480 research outputs found

    Search for f1(1285)→π+π−π0f_1(1285) \to \pi^+\pi^-\pi^0 decay with VES detector

    Full text link
    The isospin violating decay f1(1285)→π+π−π0f_1(1285)\to\pi^+\pi^-\pi^0 has been studied at VES facility. This study is based at the statistics acquired in π−Be\pi^- Be interactions at 27, 36.6 and 41 GeV/c in diffractive reaction π−N→(f1π−)N\pi^- N \to (f_1 \pi^-) N. The f1(1285)→π+π−π0f_1(1285) \to \pi^+\pi^-\pi^0 decay is observed. The ratio of decay probabilities BR(f1(1285)→π+π−π0)BR(f_1(1285) \to \pi^+\pi^-\pi^0) to BR(f1(1285)→ηπ+π−)⋅BR(η→γγ)BR(f_1(1285) \to \eta \pi^+\pi^-) \cdot BR(\eta \to \gamma\gamma) is ∌ 1.4\sim\:1.4%.Comment: 10 pages, 8 figures, presented at XII Conference on Hadron Spectroscop

    ĐŸĐ°Ń‚ĐŸĐłĐ”ĐœĐ”Ń‚ĐžŃ‡ĐœŃ– фаĐșŃ‚ĐŸŃ€Đž Ń€ĐŸĐ·ĐČотĐșу Đ°ŃƒŃ‚ĐŸŃ–ĐŒŃƒĐœĐœĐžŃ… Đ·Đ°Ń…ĐČĐŸŃ€ŃŽĐČĐ°ĐœŃŒ. ĐĄŃƒŃ‡Đ°ŃĐœŃ– ĐżŃ–ĐŽŃ…ĐŸĐŽĐž ĐŽĐŸ їх ліĐșуĐČĐ°ĐœĐœŃ

    Get PDF
    In experimental models of pathologies of autoimmune genesis there was grounded the possibility and confirmed the efficiency of using the products of fetoplacental complex. There was tested their ability to activate T-regulatory immunity link and normalize cell indices in experimental animals. More pronounced immune correcting potential of cryopreserved material has been shown at cell and molecular levels. На эĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Đ°Đ»ŃŒĐœŃ‹Ń… ĐŒĐŸĐŽĐ”Đ»ŃŃ… ĐżĐ°Ń‚ĐŸĐ»ĐŸĐłĐžĐč Đ°ŃƒŃ‚ĐŸĐžĐŒĐŒŃƒĐœĐœĐŸĐłĐŸ ĐłĐ”ĐœĐ”Đ·Đ° ĐŸĐ±ĐŸŃĐœĐŸĐČĐ°ĐœĐ° ĐČĐŸĐ·ĐŒĐŸĐ¶ĐœĐŸŃŃ‚ŃŒ Đž ĐŽĐŸĐșĐ°Đ·Đ°ĐœĐ° ŃŃ„Ń„Đ”ĐșтоĐČĐœĐŸŃŃ‚ŃŒ ĐżŃ€ĐžĐŒĐ”ĐœĐ”ĐœĐžŃ ĐżŃ€ĐŸĐŽŃƒĐșŃ‚ĐŸĐČ Ń„Đ”Ń‚ĐŸĐżĐ»Đ°Ń†Đ”ĐœŃ‚Đ°Ń€ĐœĐŸĐłĐŸ ĐșĐŸĐŒĐżĐ»Đ”Đșса. ĐŸŃ€ĐŸĐŽĐ”ĐŒĐŸĐœŃŃ‚Ń€ĐžŃ€ĐŸĐČĐ°ĐœĐ° ох ŃĐżĐŸŃĐŸĐ±ĐœĐŸŃŃ‚ŃŒ Đș  аĐșтоĐČацоо Đą-Ń€Đ”ĐłŃƒĐ»ŃŃ‚ĐŸŃ€ĐœĐŸĐłĐŸ Đ·ĐČĐ”ĐœĐ° ĐžĐŒĐŒŃƒĐœĐžŃ‚Đ”Ń‚Đ° Đž ĐœĐŸŃ€ĐŒĐ°Đ»ĐžĐ·Đ°Ń†ĐžĐž ĐșĐ»ĐžĐœĐžŃ‡Đ”ŃĐșох ĐżĐŸĐșазатДлДĐč эĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Đ°Đ»ŃŒĐœŃ‹Ń… жОĐČĐŸŃ‚ĐœŃ‹Ń…. ĐŸĐŸĐșĐ°Đ·Đ°Đœ Đ±ĐŸĐ»Đ”Đ” ĐČŃ‹Ń€Đ°Đ¶Đ”ĐœĐœŃ‹Đč Â ĐžĐŒĐŒŃƒĐœĐŸĐșĐŸŃ€Ń€ĐžĐłĐžŃ€ŃƒŃŽŃ‰ĐžĐč ĐżĐŸŃ‚Đ”ĐœŃ†ĐžĐ°Đ» ĐșŃ€ĐžĐŸĐșĐŸĐœŃĐ”Ń€ĐČĐžŃ€ĐŸĐČĐ°ĐœĐœĐŸĐłĐŸ ĐŒĐ°Ń‚Đ”Ń€ĐžĐ°Đ»Đ° ĐœĐ° ĐșĐ»Đ”Ń‚ĐŸŃ‡ĐœĐŸĐŒ Đž ĐŒĐŸĐ»Đ”ĐșŃƒĐ»ŃŃ€ĐœĐŸĐŒ ŃƒŃ€ĐŸĐČĐœŃŃ….На Đ”ĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Đ°Đ»ŃŒĐœĐžŃ… ĐŒĐŸĐŽĐ”Đ»ŃŃ… ĐżĐ°Ń‚ĐŸĐ»ĐŸĐłŃ–Đč Đ°ŃƒŃ‚ĐŸŃ–ĐŒŃƒĐœĐœĐŸĐłĐŸ ĐłĐ”ĐœĐ”Đ·Ńƒ ĐŸĐ±ĐłŃ€ŃƒĐœŃ‚ĐŸĐČĐ°ĐœĐ° ĐŒĐŸĐ¶Đ»ĐžĐČість і ĐŽĐŸĐČĐ”ĐŽĐ”ĐœĐ° ДфДĐșтоĐČĐœŃ–ŃŃ‚ŃŒ Đ·Đ°ŃŃ‚ĐŸŃŃƒĐČĐ°ĐœĐœŃ ĐżŃ€ĐŸĐŽŃƒĐșтіĐČ Ń„Đ”Ń‚ĐŸĐżĐ»Đ°Ń†Đ”ĐœŃ‚Đ°Ń€ĐœĐŸĐłĐŸ ĐșĐŸĐŒĐżĐ»Đ”Đșсу. ĐŸŃ€ĐŸĐŽĐ”ĐŒĐŸĐœŃŃ‚Ń€ĐŸĐČĐ°ĐœĐŸ Ń—Ń…ĐœŃŽ Đ·ĐŽĐ°Ń‚ĐœŃ–ŃŃ‚ŃŒ ĐŽĐŸ Đ°ĐșтоĐČації Đą-Ń€Đ”ĐłŃƒĐ»ŃŃ‚ĐŸŃ€ĐœĐŸŃ— Đ»Đ°ĐœĐșĐž Ń–ĐŒŃƒĐœŃ–Ń‚Đ”Ń‚Ńƒ і ĐœĐŸŃ€ĐŒĐ°Đ»Ń–Đ·Đ°Ń†Ń–Ń— ĐșĐ»Ń–ĐœŃ–Ń‡ĐœĐžŃ… ĐżĐŸĐșĐ°Đ·ĐœĐžĐșіĐČ Đ”ĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Đ°Đ»ŃŒĐœĐžŃ… тĐČĐ°Ń€ĐžĐœ. ĐŸĐŸĐșĐ°Đ·Đ°ĐœĐŸ Đ±Ń–Đ»ŃŒŃˆ ĐČĐžŃ€Đ°Đ¶Đ”ĐœĐžĐč Ń–ĐŒŃƒĐœĐŸĐșĐŸŃ€ĐžĐłŃƒŃŽŃ‡ĐžĐč ĐżĐŸŃ‚Đ”ĐœŃ†Ń–Đ°Đ» ĐșŃ€Ń–ĐŸĐșĐŸĐœŃĐ”Ń€ĐČĐŸĐČĐ°ĐœĐŸĐłĐŸ ĐŒĐ°Ń‚Đ”Ń€Ń–Đ°Đ»Ńƒ ĐœĐ° ĐșĐ»Ń–Ń‚ĐžĐœĐœĐŸĐŒŃƒ і ĐŒĐŸĐ»Đ”ĐșŃƒĐ»ŃŃ€ĐœĐŸĐŒŃƒ ріĐČĐœŃŃ…

    R & D for collider beauty physics at the LHC

    Get PDF
    We propose an R&D program for the development of a Beauty trigger and innovative elements of the associated spectrometer. A series of short test runs is proposed at the SPS p-pbar Collider with the minimal spectrometer which will allow a credible B signal to be obtained in an invariant mass spectrum of reconstructed B mesons. The program builds on the success of the recent collider run of the P238 Collaboration, in which clean signals from beam-beam interactions were observed in a large silicon strip microvertex detector running 1.5 mm from the circulating beams. A continuing successful R&D program of the type proposed could ultimately lead to a collider experiment at the LHC to study CP Violation and rare B decays

    First observation of Bs -> D_{s2}^{*+} X mu nu decays

    Get PDF
    Using data collected with the LHCb detector in proton-proton collisions at a centre-of-mass energy of 7 TeV, the semileptonic decays Bs -> Ds+ X mu nu and Bs -> D0 K+ X mu nu are detected. Two structures are observed in the D0 K+ mass spectrum at masses consistent with the known D^+_{s1}(2536) and $D^{*+}_{s2}(2573) mesons. The measured branching fractions relative to the total Bs semileptonic rate are B(Bs -> D_{s2}^{*+} X mu nu)/B(Bs -> X mu nu)= (3.3\pm 1.0\pm 0.4)%, and B(Bs -> D_{s1}^+ X munu)/B(Bs -> X mu nu)= (5.4\pm 1.2\pm 0.5)%, where the first uncertainty is statistical and the second is systematic. This is the first observation of the D_{s2}^{*+} state in Bs decays; we also measure its mass and width.Comment: 8 pages 2 figures. Published in Physics Letters

    KLEVER: An experiment to measure BR(KL→π0ΜΜˉK_L\to\pi^0\nu\bar{\nu}) at the CERN SPS

    Full text link
    Precise measurements of the branching ratios for the flavor-changing neutral current decays K→πΜΜˉK\to\pi\nu\bar{\nu} can provide unique constraints on CKM unitarity and, potentially, evidence for new physics. It is important to measure both decay modes, K+→π+ΜΜˉK^+\to\pi^+\nu\bar{\nu} and KL→π0ΜΜˉK_L\to\pi^0\nu\bar{\nu}, since different new physics models affect the rates for each channel differently. The goal of the NA62 experiment at the CERN SPS is to measure the BR for the charged channel to within 10%. For the neutral channel, the BR has never been measured. We are designing the KLEVER experiment to measure BR(KL→π0ΜΜˉK_L\to\pi^0\nu\bar{\nu}) to ∌\sim20% using a high-energy neutral beam at the CERN SPS starting in LHC Run 4. The boost from the high-energy beam facilitates the rejection of background channels such as KL→π0π0K_L\to\pi^0\pi^0 by detection of the additional photons in the final state. On the other hand, the layout poses particular challenges for the design of the small-angle vetoes, which must reject photons from KLK_L decays escaping through the beam exit amidst an intense background from soft photons and neutrons in the beam. Background from Λ→nπ0\Lambda \to n\pi^0 decays in the beam must also be kept under control. We present findings from our design studies for the beamline and experiment, with an emphasis on the challenges faced and the potential sensitivity for the measurement of BR(KL→π0ΜΜˉK_L\to\pi^0\nu\bar{\nu}).Comment: 13 pages, 4 figures. Submitted as input to the 2020 update of the European Strategy for Particle Physics. v2: Included authors unintentionally omitted in v

    Physics beyond the standard model with kaons at NA62

    Get PDF
    The NA62 experiment at CERN Super Proton Synchrotron was designed to measure BR(K+ \u2192 \u3c0+\u3bdv\u304) with an in-fight technique, never used before for this measurement. This decay is characterised by a very precise prediction in the Standard Model. Its branching ratio, which is expected to be less than 10-10, is one of the best candidates to indicate indirect effects of new physics beyond SM at the highest mass scales. NA62 result on K+ \u2192 \u3c0+\u3bdv\u304 from the full 2016 data set is described. Also a search for an invisible dark photon A\u2032 has been performed, exploiting the efficient photon-veto capability and high resolution tracking of the NA62. The signal stems from the chain K+ \u2192 \u3c0+\u3c00 followed by \u3c00 \u2192 A\u2032\u3b3. No significant statistical excess has been identified. Upper limits on the dark photon coupling to the ordinary photon as a function of the dark photon mass have been set, improving on the previous limits over the mass range 60 - 110 MeV/c2

    Externalities and the nucleolus

    Full text link
    In most economic applications, externalities prevail: the worth of a coalition depends on how the other players are organized. We show that there is a unique natural way of extending the nucleolus from (coalitional) games without externalities to games with externalities. This is in contrast to the Shapley value and the core for which many different extensions have been proposed

    Search for π⁰ decays to invisible particles

    Get PDF
    The NA62 experiment at the CERN SPS reports a study of a sample of 4 × 109 tagged π0 mesons from K+ → π+π0(Îł), searching for the decay of the π0 to invisible particles. No signal is observed in excess of the expected background fluctuations. An upper limit of 4.4 × 10−9 is set on the branching ratio at 90% confidence level, improving on previous results by a factor of 60. This result can also be interpreted as a model- independent upper limit on the branching ratio for the decay K+ → π+X, where X is a particle escaping detection with mass in the range 0.110–0.155 GeV/c2 and rest lifetime greater than 100 ps. Model-dependent upper limits are obtained assuming X to be an axion-like particle with dominant fermion couplings or a dark scalar mixing with the Standard Model Higgs boson
    • 

    corecore