolarisation in a Gaseous Polarised Hydrogen Target

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    Spin-polarised atomic hydrogen is used as a gaseous polarised proton target in high energy and nuclear physics experiments operating with internal beams in storage rings. When such beams are intense and bunched, this type of target can be depolarised by a resonant interaction with the transient magnetic field generated by the beam bunches. This effect has been studied with the HERA positron beam in the HERMES experiment at DESY. Resonances have been observed and a simple analytic model has been used to explain their shape and position. Operating conditions for the experiment have been found where there is no significant target depolarisation due to this effect.Comment: REVTEX, 6 pages, 5 figure
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