432 research outputs found

    Hydrogen targets for exotic-nuclei studies developed over the past 10 years

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    Hydrogen-induced reactions provide essential information on nuclear structure, complementary to other experimental probes. For studies at both low and relativistic incident energy, developments in hydrogen targets have been performed over the past 10 years in parallel with the development of new radioactive beams. We present a review of all major hydrogen target developments related to the study of exotic nuclei with direct reactions in inverse kinematics. Both polarized and non-polarized systems are presented.Comment: 24 pages, 27 figures, review articl

    Shell Gap Reduction In Exotic N = 17 Nuclei

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    In-beam gamma-ray spectroscopy of 35Mg and 33Na

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    Excited states in the very neutron-rich nuclei 35Mg and 33Na were populated in the fragmentation of a 38Si projectile beam on a Be target at 83 MeV/u beam energy. We report on the first observation of gamma-ray transitions in 35Mg, the odd-N neighbor of 34Mg and 36Mg, which are known to be part of the "Island of Inversion" around N = 20. The results are discussed in the framework of large- scale shell-model calculations. For the A = 3Z nucleus 33Na, a new gamma-ray transition was observed that is suggested to complete the gamma-ray cascade 7/2+ --> 5/2+ --> 3/2+ gs connecting three neutron 2p-2h intruder states that are predicted to form a close-to-ideal K = 3/2 rotational band in the strong-coupling limit.Comment: Accepted for publication Phys. Rev. C. March 16, 2011: Replaced figures 3 and 5. We thank Alfredo Poves for pointing out a problem with the two figure

    γ spectroscopy of 25 , 27 Ne and 26 , 27 Na

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    The γ spectroscopy of 25, 27 Ne and 26, 27 Na was studied from the reaction of 26 Ne with a deuterium target in inverse kinematics at 9.7 MeV/nucleon. The selectivity of the (d,p), (d,t), and (d,n) transfer reactions provides new spectroscopic information on low-lying states. The validity of the sd shell-model space for these nuclei isdiscussed

    Anomalous Fermi Liquid Behavior of Overdoped High-Tc Superconductors

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    According to a generic temperature vs. carrier-doping (T-p) phase diagram of high-temperature superconductors it has been proposed that as doping increases to the overdoped region they approach gradually a conventional (canonical) Fermi Liquid. However, Hall effect measurements in several systems reported by different authors show a still strong \emph{T}-dependence in overdoped samples. We report here electrical transport measurements of Y_{1-x}Ca_{x}Ba_{2}Cu_{3}O_{7-delta} thin films presenting a temperature dependence of the Hall constant, R_H, which does not present a gradual transition towards the T-independent behavior of a canonical Fermi Liquid. Instead, the T-dependence passes by a minimum near optimal doping and then increases again in the overdoped region. We discuss the theoretical predictions from two representative Fermi Liquid models and show that they can not give a satisfactory explanation to our data. We conclude that this region of the phase diagram in YBCO, as in most HTSC, is not a canonical Fermi Liquid, therefore we call it Anomalous Fermi Liquid.Comment: 9 pages, 12 figures, to be published in Phys. Rev.

    A multi-reflection time-of-flight mass spectrometer for the offline ion source of the PUMA experiment

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    The antiProton Unstable Matter Annihilation experiment (PUMA) at CERN aims at investigating the nucleon composition in the matter density tail of radioactive as well as stable isotopes by use of low-energy antiproton-nucleon annihilation processes. For this purpose, antiprotons provided by the Extra Low ENergy Antiproton (ELENA) facility will be trapped together with the ions of interest. While exotic ions will be obtained by the Isotope mass Separator On-Line DEvice (ISOLDE), stable ions will be delivered from an offline ion source setup designed for this purpose. This allows the proposed technique to be applied to a variety of stable nuclei and for reference measurements. For beam purification, the ion source setup includes a multi-reflection time-of-flight mass spectrometer (MR-ToF MS). Supported by SIMION simulations, an earlier MR-ToF MS design has been modified to meet the requirements of PUMA. During commissioning of the new MR-ToF device with Ar+^+ ions, mass resolving powers in excess of 50,000 have been obtained after 150 revolutions, limited by the chopping of the continuous beam from an electron impact ionisation source

    Effects of next-nearest-neighbor hopping tt^{\prime} on the electronic structure of cuprates

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    Photoemission spectra of underdoped and lightly-doped Bi2z_{2-z}Pbz_zSr2_2Ca1x_{1-x}{\it R}x_{x}Cu2_2O8+y_{8+y} (R=R= Pr, Er) (BSCCO) have been measured and compared with those of La2x_{2-x}Srx_xCuO4_4 (LSCO). The lower-Hubbard band of the insulating BSCCO, like Ca2_2CuO2_2Cl2_2, shows a stronger dispersion than La2_2CuO4_4 from k{\bf k}\sim(π/2,π/2\pi/2,\pi/2) to \sim(π,0\pi,0). The flat band at k{\bf k}\sim(π,0\pi,0) is found generally deeper in BSCCO. These observations together with the Fermi-surface shapes and the chemical potential shifts indicate that the next-nearest-neighbor hopping t|t^{\prime}| of the single-band model is larger in BSCCO than in LSCO and that t|t^{\prime}| rather than the super-exchange JJ influences the pseudogap energy scale.Comment: 5 pages,4 figures, 1 tabl

    Lifetime measurements in 63^{63}Co and 65^{65}Co

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    Lifetimes of the 9/219/2^-_1 and 3/213/2^-_1 states in 63^{63}Co and the 9/219/2^-_1 state in 65^{65}Co were measured using the recoil distance Doppler shift and the differential decay curve methods. The nuclei were populated by multi-nucleon transfer reactions in inverse kinematics. Gamma rays were measured with the EXOGAM Ge array and the recoiling fragments were fully identified using the large-acceptance VAMOS spectrometer. The E2 transition probabilities from the 3/213/2^-_1 and 9/219/2^-_1 states to the 7/27/2^- ground state could be extracted in 63^{63}Co as well as an upper limit for the 9/217/219/2^-_1\rightarrow7/2^-_1 BB(E2) value in 65^{65}Co. The experimental results were compared to large-scale shell-model calculations in the pfpf and pfg9/2pfg_{9/2} model spaces, allowing to draw conclusions on the single-particle or collective nature of the various states.Comment: 8 pages, 8 figures, 1 table, accepted for publication in Physical Review
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