138 research outputs found

    Analysis of Gamma Radiation from a Radon Source: Indications of a Solar Influence

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    This article presents an analysis of about 29,000 measurements of gamma radiation associated with the decay of radon in a sealed container at the Geological Survey of Israel (GSI) Laboratory in Jerusalem between 28 January 2007 and 10 May 2010. These measurements exhibit strong variations in time of year and time of day, which may be due in part to environmental influences. However, time-series analysis reveals a number of periodicities, including two at approximately 11.2 year−1^{-1} and 12.5 year−1^{-1}. We have previously found these oscillations in nuclear-decay data acquired at the Brookhaven National Laboratory (BNL) and at the Physikalisch-Technische Bundesanstalt (PTB), and we have suggested that these oscillations are attributable to some form of solar radiation that has its origin in the deep solar interior. A curious property of the GSI data is that the annual oscillation is much stronger in daytime data than in nighttime data, but the opposite is true for all other oscillations. This may be a systematic effect but, if it is not, this property should help narrow the theoretical options for the mechanism responsible for decay-rate variability.Comment: 9 pages, 21 figure

    Accurate mass measurements of 26^{26}Ne, 26−30^{26-30}Na, 29−33^{29-33}Mg performed with the {\sc Mistral} spectrometer

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    The minuteness of the nuclear binding energy requires that mass measurements be highly precise and accurate. Here we report on new measurements 29−33^{29-33}Mg and 26^{26}Na performed with the {\sc Mistral} mass spectrometer at {\sc Cern}'s {\sc Isolde} facility. Since mass measurements are prone to systematic errors, considerable effort has been devoted to their evaluation and elimination in order to achieve accuracy and not only precision. We have therefore conducted a campaign of measurements for calibration and error evaluation. As a result, we now have a satisfactory description of the {\sc Mistral} calibration laws and error budget. We have applied our new understanding to previous measurements of 26^{26}Ne, 26−30^{26-30}Na and 29,32^{29,32}Mg for which re-evaluated values are reported.Comment: submitted to Nuclear Physics

    Gamma-Ray Spectroscopy of Λ16^{16}_\LambdaO and Λ15^{15}_\LambdaN Hypernuclei via the 16^{16}O(K−,π−)(K^-, \pi^-) reaction

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    he bound-state level structures of the Λ16^{16}_{\Lambda}O and Λ15^{15}_{\Lambda}N hypernuclei were studied by γ\gamma-ray spectroscopy using a germanium detector array (Hyperball) via the 16^{16}O (K−,π−γK^-, \pi^- \gamma) reaction. A level scheme for Λ16^{16}_{\Lambda}O was determined from the observation of three γ\gamma-ray transitions from the doublet of states (2−2^-,1−1^-) at ∼6.7\sim 6.7 MeV to the ground-state doublet (1−1^-,0−0^-). The Λ15^{15}_{\Lambda}N hypernuclei were produced via proton emission from unbound states in Λ16^{16}_{\Lambda}O . Three γ\gamma -rays were observed and the lifetime of the 1/2+;11/2^+;1 state in Λ15^{15}_{\Lambda}N was measured by the Doppler shift attenuation method. By comparing the experimental results with shell-model calculations, the spin-dependence of the ΛN\Lambda N interaction is discussed. In particular, the measured Λ16^{16}_{\Lambda}O ground-state doublet spacing of 26.4 ±\pm 1.6 ±\pm 0.5 keV determines a small but nonzero strength of the ΛN\Lambda N tensor interaction.Comment: 22 pages, 17 figure

    Up-Down Quark Mass Difference Effect in Nuclear Many-Body Systems

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    A charge-symmetry-breaking nucleon-nucleon force due to the up-down quark mass difference is evaluated in the quark cluster model. It is applied to the shell-model calculation for the isovector mass shifts of isospin multiplets and the isospin-mixing matrix elements in 1s0d-shell nuclei. We find that the contribution of the quark mass difference effect is large and agrees with experiment. This contribution may explain the Okamoto-Nolen-Schiffer anomaly, alternatively to the meson-mixing contribution, which is recently predicted to be reduced by the large off-shell correction

    Power Spectrum Analysis of Physikalisch-Technische Bundesanstalt Decay-Rate Data: Evidence for Solar Rotational Modulation

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    Evidence for an anomalous annual periodicity in certain nuclear decay data has led to speculation concerning a possible solar influence on nuclear processes. We have recently analyzed data concerning the decay rates of Cl-36 and Si-32, acquired at the Brookhaven National Laboratory (BNL), to search for evidence that might be indicative of a process involving solar rotation. Smoothing of the power spectrum by weighted-running-mean analysis leads to a significant peak at frequency 11.18/yr, which is lower than the equatorial synodic rotation rates of the convection and radiative zones. This article concerns measurements of the decay rates of Ra-226 acquired at the Physikalisch-Technische Bundesanstalt (PTB) in Germany. We find that a similar (but not identical) analysis yields a significant peak in the PTB dataset at frequency 11.21/yr, and a peak in the BNL dataset at 11.25/yr. The change in the BNL result is not significant since the uncertainties in the BNL and PTB analyses are estimated to be 0.13/yr and 0.07/yr, respectively. Combining the two running means by forming the joint power statistic leads to a highly significant peak at frequency 11.23/yr. We comment briefly on the possible implications of these results for solar physics and for particle physics.Comment: 15 pages, 13 figure

    Standard Neutrino Spectrum from B-8 Decay

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    We present a systematic evaluation of the shape of the neutrino energy spectrum produced by beta-decay of 8^8B. We place special emphasis on determining the range of uncertainties permitted by existing laboratory data and theoretical ingredients (such as forbidden and radiative corrections). We review and compare the available experimental data on the 8^8B(β+)8(\beta^+){}^8Be(2α)(2\alpha) decay chain. We analyze the theoretical and experimental uncertainties quantitatively. We give a numerical representation of the best-fit (standard-model) neutrino spectrum, as well as two extreme deviations from the standard spectrum that represent the total (experimental and theoretical) effective ±3σ\pm3\sigma deviations. Solar neutrino experiments that are currently being developed will be able to measure the shape of the 8^8B neutrino spectrum above about 5 MeV. An observed distortion of the 8^8B solar neutrino spectrum outside the range given in the present work could be considered as evidence, at an effective significance level greater than three standard deviations, for physics beyond the standard electroweak model. We use the most recent available experimental data on the Gamow--Teller strengths in the A=37A=37 system to calculate the 8^8B neutrino absorption cross section on chlorine: σCl=(1.14±0.11)×10−42\sigma_{\rm Cl}=(1.14\pm0.11)\times10^{-42}~cm2^2 (±3σ\pm3\sigma errors). The chlorine cross section is also given as a function of the neutrino energy. The 8^8B neutrino absorption cross section in gallium is σGa=(2.46−1.1+2.1)×10−42\sigma_{\rm Ga}=(2.46^{+2.1}_{-1.1})\times10^{-42} cm2^2 (±3σ\pm3\sigma errors).Comment: Revised version, to appear in Phys. Rev.
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