437 research outputs found

    The N=28 shell closure; from N=Z to the neutron drip line

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    The evolution of the N=28 neutron shell closure is studied in the N=28 isotones from neutron drip line's 40^{40}Mg to N=Z doubly magic 56^{56}Ni. It is found that the N=28 closure vanishes at Z=12 in favor of a deformed ground state. For Z=14 and Z=16 closed shell and intruder configurations are almost degenerate, leading to highly mixed ground states and to very low lying excited 0+^+ states. For Z>>20 the intruder states are always above the closed shell ground states. We examine their structure and their possible existence as collective yrare bands of well defined particle-hole character

    μ s isomers of Nd 158,160

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    The neutron-rich nuclei Nd158,160 have been studied via delayed γ-ray spectroscopy of μs isomeric states at the RIBF facility, RIKEN. These nuclei were produced following the projectile fission of a 345 AMeVU238 beam and delayed γ rays were detected by the EURICA cluster Ge array. The isomeric states have measured half-lives of 339(20) ns and 1.63(21) μs for Nd158 and Nd160, respectively. From the observed γ decays and the systematics of levels in the neighboring Nd isotopes first level schemes were constructed for these nuclei. The isomeric states of Nd158,160 have been assigned spins of (6-) and (4-), with proposed ν5/2[523] - ν7/2[633] and ν1/2[521] - ν7/2[633] configurations, respectively. © 2016 American Physical Society

    Bethe Ansatz Equations for General Orbifolds of N=4 SYM

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    We consider the Bethe Ansatz Equations for orbifolds of N =4 SYM w.r.t. an arbitrary discrete group. Techniques used for the Abelian orbifolds can be extended to the generic non-Abelian case with minor modifications. We show how to make a transition between the different notations in the quiver gauge theory.Comment: LaTeX, 66 pages, 9 eps figures, minor corrections, references adde

    Perturbative Search for Fixed Lines in Large N Gauge Theories

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    The logarithmic running of marginal double-trace operators is a general feature of 4-d field theories containing scalar fields in the adjoint or bifundamental representation. Such operators provide leading contributions in the large N limit; therefore, the leading terms in their beta functions must vanish for a theory to be large N conformal. We calculate the one-loop beta functions in orbifolds of the N=4 SYM theory by a discrete subgroup Gamma of the SU(4) R-symmetry, which are dual to string theory on AdS_5 x S^5/Gamma. We present a general strategy for determining whether there is a fixed line passing through the origin of the coupling constant space. Then we study in detail some classes of non-supersymmetric orbifold theories, and emphasize the importance of decoupling the U(1) factors. Among our examples, which include orbifolds acting freely on the S^5, we do not find any large N non-supersymmetric theories with fixed lines passing through the origin. Connection of these results with closed string tachyon condensation in AdS_5 x S^5/Gamma is discussed.Comment: 31 pages, 4 figures, latex v2: Clarifications and reference adde

    Superdeformation in Asymmetric N>>Z Nucleus 40^{40}Ar

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    A rotational band with five γ\gamma-ray transitions ranging from 2+^{+} to 12+^{+} states was identified in 40^{40}Ar. This band is linked through γ\gamma transitions from the excited 2+^{+}, 4+^{+} and 6+^{+} levels to the low-lying states; this determines the excitation energy and the spin-parity of the band. The deduced transition quadrupole moment of 1.450.31+0.49eb^{+0.49}_{-0.31} eb indicates that the band has a superdeformed shape. The nature of the band is revealed by cranked Hartree--Fock--Bogoliubov calculations and a multiparticle--multihole configuration is assigned to the band

    The Bethe Ansatz for Z_S Orbifolds of N=4 Super Yang-Mills Theory

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    Worldsheet techniques can be used to argue for the integrability of string theory on AdS_5xS^5/Z_S, which is dual to the strongly coupled Z_S-orbifold of N=4 SYM. We analyze the integrability of these field theories in the perturbative regime and construct the relevant Bethe equations.Comment: 16 page

    Decay Properties of 266^{266}Bh and 262^{262}Db Produced in the 248^{248}Cm + 23^{23}Na Reaction

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    Decay properties of an isotope 266^{266}Bh and its daughter nucleus 262^{262}Db produced by the 248^{248}Cm(23^{23}Na, 5\textit{n}) reaction were studied by using a gas-filled recoil separator coupled with a position-sensitive semiconductor detector. 266^{266}Bh was clearly identified from the correlation of the known nuclide, 262^{262}Db. The obtained decay properties of 266^{266}Bh and 262^{262}Db are consistent with those observed in the 278^{278}113 chain, which provided further confirmation of the discovery of 278^{278}113.Comment: Accepted for publication in J. Phys. Soc. JPN., to be published in Vol.78 No.
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