1,299 research outputs found

    Crisis, learning and policy change in the European Union

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    This is the author accepted manuscript. The final version is available from the publisher via the DOI in this record.What is the causal relationship between crisis, learning and change? How does causality works in the current responses to the sovereign debt crisis provided by the European Union? We question the conventional identification of the cause-and-effect relationship provided by theories of crisis management, integration and policy learning. Drawing on models of contingent learning developed within psychology and behavioural and evolutionary economics, we theorise that surprise produces behavioural change via a fast-paced associative cue-outcome mechanism and that policy learning follows change. We then run our exercise in causal identification through a plausibility probe. We show that our argument passes the plausibility probe. Our conclusions on cognition and situational effects on learning suggest a new research agenda, more sensitive to how individuals behave in the real world and more robust in its micro-foundations

    Non-collinear long-range magnetic ordering in HgCr2S4

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    The low-temperature magnetic structure of \HG has been studied by high-resolution powder neutron diffraction. Long-range incommensurate magnetic order sets in at TN∼_N\sim22K with propagation vector \textbf{k}=(0,0,∼\sim0.18). On cooling below TN_N, the propagation vector increases and saturates at the commensurate value \textbf{k}=(0,0,0.25). The magnetic structure below TN_N consists of ferromagnetic layers in the \textit{ab}-plane stacked in a spiral arrangement along the \textit{c}-axis. Symmetry analysis using corepresentations theory reveals a point group symmetry in the ordered magnetic phase of 422 (D4_4), which is incompatible with macroscopic ferroelectricity. This finding indicates that the spontaneous electric polarization observed experimentally cannot be coupled to the magnetic order parameter

    Measuring design diversity: A new application of Ostrom's rule types

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    We draw on the Institutional Grammar Tool's rule types to empiricallyanalyze the design of four major procedural regulatoryinstruments in the 27 member states of the European Union andthe UK. They are: consultation, regulatory impact assessment,freedom of information, and the Ombudsman. By adopting theInstitutional Grammar Tool as conceptual lens we end up witha single measurement template applicable to a variety of actionsituations. We derive measures that are conceptually robust andsuitable for comparative analysis. With original data gathered onthe official legal base in the 28 cases, we carry out principal componentsanalysis. We identify design patterns across countriesand instruments; the specialization of each instrument in termsof rule type; and the components that best explain cross-countryvariation. In the conclusions we argue that to reframe the designfeatures of the four instruments in conceptual, theoreticalcategories is not simply a taxonomical exercise but it extends tothe territory of comparative policy analysis, practice and reform

    Electric field control of magnetic properties and electron transport in BaTiO3-based multiferroic heterostructures

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    In this paper, we report on a purely electric mechanism for achieving the electric control of the interfacial spin polarization and magnetoresistance in multiferroic tunneling junctions. We investigate micrometric devices based on the Co/Fe/BaTiO3/La0.7Sr0.3MnO3 heterostructure, where Co/Fe and La0.7Sr0.3MnO3 are the magnetic electrodes and BaTiO3 acts both as a ferroelectric element and tunneling barrier. We show that, at 20 K, devices with a 2 nm thick BaTiO3 barrier present both tunneling electroresistance (TER = 12   ±   0.1%) and tunneling magnetoresistance (TMR). The latter depends on the direction of the BaTiO3 polarization, displaying a sizable change of the TMR from  -0.32   ±   0.05% for the polarization pointing towards Fe, to  -0.12   ±   0.05% for the opposite direction. This is consistent with the on-off switching of the Fe magnetization at the Fe/BaTiO3 interface, driven by the BaTiO3 polarization, we have previously demonstrated in x-ray magnetic circular dichroism experiments

    High Performances Corrugated Feed Horns for Space Applications at Millimetre Wavelengths

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    We report on the design, fabrication and testing of a set of high performance corrugated feed horns at 30 GHz, 70 GHz and 100 GHz, built as advanced prototypes for the Low Frequency Instrument (LFI) of the ESA Planck mission. The electromagnetic designs include linear (100 GHz) and dual shaped (30 and 70 GHz) profiles. Fabrication has been achieved by direct machining at 30 GHz, and by electro-formation at higher frequencies. The measured performances on side lobes and return loss meet the stringent Planck requirements over the large (20%) instrument bandwidth. Moreover, the advantage in terms of main lobe shape and side lobes levels of the dual profiled designs has been demonstrated.Comment: 16 pages, 7 figures, accepted for publication in Experimental Astronom

    Glauber slow dynamics of the magnetization in a molecular Ising chain

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    The slow dynamics (10^-6 s - 10^4 s) of the magnetization in the paramagnetic phase, predicted by Glauber for 1d Ising ferromagnets, has been observed with ac susceptibility and SQUID magnetometry measurements in a molecular chain comprising alternating Co{2+} spins and organic radical spins strongly antiferromagnetically coupled. An Arrhenius behavior with activation energy Delta=152 K has been observed for ten decades of relaxation time and found to be consistent with the Glauber model. We have extended this model to take into account the ferrimagnetic nature of the chain as well as its helicoidal structure.Comment: 4 pages, 4 figures (low resolution), 16 references. Submitted to Physical Review Letter

    Temperature and field dependence of the phase separation, structure, and magnetic ordering in La1−x_{1-x}Cax_xMnO3_3, (x=0.47x=0.47, 0.50, and 0.53)

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    Neutron powder diffraction measurements, combined with magnetization and resistivity data, have been carried out in the doped perovskite La1−x_{1-x}Cax_xMnO3_3 (x=0.47x=0.47, 0.50, and 0.53) to elucidate the structural, magnetic, and electronic properties of the system around the composition corresponding to an equal number of Mn3+ and Mn4+. At room temperature all three samples are paramagnetic and single phase, with crystallographic symmetry Pnma. The samples then all become ferromagnetic (FM) at TC≈265T_C\approx 265 K. At ∼230\sim 230 K, however, a second distinct crystallographic phase (denoted A-II) begins to form. Initially the intrinsic widths of the peaks are quite large, but they narrow as the temperature decreases and the phase fraction increases, indicating microscopic coexistence. The fraction of the sample that exhibits the A-II phase increases with decreasing temperature and also increases with increasing Ca doping, but the transition never goes to completion to the lowest temperatures measured (5 K) and the two phases therefore coexist in this temperature-composition regime. Phase A-II orders antiferromagnetically (AFM) below a N\'{e}el temperature TN≈160T_N \approx 160 K, with the CE-type magnetic structure. Resistivity measurements show that this phase is a conductor, while the CE phase is insulating. Application of magnetic fields up to 9 T progressively inhibits the formation of the A-II phase, but this suppression is path dependent, being much stronger for example if the sample is field-cooled compared to zero-field cooling and then applying the field. The H-T phase diagram obtained from the diffraction measurements is in good agreement with the results of magnetization and resistivity.Comment: 12 pages, 3 tables, 11 figure

    Cooling rate dependence of the antiferromagnetic domain structure of a single crystalline charge ordered manganite

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    The low temperature phase of single crystals of Nd0.5_{0.5}Ca0.5_{0.5}MnO3_3 and Gd0.5_{0.5}Ca0.5_{0.5}MnO3_3 manganites is investigated by squid magnetometry. Nd0.5_{0.5}Ca0.5_{0.5}MnO3_3 undergoes a charge-ordering transition at TCOT_{CO}=245K, and a long range CE-type antiferromagnetic state is established at TNT_N=145K. The dc-magnetization shows a cooling rate dependence below TNT_N, associated with a weak spontaneous moment. The associated excess magnetization is related to uncompensated spins in the CE-type antiferromagnetic structure, and to the presence in this state of fully orbital ordered regions separated by orbital domain walls. The observed cooling rate dependence is interpreted to be a consequence of the rearrangement of the orbital domain state induced by the large structural changes occurring upon cooling.Comment: REVTeX4; 7 pages, 4 figures. Revised 2001/12/0

    Physiological and sensorial aspects of peach fruits cv. Chimarrita depending on the season and management of green pruning.

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    Made available in DSpace on 2018-01-11T23:32:07Z (GMT). No. of bitstreams: 1 LuisEduardoPODAVERDECHIMARRITA.pdf: 371835 bytes, checksum: e3f18ade57a63bec5503b96c84f41f1f (MD5) Previous issue date: 2018-01-10bitstream/item/170739/1/Luis-Eduardo-PODA-VERDE-CHIMARRITA.pd

    Crystal and magnetic structure of the La1−x_{1-x}Cax_{x}MnO3_{3} compound (x=0.8,0.85)(x=0.8,0.85)

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    We studied the crystal and magnetic structure of the La1−x_{1-x}Cax_{x}MnO3_{3} compound for x=0.8x=0.8 and x=0.85x=0.85. At T=300 K both samples are paramagnetic with crystallographic symmetry PnmaPnma. At low temperatures they undergo a monoclinic distortion from orthorhombic PnmaPnma-type structure with ap2×2ap×ap2a_p\sqrt{2}\times 2a_p\times a_p\sqrt{2} to a monoclinic structure with (ap2×2ap×ap2a_p\sqrt{2}\times 2a_p\times a_p\sqrt{2}, β=90+ϵ∼91.4o\beta=90+\epsilon\sim 91.4^{\rm o}) and P21/mP2_1/m space group below TNT_N. The onset of the structural transformation coincides with the development of the CC-type long range antiferromagnetic order with propagation vector k=(1/2,0,1/2){\bf k}=({1/2},0,{1/2}). The monoclinic unit cell allowed us to determine the direction of the Mn magnetic moment with respect to the crystallographic axes: it is perpendicular to the propagation vector, m⊥k=(1/2,0,1/2){\bf m}\perp {\bf k}=({1/2},0,{1/2}). The amplitude of the ordered magnetic moment at T=1.6T=1.6 K is found to be 2.53(2)2.53(2) and 2.47(2)μB2.47(2)\mu_{B} for x=0.8x=0.8 and 0.85, respectively.Comment: In press (Phys. Rev B 01 Feb 2002
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