94 research outputs found

    Geant4 Simulation of a filtered X-ray Source for Radiation Damage Studies

    Full text link
    Geant4 low energy extensions have been used to simulate the X-ray spectra of industrial X-ray tubes with filters for removing the uncertain low energy part of the spectrum in a controlled way. The results are compared with precisely measured X-ray spectra using a silicon drift detector. Furthermore, this paper shows how the different dose rates in silicon and silicon dioxide layers of an electronic device can be deduced from the simulations

    The marine kd and water/sediment interaction problem

    Get PDF
    The behavior of marine distribution coefficients is analyzed with the help of numerical experiments and ana-lytical solutions of equations describing kinetic models for uptake/release of radionuclides. The difficulties in measuring true kd in a marine environment perturbed by an external radionuclide source are highlighted. Differences between suspended matter and bed sediment kd are analyzed. The performances of different kinetic models (1-step/2step; single-layer/multi-layer) are studied in model/model and model/experiment compar-isons. Implications for the use of models to assess radioactive contamination after an emergency are given; as well as recommendations when kd data are compiled in order to create a useful databaseInternational Atomic Energy Agency (IAEA) KIOST PE9961

    First Observation of Radiative B^0 -> \phi K^0 \gamma Decays and Measurements of Their Time-Dependent CP Violation

    Full text link
    We report the first observation of the radiative decay B^0 -> \phi K^0 \gamma using a data sample of 772 x 10^6 B B-bar pairs collected at the \Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e^+e^- collider. We observe a signal of 37+/-8 events with a significance of 5.4 standard deviations including systematic uncertainties. The measured branching fraction is B(B0>ϕK0γ)=(2.74±0.60±0.32)×106{\cal B}(B^0 -> \phi K^0 \gamma) = (2.74\pm 0.60 \pm 0.32) \times 10^{-6}, where the uncertainties are statistical and systematic, respectively. We also report the first measurements of time-dependent CP violation parameters: SϕKS0γ=+0.741.05+0.72(stat)0.24+0.10(syst){\mathcal S}_{\phi K_S^0 \gamma} = +0.74^{+0.72}_{-1.05} (stat)^{+0.10}_{-0.24} (syst) and AϕKS0γ=+0.35+/0.58(stat)0.10+0.23(syst){\mathcal A}_{\phi K_S^0 \gamma} = +0.35 +/- 0.58 (stat)^{+0.23}_{-0.10} (syst). Furthermore, we measure B(B+>ϕK+γ)=(2.48+/0.30+/0.24)x106{\mathcal B}(B^+ -> \phi K^+ \gamma) = (2.48 +/- 0.30 +/- 0.24) x 10^{-6}, ACP=0.03+/0.11+/0.08{\mathcal A}_{CP} = -0.03 +/- 0.11 +/- 0.08 and find that the signal is concentrated in the M_{\phi K} mass region near threshold.Comment: 6 pages, 3 figures, Modified version is to be published in PRD(RC

    Bounds on the width, mass difference and other properties of X(3872) --> pi+pi-J/psi decays

    Full text link
    We present results from a study of X(3872) --> pi+pi- J/psi decays produced via exclusive B--> K X(3872) decays. We determine the mass to be M_X(3872)= (3871.84\pm 0.27 (stat)\pm 0.19 (syst)) MeV, a 90% CL upper limit on the natural width of Gamma_X(3872) K+X(3872))xBf(X(3872)-->pi+pi-J/psi)=(8.61 \pm 0.82(stat) \pm 0.52 (syst)) x10^{-6}, and a ratio of branching fractions Bf(B0--> K0 X(3872))/BF(B+--> K+ X(3872))=0.50\pm 0.14(stat)\pm0.04(syst). The difference in mass between the X(3872)-->pi+pi-J/psi signals in B+ and B0 decays is Delta M_{X(3872)= (-0.69 \pm 0.97 (stat)} \pm 0.19 (syst)) MeV. A search for a charged partner of the X(3872) in the decays Bbar0-->K- X+ or B+-->K0X+, X+-->pi+pi0 J/psi resulted in upper limits on the product branching fractions for these processes that are well below expectations for the case that the X(3872) is the neutral member of an isospin triplet. In addition, we examine possible J^{PC} quantum number assignments for the X(3872) based on comparisons of angular correlations between final state particles in X(3872)-->pi+pi-J/psi decays with simulated data for J^{PC} values of 1^{++} and 2^{-+}. We examine the influence of rho-omega interference in the M(pi+pi-) spectrum. The analysis is based on a 711fb^{-1} data sample that contains 772 million BBbar meson pairs collected at the Upsilon(4S) resonance in the Belle detector at the KEKB e+e- collider.Comment: 15 pages, 10 figures and 6 tables. Submitted to Physical Review

    Measurements of Branching Fractions and Time-dependent CP Violating Asymmetries in B0D()±DB^{0} \to D^{(*)\pm}D^{\mp} Decays

    Full text link
    We report measurements of branching fractions and time-dependent CP asymmetries in B0D+DB^{0} \to D^{+}D^{-} and B0D±DB^{0} \to D^{*\pm}D^{\mp} decays using a data sample that contains (772±11)×106BBˉ(772 \pm 11)\times 10^6 B\bar{B} pairs collected at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^+ e^- collider. We determine the branching fractions to be B(B0D+D)=(2.12±0.16±0.18)×104\mathcal{B}(B^{0} \to D^{+}D^{-})=(2.12 \pm 0.16 \pm 0.18)\times 10^{-4} and B(B0D±D=(6.14±0.29±0.50)×104\mathcal{B}(B^{0} \to D^{*\pm}D^{\mp}=(6.14 \pm 0.29 \pm 0.50)\times 10^{-4}. We measure CP asymmetry parameters SD+D=1.060.14+0.21±0.08\mathcal{S}_{D^{+}D^{-}} = -1.06_{-0.14}^{+0.21} \pm 0.08 and CD+D=0.43±0.16±0.05\mathcal{C}_{D^{+}D^{-}} = -0.43 \pm 0.16 \pm 0.05 in B0D+DB^{0} \to D^{+}D^{-} and ADD=+0.06±0.05±0.02\mathcal{A}_{D^{*}D} = +0.06 \pm 0.05 \pm 0.02, SDD=0.78±0.15±0.05\mathcal{S}_{D^{*}D} = -0.78 \pm 0.15 \pm 0.05, CDD=0.01±0.11±0.04\mathcal{C}_{D^{*}D} = -0.01 \pm 0.11 \pm 0.04, ΔSDD=0.13±0.15±0.04\Delta\mathcal{S}_{D^{*}D} = -0.13 \pm 0.15 \pm 0.04 and ΔCDD=+0.12±0.11±0.03\Delta\mathcal{C}_{D^{*}D} = +0.12 \pm 0.11 \pm 0.03 in B0D±DB^{0} \to D^{*\pm}D^{\mp}, where the first uncertainty is statistical and the second is systematic. We exclude the conservation of CP symmetry in both decays at equal to or greater than 4σ4\sigma significance.Comment: 7 pages, 2 figure

    Ab initio van der Waals interactions in simulations of water alter structure from mainly tetrahedral to high-density-like

    Get PDF
    The structure of liquid water at ambient conditions is studied in ab initio molecular dynamics simulations using van der Waals (vdW) density-functional theory, i.e. using the new exchange-correlation functionals optPBE-vdW and vdW-DF2. Inclusion of the more isotropic vdW interactions counteracts highly directional hydrogen-bonds, which are enhanced by standard functionals. This brings about a softening of the microscopic structure of water, as seen from the broadening of angular distribution functions and, in particular, from the much lower and broader first peak in the oxygen-oxygen pair-correlation function (PCF), indicating loss of structure in the outer solvation shells. In combination with softer non-local correlation terms, as in the new parameterization of vdW-DF, inclusion of vdW interactions is shown to shift the balance of resulting structures from open tetrahedral to more close-packed. The resulting O-O PCF shows some resemblance with experiment for high-density water (A. K. Soper and M. A. Ricci, Phys. Rev. Lett., 84:2881, 2000), but not directly with experiment for ambient water. However, an O-O PCF consisting of a linear combination of 70% from vdW-DF2 and 30% from experiment on low-density liquid water reproduces near-quantitatively the experimental O-O PCF for ambient water, indicating consistency with a two-liquid model with fluctuations between high- and low-density regions

    Observation of Bs0J/ψf0(980)B_s^0\to J/\psi f_0(980) and Evidence for Bs0J/ψf0(1370)B_s^0\to J/\psi f_0(1370)

    Full text link
    We report the first observation of Bs0J/ψf0(980)B_s^0\to J/\psi f_0(980) and first evidence for Bs0J/ψf0(1370)B_s^0\to J/\psi f_0(1370), which are CP eigenstate decay modes. These results are obtained from 121.4  fb1121.4\;\mathrm{fb}^{-1} of data collected at the Υ(5S)\Upsilon(5S) resonance with the Belle detector at the KEKB e+ee^+e^- collider. We measure the branching fractions B(Bs0J/ψf0(980);f0(980)π+π)=(1.160.19+0.31(stat.)0.17+0.15(syst.)0.18+0.26(NBs()Bˉs()))×104\mathcal{B}(B_s^0\to J/\psi f_0(980);f_0(980)\to\pi^+\pi^-)=(1.16^{+0.31}_{-0.19}(\mathrm{stat.})^{+0.15}_{-0.17}(\mathrm{syst.})^{+0.26}_{-0.18}(N_{B_s^{(*)}\bar B_s^{(*)}})) \times 10^{-4} with a significance of 8.4σ8.4\sigma, and B(Bs0J/ψf0(1370);f0(1370)π+π)=(0.340.14+0.11(stat.)0.02+0.03(syst.)0.05+0.08(NBs()Bˉs()))×104\mathcal{B}(B_s^0\to J/\psi f_0(1370);f_0(1370)\to\pi^+\pi^-)=(0.34^{+0.11}_{-0.14}(\mathrm{stat.})^{+0.03}_{-0.02}(\mathrm{syst.})^{+0.08}_{-0.05}(N_{B_s^{(*)}\bar B_s^{(*)}})) \times 10^{-4} with a significance of 4.2σ4.2\sigma. The last error listed is due to uncertainty in the number of produced Bs()Bˉs()B_s^{(*)}\bar B_s^{(*)} pairs.Comment: 5 pages, 2 figures, 2 tables, published in PR

    First observation of CP violation and improved measurement of the branching fraction and polarization of B0 -> D*+ D*- decays

    Full text link
    We report the measurement of the branching fraction, the polarization, and the parameters of the time-dependent CP violation in B0 -> D*+ D*- decays using a data sample of 772 million BB pairs, collected at the Y(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e- collider. We obtain a branching fraction of B = (7.82 +- 0.38 +- 0.63) x10^{-4}, a CP-odd fraction of R_\perp = 0.138 +- 0.024 +- 0.006 and, additionally, a fraction of the longitudinal component in the transversity base of R_0 = 0.624 +- 0.029 +- 0.011. The measured values of the parameters of the CP violation are S_{D*+ D*-} = -0.79 +- 0.13 +- 0.03 and A_{D*+ D*-} = 0.15 +- 0.08 +- 0.04

    Search for Time-Dependent CPT Violation in Hadronic and Semileptonic B Decays

    Full text link
    We report a new sensitive search for CPT violation, which includes improved measurements of the CPT-violating parameter z and the total decay-width difference normalized to the averaged width DeltaGamma_d/Gamma_d of the two Bd mass eigenstates. The results are based on a data sample of 535 x 10^6 BBbar pairs collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e^+e^- collider. We obtain Re(z) = [+1.9 +/- 3.7 (stat) +/- 3.3 (syst)] x 10^{-2}, Im(z) = [-5.7 +/- 3.3 (stat) +/- 3.3 (syst)] x 10^{-3}, and DeltaGamma_d/Gamma_d = [-1.7 +/- 1.8 (stat) +/- 1.1 (syst)] x 10^{-2}, all of which are consistent with zero. This is the most precise single measurement of these parameters in the neutral B-meson system to date.Comment: 7 pages, 3 figures, 2 tables, LaTeX; addition of supplemental information, corrections of typos, results unchange
    corecore