298 research outputs found

    Properties of 8^{8}Be and 12^{12}C deduced from the folding--potential model

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    The α\alpha--α\alpha differential cross sections are analyzed in the optical model using a double--folded potential. With the knowledge of this potential bound and resonance--state properties of α\alpha--cluster states in 8^{8}Be and 12^{12}C as well as astrophysical S--factors of 4^{4}He(α\alpha,Îł\gamma)8^{8}Be and 8^{8}Be(α\alpha,Îł\gamma)12^{12}C are calculated. Γγ\Gamma_{\gamma}--widths and B(E2)--values are deduced.Comment: 2 pages LaTeX, 2 figures can be obtained from the author

    Effect of ion binding on the molecular properties of low molecular weight polysaccharides

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    "The Institute of Paper Chemistry ... Donald D. Bump ... Sheldon F. Kurath ... John W. Swanson.""January 28, 1963.

    Quantum Monte Carlo calculations of A=9,10A=9,10 nuclei

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    We report on quantum Monte Carlo calculations of the ground and low-lying excited states of A=9,10A=9,10 nuclei using realistic Hamiltonians containing the Argonne v18v_{18} two-nucleon potential alone or with one of several three-nucleon potentials, including Urbana IX and three of the new Illinois models. The calculations begin with correlated many-body wave functions that have an α\alpha-like core and multiple p-shell nucleons, LSLS-coupled to the appropriate (Jπ;T)(J^{\pi};T) quantum numbers for the state of interest. After optimization, these variational trial functions are used as input to a Green's function Monte Carlo calculation of the energy, using a constrained path algorithm. We find that the Hamiltonians that include Illinois three-nucleon potentials reproduce ten states in 9^9Li, 9^9Be, 10^{10}Be, and 10^{10}B with an rms deviation as little as 900 keV. In particular, we obtain the correct 3+^+ ground state for 10^{10}B, whereas the Argonne v18v_{18} alone or with Urbana IX predicts a 1+^+ ground state. In addition, we calculate isovector and isotensor energy differences, electromagnetic moments, and one- and two-body density distributions.Comment: 28 pages, 12 tables, 7 figure

    Astrophysical Reaction Rates for 10^{10}B(p,α\alpha)7^{7}Be and 11^{11}B(p,α\alpha)8^{8}Be From a Direct Model

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    The reactions 10^{10}B(p,α\alpha)7^{7}Be and 11^{11}B(p,α\alpha)8^{8}Be are studied at thermonuclear energies using DWBA calculations. For both reactions, transitions to the ground states and first excited states are investigated. In the case of 10^{10}B(p,α\alpha)7^{7}Be, a resonance at ERes=10E_{Res}=10 keV can be consistently described in the potential model, thereby allowing the extension of the astrophysical SS-factor data to very low energies. Strong interference with a resonance at about ERes=550E_{Res}=550 keV require a Breit-Wigner description of that resonance and the introduction of an interference term for the reaction 10^{10}B(p,α1\alpha_1)7^{7}Be∗^*. Two isospin T=1T=1 resonances (at ERes1=149E_{Res1}=149 keV and ERes2=619E_{Res2}=619 keV) observed in the 11^{11}B+p reactions necessitate Breit-Wigner resonance and interference terms to fit the data of the 11^{11}B(p,α\alpha)8^{8}Be reaction. SS-factors and thermonuclear reaction rates are given for each reaction. The present calculation is the first consistent parametrization for the transition to the ground states and first excited states at low energies.Comment: 27 pages, 5 Postscript figures, uses RevTex and aps.sty; preprint also available at http://quasar.physik.unibas.ch/ Phys. Rev. C, in pres

    Alpha scattering and capture reactions in the A = 7 system at low energies

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    Differential cross sections for 3^3He-α\alpha scattering were measured in the energy range up to 3 MeV. These data together with other available experimental results for 3^3He +α+ \alpha and 3^3H +α+ \alpha scattering were analyzed in the framework of the optical model using double-folded potentials. The optical potentials obtained were used to calculate the astrophysical S-factors of the capture reactions 3^3He(α,Îł)7(\alpha,\gamma)^7Be and 3^3H(α,Îł)7(\alpha,\gamma)^7Li, and the branching ratios for the transitions into the two final 7^7Be and 7^7Li bound states, respectively. For 3^3He(α,Îł)7(\alpha,\gamma)^7Be excellent agreement between calculated and experimental data is obtained. For 3^3H(α,Îł)7(\alpha,\gamma)^7Li a S(0)S(0) value has been found which is a factor of about 1.5 larger than the adopted value. For both capture reactions a similar branching ratio of R=σ(Îł1)/σ(Îł0)≈0.43R = \sigma(\gamma_1)/\sigma(\gamma_0) \approx 0.43 has been obtained.Comment: submitted to Phys.Rev.C, 34 pages, figures available from one of the authors, LaTeX with RevTeX, IK-TUW-Preprint 930540

    Beyond Implications and Applications: the Story of ‘Safety by Design’

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    Using long-term anthropological observations at the Center for Biological and Environmental Nanotechnology in Houston, Texas, the article demonstrates in detail the creation of new objects, new venues and new modes of veridiction which have reoriented the disciplines of materials chemistry and nanotoxicology. Beginning with the confusion surrounding the meaning of ‘implications’ and ‘applications’ the article explores the creation of new venues (CBEN and its offshoot the International Council on Nanotechnology); it then demonstrates how the demands for a responsible, safe or ethical science were translated into new research and experiment in and through these venues. Finally it shows how ‘safety by design’ emerged as a way to go beyond implications and applications, even as it introduced a whole new array of controversies concerning its viability, validity and legitimacy

    A Nuclear Localization of the Infectious Haematopoietic Necrosis Virus NV Protein Is Necessary for Optimal Viral Growth

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    The nonvirion (NV) protein of infectious hematopoietic necrosis virus (IHNV) has been previously reported to be essential for efficient growth and pathogenicity of IHNV. However, little is known about the mechanism by which the NV supports the viral growth. In this study, cellular localization of NV and its role in IHNV growth in host cells was investigated. Through transient transfection in RTG-2 cells of NV fused to green fluorescent protein (GFP), a nuclear localization of NV was demonstrated. Deletion analyses showed that the 32EGDL35 residues were essential for nuclear localization of NV protein, and fusion of these 4 amino acids to GFP directed its transport to the nucleus. We generated a recombinant IHNV, rIHNV-NV-ΔEGDL in which the 32EGDL35 was deleted from the NV. rIHNVs with wild-type NV (rIHNV-NV) or with the NV gene replaced with GFP (rIHNV-ΔNV-GFP) were used as controls. RTG-2 cells infected with rIHNV-ΔNV-GFP and rIHNV-NV-ΔEGDL yielded 12- and 5-fold less infectious virion, respectively, than wild type rIHNV-infected cells at 48 h post-infection (p.i.). While treatment with poly I∶C at 24 h p.i. did not inhibit replication of wild-type rIHNVs, replication rates of rIHNV-ΔNV-GFP and rIHNV-NV-ΔEGDL were inhibited by poly I∶C. In addition, both rIHNV-ΔNV and rIHNV-NV-ΔEGDL induced higher levels of expressions of both IFN1 and Mx1 than wild-type rIHNV. These data suggest that the IHNV NV may support the growth of IHNV through inhibition of the INF system and the amino acid residues of 32EGDL35 responsible for nuclear localization are important for the inhibitory activity of NV

    On the edge: Chaucer and Gower’s queer glosses

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    In this article Diane Watt and I focus on a number of manuscript glosses accompanying the tale of Constance in Chaucer's The Man of Law's Tale and in Gower's Tale of Constance in Confessio Amantis. By applying queer theory to the paratextual apparatus of these manuscripts, we shed new light on the anxieties about authority and authorship shared by Chaucer and Gower (and their circles of collaborators). We also reevaluate the role of error and manuscripts variants, and argue for the queer pleasure provided by misprision and misinterpretation. This helps us to move away from patriarchal constructs on canon formation and manuscript transmission
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